1
|
Maltezopoulos T, Brinker F, Dietrich F, Freund W, Grünert J, Jastrow UF, Kujala N, Laksman J, Liu J, Tiedtke K, Tschentscher T. Hard X-ray operation of X-ray gas monitors at the European XFEL. JOURNAL OF SYNCHROTRON RADIATION 2024; 31:681-689. [PMID: 38838164 PMCID: PMC11226157 DOI: 10.1107/s160057752400331x] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/20/2024] [Accepted: 04/16/2024] [Indexed: 06/07/2024]
Abstract
X-ray gas monitors (XGMs) are operated at the European XFEL for non-invasive single-shot pulse energy measurements and average beam-position monitoring. The underlying measurement principle is the photo-ionization of rare gas atoms at low gas pressures and the detection of the photo-ions and photo-electrons created. These are essential for tuning and sustaining self-amplified spontaneous emission (SASE) operation, machine radiation safety, and sorting single-shot experimental data according to pulse energy. In this paper, the first results from XGM operation at photon energies up to 30 keV are presented, which are far beyond the original specification of this device. Here, the Huge Aperture MultiPlier (HAMP) is used for single-shot pulse energy measurements since the standard X-ray gas monitor detectors (XGMDs) do not provide a sufficient signal-to-noise ratio, even at the highest operating gas pressures. A single-shot correlation coefficient of 0.98 is measured between consecutive XGMs operated with HAMP, which is as good as measuring with the standard XGMD detectors. An intra-train non-linearity of the HAMP signal is discovered, and operation parameters to mitigate this effect are studied. The upper repetition rate limit of HAMP operation at 2.25 MHz is also determined. Finally, the possibilities and limits for future XGM operation at photon energies up to 50 keV are discussed.
Collapse
Affiliation(s)
| | - Frank Brinker
- Deutsches Elektronen-Synchrotron DESYNotkestrasse 8522607HamburgGermany
| | | | | | - Jan Grünert
- European XFELHolzkoppel 422869SchenefeldGermany
| | - Ulf Fini Jastrow
- Deutsches Elektronen-Synchrotron DESYNotkestrasse 8522607HamburgGermany
| | | | | | - Jia Liu
- European XFELHolzkoppel 422869SchenefeldGermany
| | - Kai Tiedtke
- Deutsches Elektronen-Synchrotron DESYNotkestrasse 8522607HamburgGermany
| | | |
Collapse
|
2
|
Bohon J, Gonzalez E, Grace C, Harris CT, Jacobsen B, Kachiguine S, Kim D, MacArthur J, Martinez-McKinney F, Mazza S, Nizam M, Norvell N, Padilla R, Potter E, Prakash T, Prebys E, Ryan E, Schumm BA, Smedley J, Stuart D, Tarka M, Torrecilla IS, Wilder M, Zhu D. Use of diamond sensors for a high-flux, high-rate X-ray pass-through diagnostic. JOURNAL OF SYNCHROTRON RADIATION 2022; 29:595-601. [PMID: 35510992 PMCID: PMC9070720 DOI: 10.1107/s1600577522003022] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 12/18/2021] [Accepted: 03/19/2022] [Indexed: 06/14/2023]
Abstract
X-ray free-electron lasers (XFELs) deliver pulses of coherent X-rays on the femtosecond time scale, with potentially high repetition rates. While XFELs provide high peak intensities, both the intensity and the centroid of the beam fluctuate strongly on a pulse-to-pulse basis, motivating high-rate beam diagnostics that operate over a large dynamic range. The fast drift velocity, low X-ray absorption and high radiation tolerance properties of chemical vapour deposition diamonds make these crystals a promising candidate material for developing a fast (multi-GHz) pass-through diagnostic for the next generation of XFELs. A new approach to the design of a diamond sensor signal path is presented, along with associated characterization studies performed in the XPP endstation of the LINAC Coherent Light Source (LCLS) at SLAC. Qualitative charge collection profiles (collected charge versus time) are presented and compared with those from a commercially available detector. Quantitative results on the charge collection efficiency and signal collection times are presented over a range of approximately four orders of magnitude in the generated electron-hole plasma density.
