1
|
Patel D, Knauer JP, Cao D, Betti R, Nora R, Shvydky A, Gopalaswamy V, Lees A, Sampat S, Donaldson WR, Regan SP, Stoeckl C, Forrest CJ, Glebov VY, Harding DR, Bonino MJ, Janezic RT, Wasilewski D, Fella C, Shuldberg C, Murray J, Guzman D, Serrato B. Effects of Laser Bandwidth in Direct-Drive High-Performance DT-Layered Implosions on the OMEGA Laser. Phys Rev Lett 2023; 131:105101. [PMID: 37739360 DOI: 10.1103/physrevlett.131.105101] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/10/2023] [Revised: 07/05/2023] [Accepted: 08/16/2023] [Indexed: 09/24/2023]
Abstract
In direct-drive inertial confinement fusion, the laser bandwidth reduces the laser imprinting seed of hydrodynamic instabilities. The impact of varying bandwidth on the performance of direct-drive DT-layered implosions was studied in targets with different hydrodynamic stability properties. The stability was controlled by changing the shell adiabat from (α_{F}≃5) (more stable) to (α_{F}≃3.5) (less stable). These experiments show that the performance of lower adiabat implosions improves considerably as the bandwidth is raised indicating that further bandwidth increases, beyond the current capabilities of OMEGA, would be greatly beneficial. These results suggest that the future generation of ultra-broadband lasers could enable achieving high convergence and possibly high gains in direct drive ICF.
Collapse
Affiliation(s)
- D Patel
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
- Department of Mechanical Engineering, University of Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - D Cao
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
- Department of Mechanical Engineering, University of Rochester, New York 14623, USA
- Department of Physics and Astronomy, University of Rochester, New York 14623, USA
| | - R Nora
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Shvydky
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - V Gopalaswamy
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - A Lees
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - S Sampat
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - W R Donaldson
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - D R Harding
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - M J Bonino
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - R T Janezic
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - D Wasilewski
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - C Fella
- Laboratory for Laser Energetics, University of Rochester, New York 14623, USA
| | - C Shuldberg
- General Atomics, San Diego, California 92186, USA
| | - J Murray
- General Atomics, San Diego, California 92186, USA
| | - D Guzman
- General Atomics, San Diego, California 92186, USA
| | - B Serrato
- General Atomics, San Diego, California 92186, USA
| |
Collapse
|
2
|
Mannion OM, Taitano WT, Appelbe BD, Crilly AJ, Forrest CJ, Glebov VY, Knauer JP, McKenty PW, Mohamed ZL, Stoeckl C, Keenan BD, Chittenden JP, Adrian P, Frenje J, Kabadi N, Gatu Johnson M, Regan SP. Evidence of non-Maxwellian ion velocity distributions in spherical shock-driven implosions. Phys Rev E 2023; 108:035201. [PMID: 37849093 DOI: 10.1103/physreve.108.035201] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/08/2023] [Accepted: 08/02/2023] [Indexed: 10/19/2023]
Abstract
The ion velocity distribution functions of thermonuclear plasmas generated by spherical laser direct drive implosions are studied using deuterium-tritium (DT) and deuterium-deuterium (DD) fusion neutron energy spectrum measurements. A hydrodynamic Maxwellian plasma model accurately describes measurements made from lower temperature (<10 keV), hydrodynamiclike plasmas, but is insufficient to describe measurements made from higher temperature more kineticlike plasmas. The high temperature measurements are more consistent with Vlasov-Fokker-Planck (VFP) simulation results which predict the presence of a bimodal plasma ion velocity distribution near peak neutron production. These measurements provide direct experimental evidence of non-Maxwellian ion velocity distributions in spherical shock driven implosions and provide useful data for benchmarking kinetic VFP simulations.
Collapse
Affiliation(s)
- O M Mannion
- Sandia National Laboratories, Albuquerque, New Mexico 87185, USA
| | - W T Taitano
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - B D Appelbe
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - A J Crilly
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - P W McKenty
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - Z L Mohamed
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - B D Keenan
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - J P Chittenden
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - P Adrian
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - N Kabadi
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
3
|
Moore AS, Schlossberg DJ, Appelbe BD, Chandler GA, Crilly AJ, Eckart MJ, Forrest CJ, Glebov VY, Grim GP, Hartouni EP, Hatarik R, Kerr SM, Kilkenny J, Knauer JP. Neutron time of flight (nToF) detectors for inertial fusion experiments. Rev Sci Instrum 2023; 94:061102. [PMID: 37862497 DOI: 10.1063/5.0133655] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/04/2022] [Accepted: 05/14/2023] [Indexed: 10/22/2023]
Abstract
Neutrons generated in Inertial Confinement Fusion (ICF) experiments provide valuable information to interpret the conditions reached in the plasma. The neutron time-of-flight (nToF) technique is well suited for measuring the neutron energy spectrum due to the short time (100 ps) over which neutrons are typically emitted in ICF experiments. By locating detectors 10s of meters from the source, the neutron energy spectrum can be measured to high precision. We present a contextual review of the current state of the art in nToF detectors at ICF facilities in the United States, outlining the physics that can be measured, the detector technologies currently deployed and analysis techniques used.
Collapse
Affiliation(s)
- A S Moore
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - D J Schlossberg
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - B D Appelbe
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW7 2AZ, United Kingdom
| | - G A Chandler
- Sandia National Laboratories, Albuquerque, New Mexico 87185, USA
| | - A J Crilly
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW7 2AZ, United Kingdom
| | - M J Eckart
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, 250 E River Rd., Rochester, New York 14623, USA
| | - V Y Glebov
- Laboratory for Laser Energetics, University of Rochester, 250 E River Rd., Rochester, New York 14623, USA
| | - G P Grim
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - E P Hartouni
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - R Hatarik
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - S M Kerr
- Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94551-0808, USA
| | - J Kilkenny
- General Atomics, San Diego, California 92121, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, 250 E River Rd., Rochester, New York 14623, USA
| |
Collapse
|
4
|
Forrest CJ, Crilly A, Schwemmlein A, Gatu-Johnson M, Mannion OM, Appelbe B, Betti R, Glebov VY, Gopalaswamy V, Knauer JP, Mohamed ZL, Radha PB, Regan SP, Stoeckl C, Theobald W. Measurements of low-mode asymmetries in the areal density of laser-direct-drive deuterium-tritium cryogenic implosions on OMEGA using neutron spectroscopy. Rev Sci Instrum 2022; 93:103505. [PMID: 36319371 DOI: 10.1063/5.0101812] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/03/2022] [Accepted: 08/17/2022] [Indexed: 06/16/2023]
Abstract
Areal density is one of the key parameters that determines the confinement time in inertial confinement fusion experiments, and low-mode asymmetries in the compressed fuel are detrimental to the implosion performance. The energy spectra from the scattering of the primary deuterium-tritium (DT) neutrons off the compressed cold fuel assembly are used to investigate low-mode nonuniformities in direct-drive cryogenic DT implosions at the Omega Laser Facility. For spherically symmetric implosions, the shape of the energy spectrum is primarily determined by the elastic and inelastic scattering cross sections for both neutron-deuterium and neutron-tritium kinematic interactions. Two highly collimated lines of sight, which are positioned at nearly orthogonal locations around the OMEGA target chamber, record the neutron time-of-flight signal in the current mode. An evolutionary algorithm is being used to extract a model-independent energy spectrum of the scattered neutrons from the experimental neutron time-of-flight data and is used to infer the modal spatial variations (l = 1) in the areal density. Experimental observations of the low-mode variations of the cold-fuel assembly (ρL0 + ρL1) show good agreement with a recently developed model, indicating a departure from the spherical symmetry of the compressed DT fuel assembly. Another key signature that has been observed in the presence of a low-mode variation is the broadening of the kinematic end-point due to the anisotropy of the dense fuel conditions.
Collapse
Affiliation(s)
- C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - A Crilly
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, South Kensington Campus, London, United Kingdom
| | - A Schwemmlein
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - M Gatu-Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - O M Mannion
- Sandia National Laboratories, Albuquerque, New Mexico 87185, USA
| | - B Appelbe
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, South Kensington Campus, London, United Kingdom
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - V Gopalaswamy
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - Z L Mohamed
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - P B Radha
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| |
Collapse
|
5
|
Glebov VY, Forrest CJ, Kendrick J, Knauer JP, Mannion OM, McClow H, Regan SP, Stoeckl C, Stanley B, Theobald W. A new neutron time-of-flight detector for yield and ion-temperature measurements at the OMEGA Laser Facility. Rev Sci Instrum 2022; 93:093522. [PMID: 36182446 DOI: 10.1063/5.0101514] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/01/2022] [Accepted: 08/25/2022] [Indexed: 06/16/2023]
Abstract
A new neutron time-of-flight (nTOF) detector for deuterium-deuterium (DD)-fusion yield and ion-temperature measurements was designed, installed, and calibrated for the OMEGA Laser Facility. This detector provides an additional line of sight for DD neutron yield and ion-temperature measurements for yields exceeding 1 × 1010 with higher precision than existing detectors. The nTOF detector consists of a 90-mm-diam, 20-mm-thick BC-422 scintillator and a gated Photek photomultiplier tube (PMT240). The PMT collects scintillating light through the 20-mm side of the scintillator without the use of a light guide. There is no lead shielding from hard x rays in order to allow the x-ray instrument response function of the detector to be measured easily. Instead, hard x-ray signals generated in implosion experiments are gated out by the PMT. The design provides a place for glass neutral-density filters between the scintillator and the PMT to avoid PMT saturation at high yields. The nTOF detector is installed in the OMEGA Target Bay along the P8A sub-port line of sight at a distance of 5.3 m from the target chamber center. In addition to DD measurements, the same detector can be used to measure the neutron yield and ion temperature from deuterium-tritium (DT) implosion targets in the 5 × 1010 to 2 × 1012 yield range. The design details and the calibration results of this nTOF detector for both D2 and DT implosions on OMEGA will be presented.
Collapse
Affiliation(s)
- V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - J Kendrick
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - O M Mannion
- Sandia National Laboratories, Albuquerque, New Mexico 87185, USA
| | - H McClow
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - B Stanley
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, New York, New York 14623-1299, USA
| |
Collapse
|
6
|
Shah RC, Cao D, Aghaian L, Bachmann B, Betti R, Campbell EM, Epstein R, Forrest CJ, Forsman A, Glebov VY, Goncharov VN, Gopalaswamy V, Harding DR, Hu SX, Igumenshchev IV, Janezic RT, Keaty L, Knauer JP, Kobs D, Lees A, Mannion OM, Mohamed ZL, Patel D, Rosenberg MJ, Shmayda WT, Stoeckl C, Theobald W, Thomas CA, Volegov P, Woo KM, Regan SP. Bound on hot-spot mix in high-velocity, high-adiabat direct-drive cryogenic implosions based on comparison of absolute x-ray and neutron yields. Phys Rev E 2022; 106:L013201. [PMID: 35974626 DOI: 10.1103/physreve.106.l013201] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/02/2021] [Accepted: 06/29/2022] [Indexed: 06/15/2023]
Abstract
In laser-driven implosions for laboratory fusion, the comparison of hot-spot x-ray yield to neutron production can serve to infer hot-spot mix. For high-performance direct-drive implosions, this ratio depends sensitively on the degree of equilibration between the ion and electron fluids. A scaling for x-ray yield as a function of neutron yield and characteristic ion and electron hot-spot temperatures is developed on the basis of simulations with varying degrees of equilibration. We apply this model to hot-spot x-ray measurements of direct-drive cryogenic implosions typical of the direct-drive designs with best ignition metrics. The comparison of the measured x-ray and neutron yields indicates that hot-spot mix, if present, is below a sensitivity estimated as ∼2% by-atom mix of ablator plastic into the hot spot.
