Integration of a TES-based X-ray spectrometer in a kaonic atom experiment
Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant develop...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Hashimoto, T. [verfasserIn] Bennett, D. A. [verfasserIn] Doriese, W. B. [verfasserIn] Durkin, M. S. [verfasserIn] Fowler, J. W. [verfasserIn] Gard, J. D. [verfasserIn] Hayakawa, R. [verfasserIn] Hayashi, T. [verfasserIn] Hilton, G. C. [verfasserIn] Ichinohe, Y. [verfasserIn] Ishimoto, S. [verfasserIn] Morgan, K. M. [verfasserIn] Noda, H. [verfasserIn] O’Neil, G. C. [verfasserIn] Okada, S. [verfasserIn] Reintsema, C. D. [verfasserIn] Schmidt, D. R. [verfasserIn] Suzuki, S. [verfasserIn] Swetz, D. S. [verfasserIn] Tatsuno, H. [verfasserIn] Ullom, J. N. [verfasserIn] Yamada, S. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of low temperature physics - Dordrecht : Springer Science + Business Media B.V., 1969, 199(2020), 3-4 vom: 27. März, Seite 1018-1026 |
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| Übergeordnetes Werk: |
volume:199 ; year:2020 ; number:3-4 ; day:27 ; month:03 ; pages:1018-1026 |
| Links: |
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| DOI / URN: |
10.1007/s10909-020-02434-1 |
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| Katalog-ID: |
SPR039587681 |
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| 245 | 1 | 0 | |a Integration of a TES-based X-ray spectrometer in a kaonic atom experiment |
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| 520 | |a Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. | ||
| 650 | 4 | |a TES |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Hadron beam |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Kaonic atom |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a X-ray |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a J-PARC |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Bennett, D. A. |e verfasserin |4 aut | |
| 700 | 1 | |a Doriese, W. B. |e verfasserin |4 aut | |
| 700 | 1 | |a Durkin, M. S. |e verfasserin |4 aut | |
| 700 | 1 | |a Fowler, J. W. |e verfasserin |4 aut | |
| 700 | 1 | |a Gard, J. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Hayakawa, R. |e verfasserin |4 aut | |
| 700 | 1 | |a Hayashi, T. |e verfasserin |4 aut | |
| 700 | 1 | |a Hilton, G. C. |e verfasserin |4 aut | |
| 700 | 1 | |a Ichinohe, Y. |e verfasserin |4 aut | |
| 700 | 1 | |a Ishimoto, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Morgan, K. M. |e verfasserin |4 aut | |
| 700 | 1 | |a Noda, H. |e verfasserin |4 aut | |
| 700 | 1 | |a O’Neil, G. C. |e verfasserin |4 aut | |
| 700 | 1 | |a Okada, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Reintsema, C. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Schmidt, D. R. |e verfasserin |4 aut | |
| 700 | 1 | |a Suzuki, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Swetz, D. S. |e verfasserin |4 aut | |
| 700 | 1 | |a Tatsuno, H. |e verfasserin |4 aut | |
| 700 | 1 | |a Ullom, J. N. |e verfasserin |4 aut | |
| 700 | 1 | |a Yamada, S. |e verfasserin |4 aut | |
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10.1007/s10909-020-02434-1 doi (DE-627)SPR039587681 (SPR)s10909-020-02434-1-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Hashimoto, T. verfasserin aut Integration of a TES-based X-ray spectrometer in a kaonic atom experiment 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. TES (dpeaa)DE-He213 Hadron beam (dpeaa)DE-He213 Kaonic atom (dpeaa)DE-He213 X-ray (dpeaa)DE-He213 J-PARC (dpeaa)DE-He213 Bennett, D. A. verfasserin aut Doriese, W. B. verfasserin aut Durkin, M. S. verfasserin aut Fowler, J. W. verfasserin aut Gard, J. D. verfasserin aut Hayakawa, R. verfasserin aut Hayashi, T. verfasserin aut Hilton, G. C. verfasserin aut Ichinohe, Y. verfasserin aut Ishimoto, S. verfasserin aut Morgan, K. M. verfasserin aut Noda, H. verfasserin aut O’Neil, G. C. verfasserin aut Okada, S. verfasserin aut Reintsema, C. D. verfasserin aut Schmidt, D. R. verfasserin aut Suzuki, S. verfasserin aut Swetz, D. S. verfasserin aut Tatsuno, H. verfasserin aut Ullom, J. N. verfasserin aut Yamada, S. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 199(2020), 3-4 vom: 27. März, Seite 1018-1026 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:199 year:2020 number:3-4 day:27 month:03 pages:1018-1026 https://dx.doi.org/10.1007/s10909-020-02434-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.09 ASE 33.30 ASE 33.60 ASE AR 199 2020 3-4 27 03 1018-1026 |
| spelling |