Collapse
Affiliation(s)
- J. Bohon
- Los Alamos National Laboratory, Los Alamos, NM 87545, USA
| | - E. Gonzalez
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - C. Grace
- Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
| | - C. T. Harris
- Sandia National Laboratories, Albuquerque, NM 87123, USA
| | - B. Jacobsen
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - S. Kachiguine
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - D. Kim
- Los Alamos National Laboratory, Los Alamos, NM 87545, USA
| | - J. MacArthur
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - F. Martinez-McKinney
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - S. Mazza
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - M. Nizam
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - N. Norvell
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - R. Padilla
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - E. Potter
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - T. Prakash
- Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
| | - E. Prebys
- University of California, Davis, CA 95616, USA
| | - E. Ryan
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - B. A. Schumm
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - J. Smedley
- Los Alamos National Laboratory, Los Alamos, NM 87545, USA
| | - D. Stuart
- University of California, Santa Barbara, CA 93106, USA
| | - M. Tarka
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | | | - M. Wilder
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - D. Zhu
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| |
Collapse
|
3
|
Sorokin AA, Bican Y, Bonfigt S, Brachmanski M, Braune M, Jastrow UF, Gottwald A, Kaser H, Richter M, Tiedtke K. An X-ray gas monitor for free-electron lasers. JOURNAL OF SYNCHROTRON RADIATION 2019; 26:1092-1100. [PMID: 31274432 PMCID: PMC6613123 DOI: 10.1107/s1600577519005174] [Citation(s) in RCA: 21] [Impact Index Per Article: 4.2] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/21/2019] [Accepted: 04/15/2019] [Indexed: 05/06/2023]
Abstract
A novel X-ray gas monitor (XGM) has been developed which allows the measurement of absolute photon pulse energy and photon beam position at all existing and upcoming free-electron lasers (FELs) over a broad spectral range covering vacuum ultraviolet (VUV), extreme ultraviolet (EUV) and soft and hard X-rays. The XGM covers a wide dynamic range from spontaneous undulator radiation to FEL radiation and provides a temporal resolution of better than 200 ns. The XGM consists of two X-ray gas-monitor detectors (XGMDs) and two huge-aperture open electron multipliers (HAMPs). The HAMP enhances the detection efficiency of the XGM for low-intensity radiation down to 105 photons per pulse and for FEL radiation in the hard X-ray spectral range, while the XGMD operates in higher-intensity regimes. The relative standard uncertainty for measurements of the absolute photon pulse energy is well below 10%, and down to 1% for measurements of relative pulse-to-pulse intensity on pulses with more than 1010 photons per pulse. The accuracy of beam-position monitoring in the vertical and horizontal directions is of the order of 10 µm.
Collapse
Affiliation(s)
- Andrey A. Sorokin
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
- Ioffe Physico-Technical Institute, Polytekhnicheskaya 26, 194021 St Petersburg, Russian Federation
| | - Yilmaz Bican
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
| | - Susanne Bonfigt
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
| | - Maciej Brachmanski
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
| | - Markus Braune
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
| | - Ulf Fini Jastrow
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
| | - Alexander Gottwald
- Physikalisch-Technische Bundesanstalt (PTB), Abbestrasse 2–12, D-10587 Berlin, Germany
| | - Hendrik Kaser
- Physikalisch-Technische Bundesanstalt (PTB), Abbestrasse 2–12, D-10587 Berlin, Germany
| | - Mathias Richter
- Physikalisch-Technische Bundesanstalt (PTB), Abbestrasse 2–12, D-10587 Berlin, Germany
| | - Kai Tiedtke
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607 Hamburg, Germany
| |
Collapse
|
4
|
Maltezopoulos T, Dietrich F, Freund W, Jastrow UF, Koch A, Laksman J, Liu J, Planas M, Sorokin AA, Tiedtke K, Grünert J. Operation of X-ray gas monitors at the European XFEL. JOURNAL OF SYNCHROTRON RADIATION 2019; 26:1045-1051. [PMID: 31274426 DOI: 10.1107/s1600577519003795] [Citation(s) in RCA: 20] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/04/2019] [Accepted: 03/19/2019] [Indexed: 06/09/2023]
Abstract
X-ray gas monitors (XGMs) are operated at the European XFEL for non-invasive single-shot pulse energy measurements and average beam position monitoring. They are used for tuning and maintaining the self-amplified spontaneous emission (SASE) operation and for sorting single-shot experimental data according to the pulse-resolved energy monitor data. The XGMs were developed at DESY based on the specific requirements for the European XFEL. In total, six XGM units are continuously in operation. Here, the main principle and experimental setup of an XGM are summarized, and the locations of the six XGMs at the facility are shown. Pulse energy measurements at 0.134 nm wavelength are presented, exceeding 1 mJ obtained with an absolute measurement uncertainty of 7-10%; correlations between different XGMs are shown, from which a SASE1 beamline transmission of 97% is deduced. Additionally, simultaneous position measurements close to the undulator and at the end of the tunnel are shown, along with the correlation of beam position data simultaneously acquired by an XGM and an imager.
Collapse
Affiliation(s)
| | - Florian Dietrich
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Wolfgang Freund
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Ulf Fini Jastrow
- FS-FLASH-D, Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Andreas Koch
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Joakim Laksman
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Jia Liu
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Marc Planas
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Andrey A Sorokin
- FS-FLASH-D, Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Kai Tiedtke
- FS-FLASH-D, Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Jan Grünert
- X-ray Photon Diagnostics Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| |
Collapse
|