Collapse
Affiliation(s)
- R C Shah
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D Cao
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - L Aghaian
- General Atomics, San Diego, California 92121, USA
| | - B Bachmann
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - E M Campbell
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Epstein
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A Forsman
- General Atomics, San Diego, California 92121, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Gopalaswamy
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D R Harding
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S X Hu
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - I V Igumenshchev
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R T Janezic
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - L Keaty
- General Atomics, San Diego, California 92121, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D Kobs
- General Atomics, San Diego, California 92121, USA
| | - A Lees
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - O M Mannion
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - Z L Mohamed
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D Patel
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M J Rosenberg
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W T Shmayda
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C A Thomas
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - P Volegov
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - K M Woo
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
7
|
Bose A, Peebles J, Walsh CA, Frenje JA, Kabadi NV, Adrian PJ, Sutcliffe GD, Gatu Johnson M, Frank CA, Davies JR, Betti R, Glebov VY, Marshall FJ, Regan SP, Stoeckl C, Campbell EM, Sio H, Moody J, Crilly A, Appelbe BD, Chittenden JP, Atzeni S, Barbato F, Forte A, Li CK, Seguin FH, Petrasso RD. Effect of Strongly Magnetized Electrons and Ions on Heat Flow and Symmetry of Inertial Fusion Implosions. Phys Rev Lett 2022; 128:195002. [PMID: 35622051 DOI: 10.1103/physrevlett.128.195002] [Citation(s) in RCA: 5] [Impact Index Per Article: 2.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/16/2021] [Revised: 02/24/2022] [Accepted: 03/31/2022] [Indexed: 06/15/2023]
Abstract
This Letter presents the first observation on how a strong, 500 kG, externally applied B field increases the mode-two asymmetry in shock-heated inertial fusion implosions. Using a direct-drive implosion with polar illumination and imposed field, we observed that magnetization produces a significant increase in the implosion oblateness (a 2.5× larger P2 amplitude in x-ray self-emission images) compared with reference experiments with identical drive but with no field applied. The implosions produce strongly magnetized electrons (ω_{e}τ_{e}≫1) and ions (ω_{i}τ_{i}>1) that, as shown using simulations, restrict the cross field heat flow necessary for lateral distribution of the laser and shock heating from the implosion pole to the waist, causing the enhanced mode-two shape.
Collapse
Affiliation(s)
- A Bose
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
- Department of Physics and Astronomy, University of Delaware, Newark, Delaware, USA
| | - J Peebles
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - C A Walsh
- Lawrence Livermore National Laboratory, Livermore, California, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - N V Kabadi
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - P J Adrian
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - G D Sutcliffe
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - C A Frank
- Department of Physics and Astronomy, University of Delaware, Newark, Delaware, USA
| | - J R Davies
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - F J Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - E M Campbell
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York, USA
| | - H Sio
- Lawrence Livermore National Laboratory, Livermore, California, USA
| | - J Moody
- Lawrence Livermore National Laboratory, Livermore, California, USA
| | - A Crilly
- Blackett Laboratory, Imperial College, London, United Kingdom
| | - B D Appelbe
- Blackett Laboratory, Imperial College, London, United Kingdom
| | - J P Chittenden
- Blackett Laboratory, Imperial College, London, United Kingdom
| | - S Atzeni
- Dipartimento SBAI, Universita di Roma La Sapienza, Rome, Italy
| | - F Barbato
- Dipartimento SBAI, Universita di Roma La Sapienza, Rome, Italy
| | - A Forte
- Dipartimento SBAI, Universita di Roma La Sapienza, Rome, Italy
- Department of Physics, University of Oxford, Oxford, United Kingdom
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - F H Seguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
| |
Collapse
|
8
|
Mannion OM, Crilly AJ, Forrest CJ, Appelbe BD, Betti R, Glebov VY, Gopalaswamy V, Knauer JP, Mohamed ZL, Stoeckl C, Chittenden JP, Regan SP. Measurements of the temperature and velocity of the dense fuel layer in inertial confinement fusion experiments. Phys Rev E 2022; 105:055205. [PMID: 35706215 DOI: 10.1103/physreve.105.055205] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/31/2021] [Accepted: 04/05/2022] [Indexed: 06/15/2023]
Abstract
The apparent ion temperature and mean velocity of the dense deuterium tritium fuel layer of an inertial confinement fusion target near peak compression have been measured using backscatter neutron spectroscopy. The average isotropic residual kinetic energy of the dense deuterium tritium fuel is estimated using the mean velocity measurement to be ∼103 J across an ensemble of experiments. The apparent ion-temperature measurements from high-implosion velocity experiments are larger than expected from radiation-hydrodynamic simulations and are consistent with enhanced levels of shell decompression. These results suggest that high-mode instabilities may saturate the scaling of implosion performance with the implosion velocity for laser-direct-drive implosions.
Collapse
Affiliation(s)
- O M Mannion
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A J Crilly
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - B D Appelbe
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Gopalaswamy
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - Z L Mohamed
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Chittenden
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
9
|
Kabadi NV, Simpson R, Adrian PJ, Bose A, Frenje JA, Gatu Johnson M, Lahmann B, Li CK, Parker CE, Séguin FH, Sutcliffe GD, Petrasso RD, Atzeni S, Eriksson J, Forrest C, Fess S, Glebov VY, Janezic R, Mannion OM, Rinderknecht HG, Rosenberg MJ, Stoeckl C, Kagan G, Hoppe M, Luo R, Schoff M, Shuldberg C, Sio HW, Sanchez J, Hopkins LB, Schlossberg D, Hahn K, Yeamans C. Thermal decoupling of deuterium and tritium during the inertial confinement fusion shock-convergence phase. Phys Rev E 2021; 104:L013201. [PMID: 34412205 DOI: 10.1103/physreve.104.l013201] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/19/2021] [Accepted: 06/23/2021] [Indexed: 11/07/2022]
Abstract
A series of thin glass-shell shock-driven DT gas-filled capsule implosions was conducted at the OMEGA laser facility. These experiments generate conditions relevant to the central plasma during the shock-convergence phase of ablatively driven inertial confinement fusion (ICF) implosions. The spectral temperatures inferred from the DTn and DDn spectra are most consistent with a two-ion-temperature plasma, where the initial apparent temperature ratio, T_{T}/T_{D}, is 1.5. This is an experimental confirmation of the long-standing conjecture that plasma shocks couple energy directly proportional to the species mass in multi-ion plasmas. The apparent temperature ratio trend with equilibration time matches expected thermal equilibration described by hydrodynamic theory. This indicates that deuterium and tritium ions have different energy distributions for the time period surrounding shock convergence in ignition-relevant ICF implosions.
Collapse
Affiliation(s)
- N V Kabadi
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - R Simpson
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - P J Adrian
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - A Bose
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - B Lahmann
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C E Parker
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - G D Sutcliffe
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - S Atzeni
- Dipartimento SBAI, Universit'a degli Studi di Roma "La Sapienza," Via Antonio Scarpa 14, 00161, Roma, Italy
| | - J Eriksson
- Department of Physics and Astronomy, Uppsala University, SE-752 37 Uppsala, Sweden
| | - C Forrest
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - S Fess
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - V Yu Glebov
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - R Janezic
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - O M Mannion
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - H G Rinderknecht
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - M J Rosenberg
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - C Stoeckl
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - G Kagan
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW7 2AZ, United Kingdom
| | - M Hoppe
- General Atomics, San Diego, California 92121, USA
| | - R Luo
- General Atomics, San Diego, California 92121, USA
| | - M Schoff
- General Atomics, San Diego, California 92121, USA
| | - C Shuldberg
- General Atomics, San Diego, California 92121, USA
| | - H W Sio
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Sanchez
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - L Berzak Hopkins
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D Schlossberg
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - K Hahn
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Yeamans
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| |
Collapse
|
10
|
Mohamed ZL, Mannion OM, Knauer JP, Forrest CJ, Glebov VY, Stoeckl C, Romanofsky MH. Application of an energy-dependent instrument response function to analysis of nTOF data from cryogenic DT experiments. Rev Sci Instrum 2021; 92:043546. [PMID: 34243381 DOI: 10.1063/5.0043647] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/10/2021] [Accepted: 04/07/2021] [Indexed: 06/13/2023]
Abstract
Neutron time-of-flight (nTOF) detectors are used to diagnose the conditions present in inertial confinement fusion (ICF) experiments and basic laboratory physics experiments performed on an ICF platform. The instrument response function (IRF) of these detectors is constructed by convolution of two components: an x-ray IRF and a neutron interaction response. The shape of the neutron interaction response varies with incident neutron energy, changing the shape of the total IRF. Analyses of nTOF data that span a broad range of energies must account for this energy-dependence in order to accurately infer plasma parameters and nuclear properties in ICF experiments. This work briefly reviews a matrix multiplication approach to convolution, which allows for an energy-dependent change in the shape of the IRF. This method is applied to synthetic data resembling symmetric cryogenic DT implosions to examine the effect of the energy-dependent IRF on the inferred areal density. The results of forward fits that infer ion temperatures and areal densities from nTOF data collected during cryogenic DT experiments on OMEGA are also discussed.
Collapse
Affiliation(s)
- Z L Mohamed
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - O M Mannion
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M H Romanofsky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
11
|
Johnson TM, Birkel A, Ramirez HE, Sutcliffe GD, Adrian PJ, Glebov VY, Sio H, Johnson MG, Frenje JA, Petrasso RD, Li CK. Yield degradation due to laser drive asymmetry in D 3He backlit proton radiography experiments at OMEGA. Rev Sci Instrum 2021; 92:043551. [PMID: 34243410 DOI: 10.1063/5.0043004] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/05/2021] [Accepted: 03/31/2021] [Indexed: 06/13/2023]
Abstract
Mono-energetic proton radiography is a vital diagnostic for numerous high-energy-density-physics, inertial-confinement-fusion, and laboratory-astrophysics experiments at OMEGA. With a large number of campaigns executing hundreds of shots, general trends in D3He backlighter performance are statistically observed. Each experimental configuration uses a different number of beams and drive symmetry, causing the backlighter to perform differently. Here, we analyze the impact of these variables on the overall performance of the D3He backlighter for proton-radiography studies. This study finds that increasing laser drive asymmetry can degrade the performance of the D3He backlighter. The results of this study can be used to help experimental designs that use proton radiography.
Collapse
Affiliation(s)
- T M Johnson
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - A Birkel
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H E Ramirez
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - G D Sutcliffe
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P J Adrian
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - H Sio
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| |
Collapse
|
12
|
Mannion OM, Woo KM, Crilly AJ, Forrest CJ, Frenje JA, Johnson MG, Glebov VY, Knauer JP, Mohamed ZL, Romanofsky MH, Stoeckl C, Theobald W, Regan SP. Reconstructing 3D asymmetries in laser-direct-drive implosions on OMEGA. Rev Sci Instrum 2021; 92:033529. [PMID: 33819982 DOI: 10.1063/5.0043514] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/08/2021] [Accepted: 02/24/2021] [Indexed: 06/12/2023]
Abstract
Three-dimensional reconstruction algorithms have been developed, which determine the hot-spot velocity, hot-spot apparent ion temperature distribution, and fuel areal-density distribution present in laser-direct-drive inertial confinement fusion implosions on the OMEGA laser. These reconstructions rely on multiple independent measurements of the neutron energy spectrum emitted from the fusing plasma. Measurements of the neutron energy spectrum on OMEGA are made using a suite of quasi-orthogonal neutron time-of-flight detectors and a magnetic recoil spectrometer. These spectrometers are positioned strategically around the OMEGA target chamber to provide unique 3D measurements of the conditions of the fusing hot spot and compressed fuel near peak compression. The uncertainties involved in these 3D reconstructions are discussed and are used to identify a new nTOF diagnostic line of sight, which when built will reduce the uncertainty in the hot-spot apparent ion temperature distribution from 700 to <400 eV.