10.1007/s10909-020-02434-1 doi (DE-627)SPR039587681 (SPR)s10909-020-02434-1-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Hashimoto, T. verfasserin aut Integration of a TES-based X-ray spectrometer in a kaonic atom experiment 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. TES (dpeaa)DE-He213 Hadron beam (dpeaa)DE-He213 Kaonic atom (dpeaa)DE-He213 X-ray (dpeaa)DE-He213 J-PARC (dpeaa)DE-He213 Bennett, D. A. verfasserin aut Doriese, W. B. verfasserin aut Durkin, M. S. verfasserin aut Fowler, J. W. verfasserin aut Gard, J. D. verfasserin aut Hayakawa, R. verfasserin aut Hayashi, T. verfasserin aut Hilton, G. C. verfasserin aut Ichinohe, Y. verfasserin aut Ishimoto, S. verfasserin aut Morgan, K. M. verfasserin aut Noda, H. verfasserin aut O’Neil, G. C. verfasserin aut Okada, S. verfasserin aut Reintsema, C. D. verfasserin aut Schmidt, D. R. verfasserin aut Suzuki, S. verfasserin aut Swetz, D. S. verfasserin aut Tatsuno, H. verfasserin aut Ullom, J. N. verfasserin aut Yamada, S. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 199(2020), 3-4 vom: 27. März, Seite 1018-1026 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:199 year:2020 number:3-4 day:27 month:03 pages:1018-1026 https://dx.doi.org/10.1007/s10909-020-02434-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.09 ASE 33.30 ASE 33.60 ASE AR 199 2020 3-4 27 03 1018-1026 |
| allfields_unstemmed |
10.1007/s10909-020-02434-1 doi (DE-627)SPR039587681 (SPR)s10909-020-02434-1-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Hashimoto, T. verfasserin aut Integration of a TES-based X-ray spectrometer in a kaonic atom experiment 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. TES (dpeaa)DE-He213 Hadron beam (dpeaa)DE-He213 Kaonic atom (dpeaa)DE-He213 X-ray (dpeaa)DE-He213 J-PARC (dpeaa)DE-He213 Bennett, D. A. verfasserin aut Doriese, W. B. verfasserin aut Durkin, M. S. verfasserin aut Fowler, J. W. verfasserin aut Gard, J. D. verfasserin aut Hayakawa, R. verfasserin aut Hayashi, T. verfasserin aut Hilton, G. C. verfasserin aut Ichinohe, Y. verfasserin aut Ishimoto, S. verfasserin aut Morgan, K. M. verfasserin aut Noda, H. verfasserin aut O’Neil, G. C. verfasserin aut Okada, S. verfasserin aut Reintsema, C. D. verfasserin aut Schmidt, D. R. verfasserin aut Suzuki, S. verfasserin aut Swetz, D. S. verfasserin aut Tatsuno, H. verfasserin aut Ullom, J. N. verfasserin aut Yamada, S. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 199(2020), 3-4 vom: 27. März, Seite 1018-1026 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:199 year:2020 number:3-4 day:27 month:03 pages:1018-1026 https://dx.doi.org/10.1007/s10909-020-02434-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.09 ASE 33.30 ASE 33.60 ASE AR 199 2020 3-4 27 03 1018-1026 |
| allfieldsGer |
10.1007/s10909-020-02434-1 doi (DE-627)SPR039587681 (SPR)s10909-020-02434-1-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Hashimoto, T. verfasserin aut Integration of a TES-based X-ray spectrometer in a kaonic atom experiment 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. TES (dpeaa)DE-He213 Hadron beam (dpeaa)DE-He213 Kaonic atom (dpeaa)DE-He213 X-ray (dpeaa)DE-He213 J-PARC (dpeaa)DE-He213 Bennett, D. A. verfasserin aut Doriese, W. B. verfasserin aut Durkin, M. S. verfasserin aut Fowler, J. W. verfasserin aut Gard, J. D. verfasserin aut Hayakawa, R. verfasserin aut Hayashi, T. verfasserin aut Hilton, G. C. verfasserin aut Ichinohe, Y. verfasserin aut Ishimoto, S. verfasserin aut Morgan, K. M. verfasserin aut Noda, H. verfasserin aut O’Neil, G. C. verfasserin aut Okada, S. verfasserin aut Reintsema, C. D. verfasserin aut Schmidt, D. R. verfasserin aut Suzuki, S. verfasserin aut Swetz, D. S. verfasserin aut Tatsuno, H. verfasserin aut Ullom, J. N. verfasserin aut Yamada, S. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 199(2020), 3-4 vom: 27. März, Seite 1018-1026 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:199 year:2020 number:3-4 day:27 month:03 pages:1018-1026 https://dx.doi.org/10.1007/s10909-020-02434-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.09 ASE 33.30 ASE 33.60 ASE AR 199 2020 3-4 27 03 1018-1026 |
