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Doriese WB, Abbamonte P, Alpert BK, Bennett DA, Denison EV, Fang Y, Fischer DA, Fitzgerald CP, Fowler JW, Gard JD, Hays-Wehle JP, Hilton GC, Jaye C, McChesney JL, Miaja-Avila L, Morgan KM, Joe YI, O'Neil GC, Reintsema CD, Rodolakis F, Schmidt DR, Tatsuno H, Uhlig J, Vale LR, Ullom JN, Swetz DS. A practical superconducting-microcalorimeter X-ray spectrometer for beamline and laboratory science. Rev Sci Instrum 2017; 88:053108. [PMID: 28571411 DOI: 10.1063/1.4983316] [Citation(s) in RCA: 17] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/20/2023]
Abstract
We describe a series of microcalorimeter X-ray spectrometers designed for a broad suite of measurement applications. The chief advantage of this type of spectrometer is that it can be orders of magnitude more efficient at collecting X-rays than more traditional high-resolution spectrometers that rely on wavelength-dispersive techniques. This advantage is most useful in applications that are traditionally photon-starved and/or involve radiation-sensitive samples. Each energy-dispersive spectrometer is built around an array of several hundred transition-edge sensors (TESs). TESs are superconducting thin films that are biased into their superconducting-to-normal-metal transitions. The spectrometers share a common readout architecture and many design elements, such as a compact, 65 mK detector package, 8-column time-division-multiplexed superconducting quantum-interference device readout, and a liquid-cryogen-free cryogenic system that is a two-stage adiabatic-demagnetization refrigerator backed by a pulse-tube cryocooler. We have adapted this flexible architecture to mate to a variety of sample chambers and measurement systems that encompass a range of observing geometries. There are two different types of TES pixels employed. The first, designed for X-ray energies below 10 keV, has a best demonstrated energy resolution of 2.1 eV (full-width-at-half-maximum or FWHM) at 5.9 keV. The second, designed for X-ray energies below 2 keV, has a best demonstrated resolution of 1.0 eV (FWHM) at 500 eV. Our team has now deployed seven of these X-ray spectrometers to a variety of light sources, accelerator facilities, and laboratory-scale experiments; these seven spectrometers have already performed measurements related to their applications. Another five of these spectrometers will come online in the near future. We have applied our TES spectrometers to the following measurement applications: synchrotron-based absorption and emission spectroscopy and energy-resolved scattering; accelerator-based spectroscopy of hadronic atoms and particle-induced-emission spectroscopy; laboratory-based time-resolved absorption and emission spectroscopy with a tabletop, broadband source; and laboratory-based metrology of X-ray-emission lines. Here, we discuss the design, construction, and operation of our TES spectrometers and show first-light measurements from the various systems. Finally, because X-ray-TES technology continues to mature, we discuss improvements to array size, energy resolution, and counting speed that we anticipate in our next generation of TES-X-ray spectrometers and beyond.