Collapse
Affiliation(s)
- O M Mannion
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - K M Woo
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A J Crilly
- Centre for Inertial Fusion Studies, The Blackett Laboratory, Imperial College, London SW72AZ, United Kingdom
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Frenje
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - Z L Mohamed
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M H Romanofsky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
13
|
Gatu Johnson M, Aguirre B, Armstrong J, Fooks JA, Forrest C, Frenje JA, Glebov VY, Hoppe M, Katz J, Knauer JP, Martin W, Parker CE, Reynolds HG, Schoff ME, Séguin FH, Sorce C, Sperry B, Stoeckl C, Petrasso RD. Using millimeter-sized carbon-deuterium foils for high-precision deuterium-tritium neutron spectrum measurements in direct-drive inertial confinement fusion at the OMEGA laser facility. Rev Sci Instrum 2021; 92:023503. [PMID: 33648107 DOI: 10.1063/5.0040549] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/14/2020] [Accepted: 01/23/2021] [Indexed: 06/12/2023]
Abstract
Millimeter-sized CD foils fielded close (order mm) to inertial confinement fusion (ICF) implosions have been proposed as a game-changer for improving energy resolution and allowing time-resolution in neutron spectrum measurements using the magnetic recoil technique. This paper presents results from initial experiments testing this concept for direct drive ICF at the OMEGA Laser Facility. While the foils are shown to produce reasonable signals, inferred spectral broadening is seen to be high (∼5 keV) and signal levels are low (by ∼20%) compared to expectation. Before this type of foil is used for precision experiments, the foil mount must be improved, oxygen uptake in the foils must be better characterized, and impact of uncontrolled foil motion prior to detection must be investigated.
Collapse
Affiliation(s)
- M Gatu Johnson
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - B Aguirre
- Sandia National Laboratories, Albuquerque, New Mexico 87123, USA
| | - J Armstrong
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Fooks
- General Atomics, San Diego, California 92186, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Frenje
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Hoppe
- General Atomics, San Diego, California 92186, USA
| | - J Katz
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W Martin
- Sandia National Laboratories, Albuquerque, New Mexico 87123, USA
| | - C E Parker
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - H G Reynolds
- General Atomics, San Diego, California 92186, USA
| | - M E Schoff
- General Atomics, San Diego, California 92186, USA
| | - F H Séguin
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C Sorce
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - B Sperry
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R D Petrasso
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| |
Collapse
|
14
|
Glebov VY, Stoeckl C, Forrest CJ, Knauer JP, Mannion OM, Romanofsky MH, Sangster TC, Regan SP. A novel photomultiplier tube neutron time-of-flight detector. Rev Sci Instrum 2021; 92:013509. [PMID: 33514216 DOI: 10.1063/5.0029005] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/10/2020] [Accepted: 12/26/2020] [Indexed: 06/12/2023]
Abstract
A traditional neutron time-of-flight (nTOF) detector used in inertial confinement fusion consists of a scintillator coupled with a photomultiplier tube (PMT). The instrument response function (IRF) of such a detector is dominated by the scintillator-light decay. In DT implosions with neutron yield larger than 1013, a novel detector consisting of a microchannel-plate (MCP) photomultiplier tube in a housing without a scintillator (PMT nTOF) can be used to measure DT yield, ion temperature, and neutron velocity. Most of the neutron signals in PMT nTOF detectors are produced from neutron interaction with a PMT window. The direct interaction of neutrons with the MCP provides negligible contribution. The elimination of the scintillator removes the scintillator decay from the instrument response function and makes the IRF of the PMT nTOF detector faster, which makes the ion temperature and neutron velocity measurements more accurate. Three PMT nTOF detectors were deployed in the OMEGA laser system for the first time to diagnose inertial confinement fusion plasma. The design details, characteristics, and calibration results of these detectors in DT implosions on OMEGA are presented. Recommendations on the use of different PMTs for specific applications are provided.
Collapse
Affiliation(s)
- V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - O M Mannion
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - M H Romanofsky
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| |
Collapse
|
15
|
Ruby JJ, Rygg JR, Chin DA, Gaffney JA, Adrian PJ, Bishel D, Forrest CJ, Glebov VY, Kabadi NV, Nilson PM, Ping Y, Stoeckl C, Collins GW. Constraining physical models at gigabar pressures. Phys Rev E 2020; 102:053210. [PMID: 33327091 DOI: 10.1103/physreve.102.053210] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/26/2020] [Accepted: 11/02/2020] [Indexed: 11/07/2022]
Abstract
High-energy-density (HED) experiments in convergent geometry are able to test physical models at pressures beyond hundreds of millions of atmospheres. The measurements from these experiments are generally highly integrated and require unique analysis techniques to procure quantitative information. This work describes a methodology to constrain the physics in convergent HED experiments by adapting the methods common to many other fields of physics. As an example, a mechanical model of an imploding shell is constrained by data from a thin-shelled direct-drive exploding-pusher experiment on the OMEGA laser system using Bayesian inference, resulting in the reconstruction of the shell dynamics and energy transfer during the implosion. The model is tested by analyzing synthetic data from a one-dimensional hydrodynamics code and is sampled using a Markov chain Monte Carlo to generate the posterior distributions of the model parameters. The goal of this work is to demonstrate a general methodology that can be used to draw conclusions from a wide variety of HED experiments.
Collapse
Affiliation(s)
- J J Ruby
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.,Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - J R Rygg
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.,Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627, USA
| | - D A Chin
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.,Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - J A Gaffney
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - P J Adrian
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - D Bishel
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.,Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - N V Kabadi
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P M Nilson
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - Y Ping
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - G W Collins
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA.,Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627, USA
| |
Collapse
|
16
|
Ruby JJ, Rygg JR, Chin DA, Gaffney JA, Adrian PJ, Forrest CJ, Glebov VY, Kabadi NV, Nilson PM, Ping Y, Stoeckl C, Collins GW. Energy Flow in Thin Shell Implosions and Explosions. Phys Rev Lett 2020; 125:215001. [PMID: 33274978 DOI: 10.1103/physrevlett.125.215001] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/26/2020] [Accepted: 10/30/2020] [Indexed: 06/12/2023]
Abstract
Energy flow and balance in convergent systems beyond petapascal energy densities controls the fate of late-stage stars and the potential for controlling thermonuclear inertial fusion ignition. Time-resolved x-ray self-emission imaging combined with a Bayesian inference analysis is used to describe the energy flow and the potential information stored in the rebounding spherical shock at 0.22 PPa (2.2 Gbar or billions of atmospheres pressure). This analysis, together with a simple mechanical model, describes the trajectory of the shell and the time history of the pressure at the fuel-shell interface, ablation pressure, and energy partitioning including kinetic energy of the shell and internal energy of the fuel. The techniques used here provide a fully self-consistent uncertainty analysis of integrated implosion data, a thermodynamic-path independent measurement of pressure in the petapascal range, and can be used to deduce the energy flow in a wide variety of implosion systems to petapascal energy densities.
Collapse
Affiliation(s)
- J J Ruby
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - J R Rygg
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627, USA
| | - D A Chin
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - J A Gaffney
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - P J Adrian
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - N V Kabadi
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P M Nilson
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - Y Ping
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - G W Collins
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627, USA
| |
Collapse
|
17
|
Haines BM, Shah RC, Smidt JM, Albright BJ, Cardenas T, Douglas MR, Forrest C, Glebov VY, Gunderson MA, Hamilton CE, Henderson KC, Kim Y, Lee MN, Murphy TJ, Oertel JA, Olson RE, Patterson BM, Randolph RB, Schmidt DW. Observation of persistent species temperature separation in inertial confinement fusion mixtures. Nat Commun 2020; 11:544. [PMID: 31992703 PMCID: PMC6987117 DOI: 10.1038/s41467-020-14412-y] [Citation(s) in RCA: 25] [Impact Index Per Article: 6.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/05/2019] [Accepted: 12/17/2019] [Indexed: 11/09/2022] Open
Abstract
The injection and mixing of contaminant mass into the fuel in inertial confinement fusion (ICF) implosions is a primary factor preventing ignition. ICF experiments have recently achieved an alpha-heating regime, in which fusion self-heating is the dominant source of yield, by reducing the susceptibility of implosions to instabilities that inject this mass. We report the results of unique separated reactants implosion experiments studying pre-mixed contaminant as well as detailed high-resolution three-dimensional simulations that are in good agreement with experiments. At conditions relevant to mixing regions in high-yield implosions, we observe persistent chunks of contaminant that do not achieve thermal equilibrium with the fuel throughout the burn phase. The assumption of thermal equilibrium is made in nearly all computational ICF modeling and methods used to infer levels of contaminant from experiments. We estimate that these methods may underestimate the amount of contaminant by a factor of two or more.
Collapse
Affiliation(s)
- Brian M Haines
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA.
| | - R C Shah
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, NY, 14623, USA
| | - J M Smidt
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - B J Albright
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - T Cardenas
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - M R Douglas
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, NY, 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, NY, 14623, USA
| | - M A Gunderson
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - C E Hamilton
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - K C Henderson
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - Y Kim
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - M N Lee
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - T J Murphy
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - J A Oertel
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - R E Olson
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - B M Patterson
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - R B Randolph
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| | - D W Schmidt
- Los Alamos National Laboratory, P.O. Box 1663, MS T087, Los Alamos, NM, 87545, USA
| |
Collapse
|
18
|
Zylstra AB, Herrmann HW, Kim YH, McEvoy A, Meaney K, Glebov VY, Forrest C, Rubery M. Improved calibration of the OMEGA gas Cherenkov detector. Rev Sci Instrum 2019; 90:123504. [PMID: 31893806 DOI: 10.1063/1.5128765] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/22/2019] [Accepted: 11/24/2019] [Indexed: 06/10/2023]
Abstract
Inertial fusion implosions are diagnosed using γ rays to characterize the implosion physics or measure basic nuclear properties, including cross sections. For the latter, previously reported measurements at laser facilities using gas Cherenkov detectors are limited by a large systematic uncertainty in the detector response. We present a novel in situ calibration technique using neutron inelastic scattering, which we apply to the new GCD-3 detector. The calibration accuracy is improved by ∼3× over the previous method.