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10.1007/s10909-020-02434-1 doi (DE-627)SPR039587681 (SPR)s10909-020-02434-1-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Hashimoto, T. verfasserin aut Integration of a TES-based X-ray spectrometer in a kaonic atom experiment 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. TES (dpeaa)DE-He213 Hadron beam (dpeaa)DE-He213 Kaonic atom (dpeaa)DE-He213 X-ray (dpeaa)DE-He213 J-PARC (dpeaa)DE-He213 Bennett, D. A. verfasserin aut Doriese, W. B. verfasserin aut Durkin, M. S. verfasserin aut Fowler, J. W. verfasserin aut Gard, J. D. verfasserin aut Hayakawa, R. verfasserin aut Hayashi, T. verfasserin aut Hilton, G. C. verfasserin aut Ichinohe, Y. verfasserin aut Ishimoto, S. verfasserin aut Morgan, K. M. verfasserin aut Noda, H. verfasserin aut O’Neil, G. C. verfasserin aut Okada, S. verfasserin aut Reintsema, C. D. verfasserin aut Schmidt, D. R. verfasserin aut Suzuki, S. verfasserin aut Swetz, D. S. verfasserin aut Tatsuno, H. verfasserin aut Ullom, J. N. verfasserin aut Yamada, S. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 199(2020), 3-4 vom: 27. März, Seite 1018-1026 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:199 year:2020 number:3-4 day:27 month:03 pages:1018-1026 https://dx.doi.org/10.1007/s10909-020-02434-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.09 ASE 33.30 ASE 33.60 ASE AR 199 2020 3-4 27 03 1018-1026 |
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Hashimoto, T. @@aut@@ Bennett, D. A. @@aut@@ Doriese, W. B. @@aut@@ Durkin, M. S. @@aut@@ Fowler, J. W. @@aut@@ Gard, J. D. @@aut@@ Hayakawa, R. @@aut@@ Hayashi, T. @@aut@@ Hilton, G. C. @@aut@@ Ichinohe, Y. @@aut@@ Ishimoto, S. @@aut@@ Morgan, K. M. @@aut@@ Noda, H. @@aut@@ O’Neil, G. C. @@aut@@ Okada, S. @@aut@@ Reintsema, C. D. @@aut@@ Schmidt, D. R. @@aut@@ Suzuki, S. @@aut@@ Swetz, D. S. @@aut@@ Tatsuno, H. @@aut@@ Ullom, J. N. @@aut@@ Yamada, S. @@aut@@ |
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Hashimoto, T. |
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Hashimoto, T. ddc 530 bkl 33.09 bkl 33.30 bkl 33.60 misc TES misc Hadron beam misc Kaonic atom misc X-ray misc J-PARC Integration of a TES-based X-ray spectrometer in a kaonic atom experiment |
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530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Integration of a TES-based X-ray spectrometer in a kaonic atom experiment TES (dpeaa)DE-He213 Hadron beam (dpeaa)DE-He213 Kaonic atom (dpeaa)DE-He213 X-ray (dpeaa)DE-He213 J-PARC (dpeaa)DE-He213 |
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Integration of a TES-based X-ray spectrometer in a kaonic atom experiment |
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Journal of low temperature physics |
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Hashimoto, T. Bennett, D. A. Doriese, W. B. Durkin, M. S. Fowler, J. W. Gard, J. D. Hayakawa, R. Hayashi, T. Hilton, G. C. Ichinohe, Y. Ishimoto, S. Morgan, K. M. Noda, H. O’Neil, G. C. Okada, S. Reintsema, C. D. Schmidt, D. R. Suzuki, S. Swetz, D. S. Tatsuno, H. Ullom, J. N. Yamada, S. |
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Hashimoto, T. |
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integration of a tes-based x-ray spectrometer in a kaonic atom experiment |
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Integration of a TES-based X-ray spectrometer in a kaonic atom experiment |
| abstract |
Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. |
| abstractGer |
Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. |
| abstract_unstemmed |
Abstract We integrated a TES X-ray spectrometer with a charged kaon beam line at J-PARC to perform X-ray spectroscopy of kaonic helium atoms. Limited beam intensity and a broad beam spot size made it crucial to increase the detector acceptance angle as much as possible, requiring significant development. To this end, our TES system shared the same vacuum with a cryogenic system of the liquid helium experimental target. We also specially developed a target cell for liquid helium and a thinned aperture array on top of the TES detector. Additionally, thermal and magnetic shields and infrared filters were optimized in terms of a larger acceptance angle and energy resolution of the detector. The scientific campaign was performed in June, 2018, where the whole system was stably operated for almost one month. |
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Integration of a TES-based X-ray spectrometer in a kaonic atom experiment |
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Bennett, D. A. Doriese, W. B. Durkin, M. S. Fowler, J. W. Gard, J. D. Hayakawa, R. Hayashi, T. Hilton, G. C. Ichinohe, Y. Ishimoto, S. Morgan, K. M. Noda, H. O’Neil, G. C. Okada, S. Reintsema, C. D. Schmidt, D. R. Suzuki, S. Swetz, D. S. Tatsuno, H. Ullom, J. N. Yamada, S. |
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