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Affiliation(s)
- W B Doriese
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - P Abbamonte
- Department of Physics, University of Illinois, Urbana, Illinois 61801, USA
| | - B K Alpert
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - D A Bennett
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - E V Denison
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - Y Fang
- Department of Physics, University of Illinois, Urbana, Illinois 61801, USA
| | - D A Fischer
- National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA
| | - C P Fitzgerald
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - J W Fowler
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - J D Gard
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - J P Hays-Wehle
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - G C Hilton
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - C Jaye
- National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA
| | - J L McChesney
- Argonne National Laboratory, Advanced Photon Source, Argonne, Illinois 60439, USA
| | - L Miaja-Avila
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - K M Morgan
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - Y I Joe
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - G C O'Neil
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - C D Reintsema
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - F Rodolakis
- Argonne National Laboratory, Advanced Photon Source, Argonne, Illinois 60439, USA
| | - D R Schmidt
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - H Tatsuno
- Department of Chemical Physics, Lund University, Lund, Sweden
| | - J Uhlig
- Department of Chemical Physics, Lund University, Lund, Sweden
| | - L R Vale
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - J N Ullom
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
| | - D S Swetz
- National Institute of Standards and Technology, Boulder, Colorado 80305, USA
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Lupi S, Baldassarre L, Mansart B, Perucchi A, Barinov A, Dudin P, Papalazarou E, Rodolakis F, Rueff JP, Itié JP, Ravy S, Nicoletti D, Postorino P, Hansmann P, Parragh N, Toschi A, Saha-Dasgupta T, Andersen OK, Sangiovanni G, Held K, Marsi M. Erratum: A microscopic view on the Mott transition in chromium-doped V2O3. Nat Commun 2012. [DOI: 10.1038/ncomms1397] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/09/2022] Open
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Lupi S, Baldassarre L, Mansart B, Perucchi A, Barinov A, Dudin P, Papalazarou E, Rodolakis F, Rueff JP, Itié JP, Ravy S, Nicoletti D, Postorino P, Hansmann P, Parragh N, Toschi A, Saha-Dasgupta T, Andersen OK, Sangiovanni G, Held K, Marsi M. A microscopic view on the Mott transition in chromium-doped V2O3. Nat Commun 2010; 1:105. [DOI: 10.1038/ncomms1109] [Citation(s) in RCA: 107] [Impact Index Per Article: 7.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/07/2010] [Accepted: 10/07/2010] [Indexed: 11/09/2022] Open
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Rodolakis F, Hansmann P, Rueff JP, Toschi A, Haverkort MW, Sangiovanni G, Tanaka A, Saha-Dasgupta T, Andersen OK, Held K, Sikora M, Alliot I, Itié JP, Baudelet F, Wzietek P, Metcalf P, Marsi M. Inequivalent routes across the Mott transition in V2O3 explored by X-ray absorption. Phys Rev Lett 2010; 104:047401. [PMID: 20366736 DOI: 10.1103/physrevlett.104.047401] [Citation(s) in RCA: 8] [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: 05/29/2009] [Indexed: 05/29/2023]
Abstract
The changes in the electronic structure of V2O3 across the metal-insulator transition induced by temperature, doping, and pressure are identified using high resolution x-ray absorption spectroscopy at the V pre-K edge. Contrary to what has been taken for granted so far, the metallic phase reached under pressure is shown to differ from the one obtained by changing doping or temperature. Using a novel computational scheme, we relate this effect to the role and occupancy of the a{1g} orbitals. This finding unveils the inequivalence of different routes across the Mott transition in V2O3.
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Affiliation(s)
- F Rodolakis
- Laboratoire de Physique des Solides, CNRS-UMR 8502, Université Paris-Sud, F-91405 Orsay, France
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Rodolakis F, Mansart B, Papalazarou E, Gorovikov S, Vilmercati P, Petaccia L, Goldoni A, Rueff JP, Lupi S, Metcalf P, Marsi M. Quasiparticles at the Mott transition in V2O3: wave vector dependence and surface attenuation. Phys Rev Lett 2009; 102:066805. [PMID: 19257621 DOI: 10.1103/physrevlett.102.066805] [Citation(s) in RCA: 7] [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: 10/03/2008] [Indexed: 05/27/2023]
Abstract
We present an angle resolved photoemission study of V2O3, a prototype system for the observation of Mott transitions in correlated materials. We show that the spectral features corresponding to the quasiparticle peak in the metallic phase present a marked wave vector dependence, with a stronger intensity along the GammaZ direction. The analysis of their intensity for different probing depths shows the existence of a characteristic length scale for the attenuation of coherent electronic excitations at the surface. This length scale, which is larger than the thickness of the surface region as normally defined for noncorrelated electronic states, is found to increase when approaching the Mott transition. These results are in agreement with the behavior of quasiparticles at surfaces as predicted by Borghi et al.
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Affiliation(s)
- F Rodolakis
- Laboratoire de Physique des Solides, CNRS-UMR 8502, Université Paris-Sud, F-91405 Orsay, France
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