Collapse
Affiliation(s)
- A B Zylstra
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - H W Herrmann
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - Y H Kim
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A McEvoy
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - K Meaney
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Rubery
- Plasma Physics Department, AWE plc, Reading RG7 4PR, United Kingdom
| |
Collapse
|
19
|
Ruskov E, Glebov VY, Darling TW, Wessel FJ, Conti F, Valenzuela JC, Rahman HU, Beg FN. Gated liquid scintillator detector for neutron time of flight measurements in a gas-puff Z-pinch experiment. Rev Sci Instrum 2019; 90:073505. [PMID: 31370449 DOI: 10.1063/1.5090785] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/29/2019] [Accepted: 07/06/2019] [Indexed: 06/10/2023]
Abstract
Detection of secondary D(t, n)4He neutrons produced when thin argon or krypton gas shells implode on a deuterium gas target is a very challenging task because the secondary neutron yield is a small fraction of the primary neutron yield and because the implosion is often accompanied by an intense hard X-ray burst. We built a large volume neutron time of flight (nTOF) detector using liquid scintillator (xylene solvent with small quantities of wavelength shifting PPO + bis-MSB fluors) in an attempt to increase the detection probability for secondary neutrons in our staged Z-pinch experiments at the 1 MA Zebra pulsed-power generator. Two fast, gated microchannel plate photomultiplier tubes detect the light created in 21 liters of liquid. The hard X-rays were successfully suppressed in the recorded nTOF traces, but we found no evidence of secondary neutrons. The signal quality from the primary D(d, n)3He neutrons was higher compared to the signal quality from a plastic scintillator nTOF, thus providing a more reliable estimate of the deuterium ion temperature at the pinch stagnation time. Cross-calibration with a silver activation detector enables standalone neutron yield measurement.
Collapse
Affiliation(s)
- E Ruskov
- Magneto-Inertial Fusion Technologies, Inc., Tustin, California 92612, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - T W Darling
- University of Nevada, Reno, Reno, Nevada 89557, USA
| | - F J Wessel
- L-Egant Solutions, LLC, Irvine, California 92606, USA
| | - F Conti
- University of California, San Diego, La Jolla, California 92093, USA
| | - J C Valenzuela
- University of California, San Diego, La Jolla, California 92093, USA
| | - H U Rahman
- Magneto-Inertial Fusion Technologies, Inc., Tustin, California 92612, USA
| | - F N Beg
- University of California, San Diego, La Jolla, California 92093, USA
| |
Collapse
|
20
|
Gopalaswamy V, Betti R, Knauer JP, Luciani N, Patel D, Woo KM, Bose A, Igumenshchev IV, Campbell EM, Anderson KS, Bauer KA, Bonino MJ, Cao D, Christopherson AR, Collins GW, Collins TJB, Davies JR, Delettrez JA, Edgell DH, Epstein R, Forrest CJ, Froula DH, Glebov VY, Goncharov VN, Harding DR, Hu SX, Jacobs-Perkins DW, Janezic RT, Kelly JH, Mannion OM, Maximov A, Marshall FJ, Michel DT, Miller S, Morse SFB, Palastro J, Peebles J, Radha PB, Regan SP, Sampat S, Sangster TC, Sefkow AB, Seka W, Shah RC, Shmyada WT, Shvydky A, Stoeckl C, Solodov AA, Theobald W, Zuegel JD, Johnson MG, Petrasso RD, Li CK, Frenje JA. Tripled yield in direct-drive laser fusion through statistical modelling. Nature 2019; 565:581-586. [PMID: 30700868 DOI: 10.1038/s41586-019-0877-0] [Citation(s) in RCA: 69] [Impact Index Per Article: 13.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/01/2018] [Accepted: 12/04/2018] [Indexed: 11/09/2022]
Abstract
Focusing laser light onto a very small target can produce the conditions for laboratory-scale nuclear fusion of hydrogen isotopes. The lack of accurate predictive models, which are essential for the design of high-performance laser-fusion experiments, is a major obstacle to achieving thermonuclear ignition. Here we report a statistical approach that was used to design and quantitatively predict the results of implosions of solid deuterium-tritium targets carried out with the 30-kilojoule OMEGA laser system, leading to tripling of the fusion yield to its highest value so far for direct-drive laser fusion. When scaled to the laser energies of the National Ignition Facility (1.9 megajoules), these targets are predicted to produce a fusion energy output of about 500 kilojoules-several times larger than the fusion yields currently achieved at that facility. This approach could guide the exploration of the vast parameter space of thermonuclear ignition conditions and enhance our understanding of laser-fusion physics.
Collapse
Affiliation(s)
- V Gopalaswamy
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA. .,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA.
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA.,Department of Physics and Astronomy, University of Rochester, Rochester, NY, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - N Luciani
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA.,Dipartimento di Energetica, Politecnico di Milano, Milan, Italy
| | - D Patel
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA
| | - K M Woo
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Physics and Astronomy, University of Rochester, Rochester, NY, USA
| | - A Bose
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Massachusetts Institute of Technology, Cambridge, MA, USA
| | - I V Igumenshchev
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - E M Campbell
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - K S Anderson
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - K A Bauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - M J Bonino
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - D Cao
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - A R Christopherson
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA
| | - G W Collins
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - T J B Collins
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J R Davies
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J A Delettrez
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - D H Edgell
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - R Epstein
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - D H Froula
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - V Y Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - D R Harding
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - S X Hu
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - D W Jacobs-Perkins
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - R T Janezic
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J H Kelly
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - O M Mannion
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Physics and Astronomy, University of Rochester, Rochester, NY, USA
| | - A Maximov
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA
| | - F J Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - D T Michel
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - S Miller
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA.,Department of Mechanical Engineering, University of Rochester, Rochester, NY, USA
| | - S F B Morse
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J Palastro
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J Peebles
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - P B Radha
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - S Sampat
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - A B Sefkow
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - W Seka
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - R C Shah
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - W T Shmyada
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - A Shvydky
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - A A Solodov
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J D Zuegel
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Cambridge, MA, USA
| | - R D Petrasso
- Massachusetts Institute of Technology, Cambridge, MA, USA
| | - C K Li
- Massachusetts Institute of Technology, Cambridge, MA, USA
| | - J A Frenje
- Massachusetts Institute of Technology, Cambridge, MA, USA
| |
Collapse
|
21
|
Frenje JA, Florido R, Mancini R, Nagayama T, Grabowski PE, Rinderknecht H, Sio H, Zylstra A, Gatu Johnson M, Li CK, Séguin FH, Petrasso RD, Glebov VY, Regan SP. Experimental Validation of Low-Z Ion-Stopping Formalisms around the Bragg Peak in High-Energy-Density Plasmas. Phys Rev Lett 2019; 122:015002. [PMID: 31012651 DOI: 10.1103/physrevlett.122.015002] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/05/2018] [Revised: 10/21/2018] [Indexed: 06/09/2023]
Abstract
We report on the first accurate validation of low-Z ion-stopping formalisms in the regime ranging from low-velocity ion stopping-through the Bragg peak-to high-velocity ion stopping in well-characterized high-energy-density plasmas. These measurements were executed at electron temperatures and number densities in the range of 1.4-2.8 keV and 4×10^{23}-8×10^{23} cm^{-3}, respectively. For these conditions, it is experimentally demonstrated that the Brown-Preston-Singleton formalism provides a better description of the ion stopping than other formalisms around the Bragg peak, except for the ion stopping at v_{i}∼0.3v_{th}, where the Brown-Preston-Singleton formalism significantly underpredicts the observation. It is postulated that the inclusion of nuclear-elastic scattering, and possibly coupled modes of the plasma ions, in the modeling of the ion-ion interaction may explain the discrepancy of ∼20% at this velocity, which would have an impact on our understanding of the alpha energy deposition and heating of the fuel ions, and thus reduce the ignition threshold in an ignition experiment.
Collapse
Affiliation(s)
- J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R Florido
- iUNAT-Departamento de Física, Universidad de Las Palmas de Gran Canaria, 35017 Las Palmas de Gran Canaria, Spain
| | - R Mancini
- Physics Department, University of Nevada, Reno, Nevada 89557, USA
| | - T Nagayama
- Sandia National Laboratory, Albuquerque, New Mexico 87185, USA
| | - P E Grabowski
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - H Rinderknecht
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - H Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - A Zylstra
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
22
|
Gatu Johnson M, Katz J, Forrest C, Frenje JA, Glebov VY, Li CK, Paguio R, Parker CE, Robillard C, Sangster TC, Schoff M, Séguin FH, Stoeckl C, Petrasso RD. Measurement of apparent ion temperature using the magnetic recoil spectrometer at the OMEGA laser facility. Rev Sci Instrum 2018; 89:10I129. [PMID: 30399924 DOI: 10.1063/1.5035287] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/13/2018] [Accepted: 06/05/2018] [Indexed: 06/08/2023]
Abstract
The Magnetic Recoil neutron Spectrometer (MRS) at the OMEGA laser facility has been routinely used to measure deuterium-tritium (DT) yield and areal density in cryogenically layered implosions since 2008. Recently, operation of the OMEGA MRS in higher-resolution mode with a new smaller, thinner (4 cm2, 57 μm thick) CD2 conversion foil has also enabled inference of the apparent DT ion temperature (T ion) from MRS data. MRS-inferred T ion compares well with T ion as measured using neutron time-of-flight spectrometers, which is important as it demonstrates good understanding of the very different systematics associated with the two independent measurements. The MRS resolution in this configuration, ΔE MRS = 0.91 MeV FWHM, is still higher than that required for a high-precision T ion measurement. We show how fielding a smaller foil closer to the target chamber center and redesigning the MRS detector array could bring the resolution to ΔE MRS = 0.45 MeV, reducing the systematic T ion uncertainty by more than a factor of 4.
Collapse
Affiliation(s)
- M Gatu Johnson
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - J Katz
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Frenje
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C K Li
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - R Paguio
- General Atomics, San Diego, California 92186, USA
| | - C E Parker
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C Robillard
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Schoff
- General Atomics, San Diego, California 92186, USA
| | - F H Séguin
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R D Petrasso
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| |
Collapse
|
23
|
Mannion OM, Glebov VY, Forrest CJ, Knauer JP, Goncharov VN, Regan SP, Sangster TC, Stoeckl C, Gatu Johnson M. Calibration of a neutron time-of-flight detector with a rapid instrument response function for measurements of bulk fluid motion on OMEGA. Rev Sci Instrum 2018; 89:10I131. [PMID: 30399681 DOI: 10.1063/1.5037324] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/23/2018] [Accepted: 07/03/2018] [Indexed: 06/08/2023]
Abstract
A newly developed neutron time-of-flight (nTOF) diagnostic with a fast instrument response function has been fielded on the OMEGA laser in a highly collimated line of sight. By using a small plastic scintillator volume, the detector provides a narrow instrument response of 1.7 ns full width at half maximum while maintaining a large signal-to-noise ratio for neutron yields between 1010 and 1014. The OMEGA hardware timing system is used along with an optical fiducial to provide an absolute nTOF measurement to an accuracy of ∼56 ps. The fast instrument response enables the accurate measurement of the primary deuterium-tritium neutron peak shape, while the optical fiducial allows for an absolute neutron energy measurement. The new detector measures the neutron mean energy with an uncertainty of ∼7 keV, corresponding to a hot-spot velocity projection uncertainty of ∼12 km/s. Evidence of bulk fluid motion in cryogenic targets is presented with measurements of the neutron energy spectrum.
Collapse
Affiliation(s)
- O M Mannion
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C J Forrest
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V N Goncharov
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S P Regan
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory or Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| |
Collapse
|
24
|
Glebov VY, Eckart MJ, Forrest CJ, Grim GP, Hartouni EP, Hatarik R, Knauer JP, Moore AS, Regan SP, Sangster TC, Schlossberg DJ, Stoeckl C. Testing a Cherenkov neutron time-of-flight detector on OMEGA. Rev Sci Instrum 2018; 89:10I122. [PMID: 30399883 DOI: 10.1063/1.5035289] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/13/2018] [Accepted: 06/13/2018] [Indexed: 06/08/2023]
Abstract
A Cherenkov neutron time-of-flight (nTOF) detector developed and constructed at Lawrence Livermore National Laboratory was tested at 13 m from the target in a collimated line of sight (LOS) and at 5.3 m from the target in the open space inside the OMEGA Target Bay. Neutrons interacting with the quartz rod generate gammas, which through Compton scattering produce relativistic electrons that give rise to Cherenkov light. A photomultiplier tube (PMT) transferred the Cherenkov light into an amplified electrical signal. The Cherenkov nTOF detector consists of an 8-mm-diam, 25-cm quartz hexagonal prism coupled with a Hamamatsu gated PMT R5916U-52. The tests were performed with DT direct-drive implosions with cryogenic and room-temperature targets, producing a wide range of neutron yields and ion temperatures. The results of the tests and comparison with other nTOF detectors on OMEGA are presented. In the collimated LOS at 13 m from the target, the Cherenkov nTOF detector demonstrated good precision measurement in both the yield and ion temperature for DT yields above 3 × 1013.
Collapse
Affiliation(s)
- V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - M J Eckart
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - G P Grim
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - E P Hartouni
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R Hatarik
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - A S Moore
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - D J Schlossberg
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| |
Collapse
|
25
|
Gatu Johnson M, Forrest CJ, Sayre DB, Bacher A, Bourgade JL, Brune CR, Caggiano JA, Casey DT, Frenje JA, Glebov VY, Hale GM, Hatarik R, Herrmann HW, Janezic R, Kim YH, Knauer JP, Landoas O, McNabb DP, Paris MW, Petrasso RD, Pino JE, Quaglioni S, Rosse B, Sanchez J, Sangster TC, Sio H, Shmayda W, Stoeckl C, Thompson I, Zylstra AB. Experimental Evidence of a Variant Neutron Spectrum from the T(t,2n)α Reaction at Center-of-Mass Energies in the Range of 16-50 keV. Phys Rev Lett 2018; 121:042501. [PMID: 30095940 DOI: 10.1103/physrevlett.121.042501] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/02/2017] [Revised: 03/20/2018] [Indexed: 06/08/2023]
Abstract
Full calculations of six-nucleon reactions with a three-body final state have been elusive and a long-standing issue. We present neutron spectra from the T(t,2n)α (TT) reaction measured in inertial confinement fusion experiments at the OMEGA laser facility at ion temperatures from 4 to 18 keV, corresponding to center-of-mass energies (E_{c.m.}) from 16 to 50 keV. A clear difference in the shape of the TT-neutron spectrum is observed between the two E_{c.m.}, with the ^{5}He ground state resonant peak at 8.6 MeV being significantly stronger at the higher than at the lower energy. The data provide the first conclusive evidence of a variant TT-neutron spectrum in this E_{c.m.} range. In contrast to earlier available data, this indicates a reaction mechanism that must involve resonances and/or higher angular momenta than L=0. This finding provides an important experimental constraint on theoretical efforts that explore this and complementary six-nucleon systems, such as the solar ^{3}He(^{3}He,2p)α reaction.
Collapse
Affiliation(s)
- M Gatu Johnson
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D B Sayre
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Bacher
- Indiana University, Bloomington, Indiana 47405, USA
| | | | - C R Brune
- Ohio University, Athens, Ohio 45701, USA
| | - J A Caggiano
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D T Casey
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J A Frenje
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - G M Hale
- Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA
| | - R Hatarik
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - H W Herrmann
- Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA
| | - R Janezic
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - Y H Kim
- Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - O Landoas
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - D P McNabb
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M W Paris
- Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA
| | - R D Petrasso
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - J E Pino
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S Quaglioni
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B Rosse
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - J Sanchez
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - H Sio
- Massachusetts Institute of Technology Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - W Shmayda
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - I Thompson
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A B Zylstra
- Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA
| |
Collapse
|
26
|
Zylstra AB, Hoffman NM, Herrmann HW, Schmitt MJ, Kim YH, Meaney K, Leatherland A, Gales S, Forrest C, Glebov VY, Schoff M, Hoppe M, Ravelo N. Diffusion-dominated mixing in moderate convergence implosions. Phys Rev E 2018; 97:061201. [PMID: 30011491 DOI: 10.1103/physreve.97.061201] [Citation(s) in RCA: 12] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/01/2017] [Indexed: 11/06/2022]
Abstract
High-Z material mixed into the fuel degrades inertial fusion implosions and can prevent ignition. Mix is often assumed to be dominated by hydrodynamic instabilities, but we report Omega data, using shells with ∼150nm deuterated layers to gain unprecedented resolution, which give strong evidence that the dominant mix mechanism is diffusion for these moderate temperature (≲6 keV) and convergence (∼12) implosions. Small-scale instability-driven or turbulent mix is negligible.
Collapse
Affiliation(s)
- A B Zylstra
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - N M Hoffman
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - H W Herrmann
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - M J Schmitt
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - Y H Kim
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - K Meaney
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A Leatherland
- Plasma Physics Department, AWE plc, Reading RG7 4PR, United Kingdom
| | - S Gales
- Plasma Physics Department, AWE plc, Reading RG7 4PR, United Kingdom
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Schoff
- General Atomics, San Diego, California 92186, USA
| | - M Hoppe
- General Atomics, San Diego, California 92186, USA
| | - N Ravelo
- General Atomics, San Diego, California 92186, USA
| |
Collapse
|
27
|
Marshall FJ, Bahr RE, Goncharov VN, Glebov VY, Peng B, Regan SP, Sangster TC, Stoeckl C. A framed, 16-image Kirkpatrick-Baez x-ray microscope. Rev Sci Instrum 2017; 88:093702. [PMID: 28964245 DOI: 10.1063/1.5000737] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/20/2017] [Accepted: 08/17/2017] [Indexed: 06/07/2023]
Abstract
A 16-image Kirkpatrick-Baez (KB)-type x-ray microscope consisting of compact KB mirrors [F. J. Marshall, Rev. Sci. Instrum. 83, 10E518 (2012)] has been assembled for the first time with mirrors aligned to allow it to be coupled to a high-speed framing camera. The high-speed framing camera has four independently gated strips whose emission sampling interval is ∼30 ps. Images are arranged four to a strip with ∼60-ps temporal spacing between frames on a strip. By spacing the timing of the strips, a frame spacing of ∼15 ps is achieved. A framed resolution of ∼6-μm is achieved with this combination in a 400-μm region of laser-plasma x-ray emission in the 2- to 8-keV energy range. A principal use of the microscope is to measure the evolution of the implosion stagnation region of cryogenic DT target implosions on the University of Rochester's OMEGA Laser System [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)]. The unprecedented time and spatial resolutions achieved with this framed, multi-image KB microscope have made it possible to accurately determine the cryogenic implosion core emission size and shape at the peak of stagnation. These core size measurements, taken in combination with those of ion temperature, neutron-production temporal width, and neutron yield allow for inference of core pressures, currently exceeding 50 Gbar in OMEGA cryogenic target implosions [Regan et al., Phys. Rev. Lett. 117, 025001 (2016)].
Collapse
Affiliation(s)
- F J Marshall
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - R E Bahr
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - B Peng
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, 250 E. River Rd., Rochester, New York 14623, USA
| |
Collapse
|
28
|
Michel DT, Hu SX, Davis AK, Glebov VY, Goncharov VN, Igumenshchev IV, Radha PB, Stoeckl C, Froula DH. Measurement of the shell decompression in direct-drive inertial-confinement-fusion implosions. Phys Rev E 2017; 95:051202. [PMID: 28618558 DOI: 10.1103/physreve.95.051202] [Citation(s) in RCA: 14] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/31/2016] [Indexed: 11/07/2022]
Abstract
A series of direct-drive implosions performed on OMEGA were used to isolate the effect of an adiabat on the in-flight shell thickness. The maximum in-flight shell thickness was measured to decrease from 75±2 to 60±2μm when the adiabat of the shell was reduced from 6 to 4.5, but when decreasing the adiabat further (1.8), the shell thickness increased to 75±2μm due to the growth of the Rayleigh-Taylor instability. Hydrodynamic simulations suggest that a laser imprint is the dominant seed for these nonuniformities.
Collapse
Affiliation(s)
- D T Michel
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - S X Hu
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - A K Davis
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - I V Igumenshchev
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - P B Radha
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| | - D H Froula
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14636, USA
| |
Collapse
|
29
|
Zylstra AB, Herrmann HW, Kim YH, McEvoy AM, Schmitt MJ, Hale G, Forrest C, Glebov VY, Stoeckl C. Simultaneous measurement of the HT and DT fusion burn histories in inertial fusion implosions. Rev Sci Instrum 2017; 88:053504. [PMID: 28571443 DOI: 10.1063/1.4983923] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
Measuring the thermonuclear burn history is an important way to diagnose inertial fusion implosions. Using the gas Cherenkov detectors at the OMEGA laser facility, we measure the HT fusion burn in a H2+T2 gas-fueled implosion for the first time. Using multiple detectors with varied Cherenkov thresholds, we demonstrate a technique for simultaneously measuring both the HT and DT burn histories from an implosion where the total reaction yields are comparable. This new technique will be used to study material mixing and kinetic phenomena in implosions.
Collapse
Affiliation(s)
- A B Zylstra
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - H W Herrmann
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - Y H Kim
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A M McEvoy
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - M J Schmitt
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - G Hale
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
30
|
Forrest CJ, Radha PB, Knauer JP, Glebov VY, Goncharov VN, Regan SP, Rosenberg MJ, Sangster TC, Shmayda WT, Stoeckl C, Gatu Johnson M. First Measurements of Deuterium-Tritium and Deuterium-Deuterium Fusion Reaction Yields in Ignition-Scalable Direct-Drive Implosions. Phys Rev Lett 2017; 118:095002. [PMID: 28306316 DOI: 10.1103/physrevlett.118.095002] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/05/2016] [Indexed: 06/06/2023]
Abstract
The deuterium-tritium (D-T) and deuterium-deuterium neutron yield ratio in cryogenic inertial confinement fusion (ICF) experiments is used to examine multifluid effects, traditionally not included in ICF modeling. This ratio has been measured for ignition-scalable direct-drive cryogenic DT implosions at the Omega Laser Facility [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)OPCOB80030-401810.1016/S0030-4018(96)00325-2] using a high-dynamic-range neutron time-of-flight spectrometer. The experimentally inferred yield ratio is consistent with both the calculated values of the nuclear reaction rates and the measured preshot target-fuel composition. These observations indicate that the physical mechanisms that have been proposed to alter the fuel composition, such as species separation of the hydrogen isotopes [D. T. Casey et al., Phys. Rev. Lett. 108, 075002 (2012)PRLTAO0031-900710.1103/PhysRevLett.108.075002], are not significant during the period of peak neutron production in ignition-scalable cryogenic direct-drive DT implosions.
Collapse
Affiliation(s)
- C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - P B Radha
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M J Rosenberg
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W T Shmayda
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| |
Collapse
|
31
|
Forrest CJ, Glebov VY, Goncharov VN, Knauer JP, Radha PB, Regan SP, Romanofsky MH, Sangster TC, Shoup MJ, Stoeckl C. High-dynamic-range neutron time-of-flight detector used to infer the D(t,n) 4He and D(d,n) 3He reaction yield and ion temperature on OMEGA. Rev Sci Instrum 2016; 87:11D814. [PMID: 27910405 DOI: 10.1063/1.4960412] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/06/2023]
Abstract
Upgraded microchannel-plate-based photomultiplier tubes (MCP-PMT's) with increased stability to signal-shape linearity have been implemented on the 13.4-m neutron time-of-flight (nTOF) detector at the Omega Laser Facility. This diagnostic uses oxygenated xylene doped with diphenyloxazole C15H11NO + p-bis-(o-methylstyryl)-benzene (PPO + bis-MSB) wavelength shifting dyes and is coupled through four viewing ports to fast-gating MCP-PMT's, each with a different gain to allow one to measure the light output over a dynamic range of 1 × 106. With these enhancements, the 13.4-m nTOF can measure the D(t,n)4He and D(d,n)3He reaction yields and average ion temperatures in a single line of sight. Once calibrated for absolute neutron sensitivity, the nTOF detectors can be used to measure the neutron yield from 1 × 109 to 1 × 1014 and the ion temperature with an accuracy approaching 5% for both the D(t,n)4He and D(d,n)3He reactions.
Collapse
Affiliation(s)
- C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - P B Radha
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - M H Romanofsky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - M J Shoup
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| |
Collapse
|
32
|
Sutcliffe GD, Milanese LM, Orozco D, Lahmann B, Gatu Johnson M, Séguin FH, Sio H, Frenje JA, Li CK, Petrasso RD, Park HS, Rygg JR, Casey DT, Bionta R, Turnbull DP, Huntington CM, Ross JS, Zylstra AB, Rosenberg MJ, Glebov VY. A novel method to recover DD fusion proton CR-39 data corrupted by fast ablator ions at OMEGA and the National Ignition Facility. Rev Sci Instrum 2016; 87:11D812. [PMID: 27910586 DOI: 10.1063/1.4960072] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/06/2023]
Abstract
CR-39 detectors are used routinely in inertial confinement fusion (ICF) experiments as a part of nuclear diagnostics. CR-39 is filtered to stop fast ablator ions which have been accelerated from an ICF implosion due to electric fields caused by laser-plasma interactions. In some experiments, the filtering is insufficient to block these ions and the fusion-product signal tracks are lost in the large background of accelerated ion tracks. A technique for recovering signal in these scenarios has been developed, tested, and implemented successfully. The technique involves removing material from the surface of the CR-39 to a depth beyond the endpoint of the ablator ion tracks. The technique preserves signal magnitude (yield) as well as structure in radiograph images. The technique is effective when signal particle range is at least 10 μm deeper than the necessary bulk material removal.
Collapse
Affiliation(s)
- G D Sutcliffe
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - L M Milanese
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - D Orozco
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - B Lahmann
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H-S Park
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J R Rygg
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D T Casey
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R Bionta
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D P Turnbull
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C M Huntington
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J S Ross
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A B Zylstra
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - M J Rosenberg
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| |
Collapse
|
33
|
Gatu Johnson M, Knauer JP, Cerjan CJ, Eckart MJ, Grim GP, Hartouni EP, Hatarik R, Kilkenny JD, Munro DH, Sayre DB, Spears BK, Bionta RM, Bond EJ, Caggiano JA, Callahan D, Casey DT, Döppner T, Frenje JA, Glebov VY, Hurricane O, Kritcher A, LePape S, Ma T, Mackinnon A, Meezan N, Patel P, Petrasso RD, Ralph JE, Springer PT, Yeamans CB. Indications of flow near maximum compression in layered deuterium-tritium implosions at the National Ignition Facility. Phys Rev E 2016; 94:021202. [PMID: 27627237 DOI: 10.1103/physreve.94.021202] [Citation(s) in RCA: 13] [Impact Index Per Article: 1.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/24/2016] [Indexed: 06/06/2023]
Abstract
An accurate understanding of burn dynamics in implosions of cryogenically layered deuterium (D) and tritium (T) filled capsules, obtained partly through precision diagnosis of these experiments, is essential for assessing the impediments to achieving ignition at the National Ignition Facility. We present measurements of neutrons from such implosions. The apparent ion temperatures T_{ion} are inferred from the variance of the primary neutron spectrum. Consistently higher DT than DD T_{ion} are observed and the difference is seen to increase with increasing apparent DT T_{ion}. The line-of-sight rms variations of both DD and DT T_{ion} are small, ∼150eV, indicating an isotropic source. The DD neutron yields are consistently high relative to the DT neutron yields given the observed T_{ion}. Spatial and temporal variations of the DT temperature and density, DD-DT differential attenuation in the surrounding DT fuel, and fluid motion variations contribute to a DT T_{ion} greater than the DD T_{ion}, but are in a one-dimensional model insufficient to explain the data. We hypothesize that in a three-dimensional interpretation, these effects combined could explain the results.
Collapse
Affiliation(s)
- M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C J Cerjan
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M J Eckart
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G P Grim
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - E P Hartouni
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R Hatarik
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J D Kilkenny
- General Atomics, San Diego, California 92186, USA
| | - D H Munro
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D B Sayre
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B K Spears
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R M Bionta
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - E J Bond
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J A Caggiano
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D Callahan
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D T Casey
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - T Döppner
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - O Hurricane
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Kritcher
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S LePape
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - T Ma
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Mackinnon
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N Meezan
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - P Patel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J E Ralph
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - P T Springer
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C B Yeamans
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| |
Collapse
|
34
|
Regan SP, Goncharov VN, Igumenshchev IV, Sangster TC, Betti R, Bose A, Boehly TR, Bonino MJ, Campbell EM, Cao D, Collins TJB, Craxton RS, Davis AK, Delettrez JA, Edgell DH, Epstein R, Forrest CJ, Frenje JA, Froula DH, Gatu Johnson M, Glebov VY, Harding DR, Hohenberger M, Hu SX, Jacobs-Perkins D, Janezic R, Karasik M, Keck RL, Kelly JH, Kessler TJ, Knauer JP, Kosc TZ, Loucks SJ, Marozas JA, Marshall FJ, McCrory RL, McKenty PW. Publisher's Note: Demonstration of Fuel Hot-Spot Pressure in Excess of 50 Gbar for Direct-Drive, Layered Deuterium-Tritium Implosions on OMEGA [Phys. Rev. Lett. 117, 025001 (2016)]. Phys Rev Lett 2016; 117:059903. [PMID: 27517797 DOI: 10.1103/physrevlett.117.059903] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/20/2016] [Indexed: 06/06/2023]
Abstract
This corrects the article DOI: 10.1103/PhysRevLett.117.025001.
Collapse
|
35
|
Zylstra AB, Herrmann HW, Johnson MG, Kim YH, Frenje JA, Hale G, Li CK, Rubery M, Paris M, Bacher A, Brune CR, Forrest C, Glebov VY, Janezic R, McNabb D, Nikroo A, Pino J, Sangster TC, Séguin FH, Seka W, Sio H, Stoeckl C, Petrasso RD. Using Inertial Fusion Implosions to Measure the T+^{3}He Fusion Cross Section at Nucleosynthesis-Relevant Energies. Phys Rev Lett 2016; 117:035002. [PMID: 27472118 DOI: 10.1103/physrevlett.117.035002] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/13/2016] [Indexed: 06/06/2023]
Abstract
Light nuclei were created during big-bang nucleosynthesis (BBN). Standard BBN theory, using rates inferred from accelerator-beam data, cannot explain high levels of ^{6}Li in low-metallicity stars. Using high-energy-density plasmas we measure the T(^{3}He,γ)^{6}Li reaction rate, a candidate for anomalously high ^{6}Li production; we find that the rate is too low to explain the observations, and different than values used in common BBN models. This is the first data directly relevant to BBN, and also the first use of laboratory plasmas, at comparable conditions to astrophysical systems, to address a problem in nuclear astrophysics.
Collapse
Affiliation(s)
- A B Zylstra
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - H W Herrmann
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - Y H Kim
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - G Hale
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Rubery
- Plasma Physics Department, AWE plc, Reading RG7 4PR, United Kingdom
| | - M Paris
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A Bacher
- Indiana University, Bloomington, Indiana 47405, USA
| | - C R Brune
- Ohio University, Athens, Ohio 45701, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Janezic
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D McNabb
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Nikroo
- General Atomics, San Diego, California 92186, USA
| | - J Pino
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - W Seka
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - H Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| |
Collapse
|
36
|
Regan SP, Goncharov VN, Igumenshchev IV, Sangster TC, Betti R, Bose A, Boehly TR, Bonino MJ, Campbell EM, Cao D, Collins TJB, Craxton RS, Davis AK, Delettrez JA, Edgell DH, Epstein R, Forrest CJ, Frenje JA, Froula DH, Gatu Johnson M, Glebov VY, Harding DR, Hohenberger M, Hu SX, Jacobs-Perkins D, Janezic R, Karasik M, Keck RL, Kelly JH, Kessler TJ, Knauer JP, Kosc TZ, Loucks SJ, Marozas JA, Marshall FJ, McCrory RL, McKenty PW, Meyerhofer DD, Michel DT, Myatt JF, Obenschain SP, Petrasso RD, Radha PB, Rice B, Rosenberg MJ, Schmitt AJ, Schmitt MJ, Seka W, Shmayda WT, Shoup MJ, Shvydky A, Skupsky S, Solodov AA, Stoeckl C, Theobald W, Ulreich J, Wittman MD, Woo KM, Yaakobi B, Zuegel JD. Demonstration of Fuel Hot-Spot Pressure in Excess of 50 Gbar for Direct-Drive, Layered Deuterium-Tritium Implosions on OMEGA. Phys Rev Lett 2016; 117:025001. [PMID: 27447511 DOI: 10.1103/physrevlett.117.025001] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/07/2015] [Indexed: 06/06/2023]
Abstract
A record fuel hot-spot pressure P_{hs}=56±7 Gbar was inferred from x-ray and nuclear diagnostics for direct-drive inertial confinement fusion cryogenic, layered deuterium-tritium implosions on the 60-beam, 30-kJ, 351-nm OMEGA Laser System. When hydrodynamically scaled to the energy of the National Ignition Facility, these implosions achieved a Lawson parameter ∼60% of the value required for ignition [A. Bose et al., Phys. Rev. E 93, 011201(R) (2016)], similar to indirect-drive implosions [R. Betti et al., Phys. Rev. Lett. 114, 255003 (2015)], and nearly half of the direct-drive ignition-threshold pressure. Relative to symmetric, one-dimensional simulations, the inferred hot-spot pressure is approximately 40% lower. Three-dimensional simulations suggest that low-mode distortion of the hot spot seeded by laser-drive nonuniformity and target-positioning error reduces target performance.
Collapse
Affiliation(s)
- S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - I V Igumenshchev
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
| | - A Bose
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
| | - T R Boehly
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M J Bonino
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - E M Campbell
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D Cao
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T J B Collins
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R S Craxton
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A K Davis
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Delettrez
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D H Edgell
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Epstein
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Frenje
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - D H Froula
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D R Harding
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Hohenberger
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S X Hu
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D Jacobs-Perkins
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Janezic
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Karasik
- Naval Research Laboratory, Washington, D.C. 20375, USA
| | - R L Keck
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J H Kelly
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T J Kessler
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T Z Kosc
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S J Loucks
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Marozas
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - F J Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R L McCrory
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - P W McKenty
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D D Meyerhofer
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - D T Michel
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J F Myatt
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | | | - R D Petrasso
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - P B Radha
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - B Rice
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M J Rosenberg
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A J Schmitt
- Naval Research Laboratory, Washington, D.C. 20375, USA
| | - M J Schmitt
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - W Seka
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W T Shmayda
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M J Shoup
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A Shvydky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S Skupsky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - A A Solodov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J Ulreich
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M D Wittman
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - K M Woo
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
| | - B Yaakobi
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J D Zuegel
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
37
|
Bose A, Woo KM, Betti R, Campbell EM, Mangino D, Christopherson AR, McCrory RL, Nora R, Regan SP, Goncharov VN, Sangster TC, Forrest CJ, Frenje J, Gatu Johnson M, Glebov VY, Knauer JP, Marshall FJ, Stoeckl C, Theobald W. Core conditions for alpha heating attained in direct-drive inertial confinement fusion. Phys Rev E 2016; 94:011201. [PMID: 27575069 DOI: 10.1103/physreve.94.011201] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/16/2015] [Indexed: 06/06/2023]
Abstract
It is shown that direct-drive implosions on the OMEGA laser have achieved core conditions that would lead to significant alpha heating at incident energies available on the National Ignition Facility (NIF) scale. The extrapolation of the experimental results from OMEGA to NIF energy assumes only that the implosion hydrodynamic efficiency is unchanged at higher energies. This approach is independent of the uncertainties in the physical mechanism that degrade implosions on OMEGA, and relies solely on a volumetric scaling of the experimentally observed core conditions. It is estimated that the current best-performing OMEGA implosion [Regan et al., Phys. Rev. Lett. 117, 025001 (2016)10.1103/PhysRevLett.117.025001] extrapolated to a 1.9 MJ laser driver with the same illumination configuration and laser-target coupling would produce 125 kJ of fusion energy with similar levels of alpha heating observed in current highest performing indirect-drive NIF implosions.
Collapse
Affiliation(s)
- A Bose
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - K M Woo
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - R Betti
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - E M Campbell
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - D Mangino
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - A R Christopherson
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - R L McCrory
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - R Nora
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - J Frenje
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Massachusetts Institute of Technology, Plasma Science and Fusion Center, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - J P Knauer
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - F J Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| | - W Theobald
- Fusion Science Center, University of Rochester, Rochester, New York 14623, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester New York 14623, USA
| |
Collapse
|
38
|
Hahn KD, Chandler GA, Ruiz CL, Cooper GW, Gomez MR, Slutz S, Sefkow AB, Sinars DB, Hansen SB, Knapp PF, Schmit PF, Harding E, Jennings CA, Awe TJ, Geissel M, Rovang DC, Torres JA, Bur JA, Cuneo ME, Glebov VY, Harvey-Thompson AJ, Herrman MC, Hess MH, Johns O, Jones B, Lamppa DC, Lash JS, Martin MR, McBride RD, Peterson KJ, Porter JL, Reneker J, Robertson GK, Rochau GA, Savage ME, Smith IC, Styron JD, Vesey RA. Fusion-neutron measurements for magnetized liner inertial fusion experiments on the Z accelerator. ACTA ACUST UNITED AC 2016. [DOI: 10.1088/1742-6596/717/1/012020] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
|
39
|
Stoeckl C, Boni R, Ehrne F, Forrest CJ, Glebov VY, Katz J, Lonobile DJ, Magoon J, Regan SP, Shoup MJ, Sorce A, Sorce C, Sangster TC, Weiner D. Neutron temporal diagnostic for high-yield deuterium-tritium cryogenic implosions on OMEGA. Rev Sci Instrum 2016; 87:053501. [PMID: 27250417 DOI: 10.1063/1.4948293] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/07/2016] [Accepted: 04/15/2016] [Indexed: 06/05/2023]
Abstract
A next-generation neutron temporal diagnostic (NTD) capable of recording high-quality data for the highest anticipated yield cryogenic deuterium-tritium (DT) implosion experiments was recently installed at the Omega Laser Facility. A high-quality measurement of the neutron production width is required to determine the hot-spot pressure achieved in inertial confinement fusion experiments-a key metric in assessing the quality of these implosions. The design of this NTD is based on a fast-rise-time plastic scintillator, which converts the neutron kinetic energy to 350- to 450-nm-wavelength light. The light from the scintillator inside the nose-cone assembly is relayed ∼16 m to a streak camera in a well-shielded location. An ∼200× reduction in neutron background was observed during the first high-yield DT cryogenic implosions compared to the current NTD installation on OMEGA. An impulse response of ∼40 ± 10 ps was measured in a dedicated experiment using hard x-rays from a planar target irradiated with a 10-ps short pulse from the OMEGA EP laser. The measured instrument response includes contributions from the scintillator rise time, optical relay, and streak camera.
Collapse
Affiliation(s)
- C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - R Boni
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - F Ehrne
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - J Katz
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - D J Lonobile
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - J Magoon
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - M J Shoup
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - A Sorce
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - C Sorce
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| | - D Weiner
- Laboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623-1299, USA
| |
Collapse
|
40
|
Simpson R, Danly C, Glebov VY, Hurlbut C, Merrill FE, Volegov PL, Wilde C. Solid polystyrene and deuterated polystyrene light output response to fast neutrons. Rev Sci Instrum 2016; 87:043513. [PMID: 27131680 DOI: 10.1063/1.4947515] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/05/2023]
Abstract
The Neutron Imaging System has proven to be an important diagnostic in studying DT implosion characteristics at the National Ignition Facility. The current system depends on a polystyrene scintillating fiber array, which detects fusion neutrons born in the DT hotspot as well as neutrons that have scattered to lower energies in the surrounding cold fuel. Increasing neutron yields at NIF, as well as a desire to resolve three-dimensional information about the fuel assembly, have provided the impetus to build and install two additional next-generation neutron imaging systems. We are currently investigating a novel neutron imaging system that will utilize a deuterated polystyrene (CD) fiber array instead of standard hydrogen-based polystyrene (CH). Studies of deuterated xylene or deuterated benzene liquid scintillator show an improvement in imaging resolution by a factor of two [L. Disdier et al., Rev. Sci. Instrum. 75, 2134 (2004)], but also a reduction in light output [V. Bildstein et al., Nucl. Instrum. Methods Phys. Res., Sect. A 729, 188 (2013); M. I. Ojaruega, Ph.D. thesis, University of Michigan, 2009; M. T. Febbraro, Ph.D. thesis, University of Michigan, 2014] as compared to standard plastic. Tests of the relative light output of deuterated polystyrene and standard polystyrene were completed using 14 MeV fusion neutrons generated through implosions of deuterium-tritium filled capsules at the OMEGA laser facility. In addition, we collected data of the relative response of these two scintillators to a wide energy range of neutrons (1-800 MeV) at the Weapons Neutrons Research Facility. Results of these measurements are presented.
Collapse
Affiliation(s)
- R Simpson
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - C Danly
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - C Hurlbut
- Eljen Technology, Sweetwater, Texas 79556, USA
| | - F E Merrill
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - P L Volegov
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - C Wilde
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| |
Collapse
|
41
|
Kilkenny JD, Caggiano JA, Hatarik R, Knauer JP, Sayre DB, Spears BK, Weber SV, Yeamans CB, Cerjan CJ, Divol L, Eckart MJ, Glebov VY, Herrmann HW, Pape SL, Munro DH, Grim GP, Jones OS, Berzak-Hopkins L, Gatu-Johnson M, Mackinnon AJ, Meezan NB, Casey DT, Frenje JA, Mcnaney JM, Petrasso R, Rinderknecht H, Stoeffl W, Zylstra AB. Understanding the stagnation and burn of implosions on NIF. ACTA ACUST UNITED AC 2016. [DOI: 10.1088/1742-6596/688/1/012048] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
|
42
|
Frenje JA, Grabowski PE, Li CK, Séguin FH, Zylstra AB, Gatu Johnson M, Petrasso RD, Glebov VY, Sangster TC. Measurements of Ion Stopping Around the Bragg Peak in High-Energy-Density Plasmas. Phys Rev Lett 2015; 115:205001. [PMID: 26613448 DOI: 10.1103/physrevlett.115.205001] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/14/2015] [Indexed: 06/05/2023]
Abstract
For the first time, quantitative measurements of ion stopping at energies around the Bragg peak (or peak ion stopping, which occurs at an ion velocity comparable to the average thermal electron velocity), and its dependence on electron temperature (T(e)) and electron number density (n(e)) in the range of 0.5-4.0 keV and 3×10(22) to 3×10(23) cm(-3) have been conducted, respectively. It is experimentally demonstrated that the position and amplitude of the Bragg peak varies strongly with T(e) with n(e). The importance of including quantum diffraction is also demonstrated in the stopping-power modeling of high-energy-density plasmas.
Collapse
Affiliation(s)
- J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P E Grabowski
- Department of Chemistry, University of California Irvine, Irvine, California 92697, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - A B Zylstra
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
43
|
Casey DT, Woods DT, Smalyuk VA, Hurricane OA, Glebov VY, Stoeckl C, Theobald W, Wallace R, Nikroo A, Schoff M, Shuldberg C, Wu KJ, Frenje JA, Landen OL, Remington BA, Glendinning G. Performance and Mix Measurements of Indirect Drive Cu-Doped Be Implosions. Phys Rev Lett 2015; 114:205002. [PMID: 26047234 DOI: 10.1103/physrevlett.114.205002] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/22/2014] [Indexed: 06/04/2023]
Abstract
The ablator couples energy between the driver and fusion fuel in inertial confinement fusion (ICF). Because of its low opacity, high solid density, and material properties, beryllium has long been considered an ideal ablator for ICF ignition experiments at the National Ignition Facility. We report here the first indirect drive Be implosions driven with shaped laser pulses and diagnosed with fusion yield at the OMEGA laser. The results show good performance with an average DD neutron yield of ∼2×10^{9} at a convergence ratio of R_{0}/R∼10 and little impact due to the growth of hydrodynamic instabilities and mix. In addition, the effect of adding an inner liner of W between the Be and DD is demonstrated.
Collapse
Affiliation(s)
- D T Casey
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D T Woods
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - V A Smalyuk
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - O A Hurricane
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - V Y Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W Theobald
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Wallace
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Nikroo
- General Atomics, San Diego, California 92121, USA
| | - M Schoff
- General Atomics, San Diego, California 92121, USA
| | - C Shuldberg
- General Atomics, San Diego, California 92121, USA
| | - K J Wu
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J A Frenje
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - O L Landen
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B A Remington
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G Glendinning
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| |
Collapse
|
44
|
Waugh CJ, Rosenberg MJ, Zylstra AB, Frenje JA, Séguin FH, Petrasso RD, Glebov VY, Sangster TC, Stoeckl C. A method for in situ absolute DD yield calibration of neutron time-of-flight detectors on OMEGA using CR-39-based proton detectors. Rev Sci Instrum 2015; 86:053506. [PMID: 26026524 DOI: 10.1063/1.4919290] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/04/2023]
Abstract
Neutron time of flight (nTOF) detectors are used routinely to measure the absolute DD neutron yield at OMEGA. To check the DD yield calibration of these detectors, originally calibrated using indium activation systems, which in turn were cross-calibrated to NOVA nTOF detectors in the early 1990s, a direct in situ calibration method using CR-39 range filter proton detectors has been successfully developed. By measuring DD neutron and proton yields from a series of exploding pusher implosions at OMEGA, a yield calibration coefficient of 1.09 ± 0.02 (relative to the previous coefficient) was determined for the 3m nTOF detector. In addition, comparison of these and other shots indicates that significant reduction in charged particle flux anisotropies is achieved when bang time occurs significantly (on the order of 500 ps) after the trailing edge of the laser pulse. This is an important observation as the main source of the yield calibration error is due to particle anisotropies caused by field effects. The results indicate that the CR-39-nTOF in situ calibration method can serve as a valuable technique for calibrating and reducing the uncertainty in the DD absolute yield calibration of nTOF detector systems on OMEGA, the National Ignition Facility, and laser megajoule.
Collapse
Affiliation(s)
- C J Waugh
- Plasma Science and Fusion Center, MIT, Cambridge, Massachusetts 02139, USA
| | - M J Rosenberg
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - A B Zylstra
- Plasma Science and Fusion Center, MIT, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Plasma Science and Fusion Center, MIT, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, MIT, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, MIT, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| |
Collapse
|
45
|
Rinderknecht HG, Rosenberg MJ, Li CK, Hoffman NM, Kagan G, Zylstra AB, Sio H, Frenje JA, Gatu Johnson M, Séguin FH, Petrasso RD, Amendt P, Bellei C, Wilks S, Delettrez J, Glebov VY, Stoeckl C, Sangster TC, Meyerhofer DD, Nikroo A. Ion thermal decoupling and species separation in shock-driven implosions. Phys Rev Lett 2015; 114:025001. [PMID: 25635549 DOI: 10.1103/physrevlett.114.025001] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/19/2014] [Indexed: 06/04/2023]
Abstract
Anomalous reduction of the fusion yields by 50% and anomalous scaling of the burn-averaged ion temperatures with the ion-species fraction has been observed for the first time in D^{3}He-filled shock-driven inertial confinement fusion implosions. Two ion kinetic mechanisms are used to explain the anomalous observations: thermal decoupling of the D and ^{3}He populations and diffusive species separation. The observed insensitivity of ion temperature to a varying deuterium fraction is shown to be a signature of ion thermal decoupling in shock-heated plasmas. The burn-averaged deuterium fraction calculated from the experimental data demonstrates a reduction in the average core deuterium density, as predicted by simulations that use a diffusion model. Accounting for each of these effects in simulations reproduces the observed yield trends.
Collapse
Affiliation(s)
- Hans G Rinderknecht
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M J Rosenberg
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - N M Hoffman
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - G Kagan
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A B Zylstra
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H Sio
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P Amendt
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Bellei
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S Wilks
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Delettrez
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - D D Meyerhofer
- Laboratory for Laser Energetics, Rochester, New York 14623, USA
| | - A Nikroo
- General Atomics, San Diego, California 92121, USA
| |
Collapse
|
46
|
Glebov VY, Forrest CJ, Marshall KL, Romanofsky M, Sangster TC, Shoup MJ, Stoeckl C. A new neutron time-of-flight detector for fuel-areal-density measurements on OMEGA. Rev Sci Instrum 2014; 85:11E102. [PMID: 25430281 DOI: 10.1063/1.4886428] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/04/2023]
Abstract
A new neutron time-of-flight (nTOF) detector for fuel-areal-density measurements in cryogenic DT implosions was installed on the OMEGA Laser System. The nTOF detector has a cylindrical thin-wall, stainless-steel, 8-in.-diam, 4-in.-thick cavity filled with an oxygenated liquid xylene scintillator. Four gated photomultiplier tubes (PMTs) with different gains are used to measure primary DT and D2 neutrons, down-scattered neutrons in nT and nD kinematic edge regions, and to study tertiary neutrons in the same detector. The nTOF detector is located 13.4 m from target chamber center in a well-collimated line of sight. The design details of the nTOF detector, PMT optimization, and test results on OMEGA will be presented.
Collapse
Affiliation(s)
- V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - K L Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Romanofsky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M J Shoup
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
47
|
Rosenberg MJ, Zylstra AB, Frenje JA, Rinderknecht HG, Johnson MG, Waugh CJ, Séguin FH, Sio H, Sinenian N, Li CK, Petrasso RD, Glebov VY, Hohenberger M, Stoeckl C, Sangster TC, Yeamans CB, LePape S, Mackinnon AJ, Bionta RM, Talison B, Casey DT, Landen OL, Moran MJ, Zacharias RA, Kilkenny JD, Nikroo A. A compact proton spectrometer for measurement of the absolute DD proton spectrum from which yield and ρR are determined in thin-shell inertial-confinement-fusion implosions. Rev Sci Instrum 2014; 85:103504. [PMID: 25362390 DOI: 10.1063/1.4897193] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/05/2014] [Accepted: 09/22/2014] [Indexed: 06/04/2023]
Abstract
A compact, step range filter proton spectrometer has been developed for the measurement of the absolute DD proton spectrum, from which yield and areal density (ρR) are inferred for deuterium-filled thin-shell inertial confinement fusion implosions. This spectrometer, which is based on tantalum step-range filters, is sensitive to protons in the energy range 1-9 MeV and can be used to measure proton spectra at mean energies of ∼1-3 MeV. It has been developed and implemented using a linear accelerator and applied to experiments at the OMEGA laser facility and the National Ignition Facility (NIF). Modeling of the proton slowing in the filters is necessary to construct the spectrum, and the yield and energy uncertainties are ±<10% in yield and ±120 keV, respectively. This spectrometer can be used for in situ calibration of DD-neutron yield diagnostics at the NIF.
Collapse
Affiliation(s)
- M J Rosenberg
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - A B Zylstra
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H G Rinderknecht
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C J Waugh
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - N Sinenian
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - M Hohenberger
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C B Yeamans
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S LePape
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A J Mackinnon
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R M Bionta
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B Talison
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D T Casey
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - O L Landen
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M J Moran
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R A Zacharias
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J D Kilkenny
- General Atomics, San Diego, California 92186, USA
| | - A Nikroo
- General Atomics, San Diego, California 92186, USA
| |
Collapse
|
48
|
Zylstra AB, Gatu Johnson M, Frenje JA, Séguin FH, Rinderknecht HG, Rosenberg MJ, Sio HW, Li CK, Petrasso RD, McCluskey M, Mastrosimone D, Glebov VY, Forrest C, Stoeckl C, Sangster TC. A compact neutron spectrometer for characterizing inertial confinement fusion implosions at OMEGA and the NIF. Rev Sci Instrum 2014; 85:063502. [PMID: 24985814 DOI: 10.1063/1.4880203] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/03/2023]
Abstract
A compact spectrometer for measurements of the primary deuterium-tritium neutron spectrum has been designed and implemented on the OMEGA laser facility [T. Boehly et al., Opt. Commun. 133, 495 (1997)]. This instrument uses the recoil spectrometry technique, where neutrons produced in an implosion elastically scatter protons in a plastic foil, which are subsequently detected by a proton spectrometer. This diagnostic is currently capable of measuring the yield to ~±10% accuracy, and mean neutron energy to ~±50 keV precision. As these compact spectrometers can be readily placed at several locations around an implosion, effects of residual fuel bulk flows during burn can be measured. Future improvements to reduce the neutron energy uncertainty to ±15-20 keV are discussed, which will enable measurements of fuel velocities to an accuracy of ~±25-40 km/s.
Collapse
Affiliation(s)
- A B Zylstra
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H G Rinderknecht
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M J Rosenberg
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H W Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M McCluskey
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D Mastrosimone
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| |
Collapse
|
49
|
Rosenberg MJ, Rinderknecht HG, Hoffman NM, Amendt PA, Atzeni S, Zylstra AB, Li CK, Séguin FH, Sio H, Johnson MG, Frenje JA, Petrasso RD, Glebov VY, Stoeckl C, Seka W, Marshall FJ, Delettrez JA, Sangster TC, Betti R, Goncharov VN, Meyerhofer DD, Skupsky S, Bellei C, Pino J, Wilks SC, Kagan G, Molvig K, Nikroo A. Exploration of the transition from the hydrodynamiclike to the strongly kinetic regime in shock-driven implosions. Phys Rev Lett 2014; 112:185001. [PMID: 24856701 DOI: 10.1103/physrevlett.112.185001] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/01/2013] [Indexed: 06/03/2023]
Abstract
Clear evidence of the transition from hydrodynamiclike to strongly kinetic shock-driven implosions is, for the first time, revealed and quantitatively assessed. Implosions with a range of initial equimolar D3He gas densities show that as the density is decreased, hydrodynamic simulations strongly diverge from and increasingly overpredict the observed nuclear yields, from a factor of ∼2 at 3.1 mg/cm3 to a factor of 100 at 0.14 mg/cm3. (The corresponding Knudsen number, the ratio of ion mean-free path to minimum shell radius, varied from 0.3 to 9; similarly, the ratio of fusion burn duration to ion diffusion time, another figure of merit of kinetic effects, varied from 0.3 to 14.) This result is shown to be unrelated to the effects of hydrodynamic mix. As a first step to garner insight into this transition, a reduced ion kinetic (RIK) model that includes gradient-diffusion and loss-term approximations to several transport processes was implemented within the framework of a one-dimensional radiation-transport code. After empirical calibration, the RIK simulations reproduce the observed yield trends, largely as a result of ion diffusion and the depletion of the reacting tail ions.
Collapse
Affiliation(s)
- M J Rosenberg
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H G Rinderknecht
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - N M Hoffman
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - P A Amendt
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S Atzeni
- Dipartimento SBAI, Università di Roma "La Sapienza", Via A Scarpa, 14-16, I-00161 Roma, Italy
| | - A B Zylstra
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - W Seka
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - F J Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - J A Delettrez
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V N Goncharov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D D Meyerhofer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S Skupsky
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Bellei
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Pino
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S C Wilks
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G Kagan
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - K Molvig
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A Nikroo
- General Atomics, San Diego, California 92186, USA
| |
Collapse
|
50
|
Rinderknecht HG, Sio H, Li CK, Zylstra AB, Rosenberg MJ, Amendt P, Delettrez J, Bellei C, Frenje JA, Gatu Johnson M, Séguin FH, Petrasso RD, Betti R, Glebov VY, Meyerhofer DD, Sangster TC, Stoeckl C, Landen O, Smalyuk VA, Wilks S, Greenwood A, Nikroo A. First observations of nonhydrodynamic mix at the fuel-shell interface in shock-driven inertial confinement implosions. Phys Rev Lett 2014; 112:135001. [PMID: 24745431 DOI: 10.1103/physrevlett.112.135001] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/06/2013] [Indexed: 06/03/2023]
Abstract
A strong nonhydrodynamic mechanism generating atomic fuel-shell mix has been observed in strongly shocked inertial confinement fusion implosions of thin deuterated-plastic shells filled with 3He gas. These implosions were found to produce D3He-proton shock yields comparable to implosions of identical shells filled with a hydroequivalent 50∶50 D3He gas mixture. Standard hydrodynamic mixing cannot explain this observation, as hydrodynamic modeling including mix predicts a yield an order of magnitude lower than was observed. Instead, these results can be attributed to ion diffusive mix at the fuel-shell interface.
Collapse
Affiliation(s)
- H G Rinderknecht
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - H Sio
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C K Li
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - A B Zylstra
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M J Rosenberg
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P Amendt
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Delettrez
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Bellei
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J A Frenje
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - M Gatu Johnson
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - F H Séguin
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R D Petrasso
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - R Betti
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - D D Meyerhofer
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - T C Sangster
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - O Landen
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - V A Smalyuk
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S Wilks
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Greenwood
- General Atomics, San Diego, California 92121, USA
| | - A Nikroo
- General Atomics, San Diego, California 92121, USA
| |
Collapse
|