The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection

Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and...
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Autor*in:	Kikuchi, T. [verfasserIn] Hoshino, M. [verfasserIn] Nakayama, T. [verfasserIn] Yamasaki, N. Y. [verfasserIn] Maehata, K. [verfasserIn] Mitsuda, K. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2016

Schlagwörter:	X-ray Microcalorimeter Dielectric material

Übergeordnetes Werk:	Enthalten in: Journal of low temperature physics - Dordrecht : Springer Science + Business Media B.V., 1969, 184(2016), 1-2 vom: 22. März, Seite 250-256
Übergeordnetes Werk:	volume:184 ; year:2016 ; number:1-2 ; day:22 ; month:03 ; pages:250-256

Links:	Volltext

DOI / URN:	10.1007/s10909-016-1587-8

Katalog-ID:	SPR014527235

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520			\|a Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection.
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700	1		\|a Yamasaki, N. Y. \|e verfasserin \|4 aut
700	1		\|a Maehata, K. \|e verfasserin \|4 aut
700	1		\|a Mitsuda, K. \|e verfasserin \|4 aut
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912			\|a GBV_ILN_24
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912			\|a GBV_ILN_32
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2116
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2119
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2144
912			\|a GBV_ILN_2147
912			\|a GBV_ILN_2148
912			\|a GBV_ILN_2152
912			\|a GBV_ILN_2153
912			\|a GBV_ILN_2188
912			\|a GBV_ILN_2190
912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
912			\|a GBV_ILN_2470
912			\|a GBV_ILN_2472
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_2548
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4246
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4251
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4328
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4393
912			\|a GBV_ILN_4700
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951			\|a AR
952			\|d 184 \|j 2016 \|e 1-2 \|b 22 \|c 03 \|h 250-256

Indexfelder

author_variant	t k tk m h mh t n tn n y y ny nyy k m km k m km
matchkey_str	article:15737357:2016----::hdsgadhrceiainfilcrcirclrmtr
hierarchy_sort_str	2016
bklnumber	33.09 33.30 33.60
publishDate	2016
allfields	10.1007/s10909-016-1587-8 doi (DE-627)SPR014527235 (SPR)s10909-016-1587-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Kikuchi, T. verfasserin aut The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection. X-ray (dpeaa)DE-He213 Microcalorimeter (dpeaa)DE-He213 Dielectric material (dpeaa)DE-He213 Hoshino, M. verfasserin aut Nakayama, T. verfasserin aut Yamasaki, N. Y. verfasserin aut Maehata, K. verfasserin aut Mitsuda, K. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 184(2016), 1-2 vom: 22. März, Seite 250-256 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256 https://dx.doi.org/10.1007/s10909-016-1587-8 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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 184 2016 1-2 22 03 250-256
spelling	10.1007/s10909-016-1587-8 doi (DE-627)SPR014527235 (SPR)s10909-016-1587-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Kikuchi, T. verfasserin aut The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection. X-ray (dpeaa)DE-He213 Microcalorimeter (dpeaa)DE-He213 Dielectric material (dpeaa)DE-He213 Hoshino, M. verfasserin aut Nakayama, T. verfasserin aut Yamasaki, N. Y. verfasserin aut Maehata, K. verfasserin aut Mitsuda, K. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 184(2016), 1-2 vom: 22. März, Seite 250-256 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256 https://dx.doi.org/10.1007/s10909-016-1587-8 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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 184 2016 1-2 22 03 250-256
allfields_unstemmed	10.1007/s10909-016-1587-8 doi (DE-627)SPR014527235 (SPR)s10909-016-1587-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Kikuchi, T. verfasserin aut The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection. X-ray (dpeaa)DE-He213 Microcalorimeter (dpeaa)DE-He213 Dielectric material (dpeaa)DE-He213 Hoshino, M. verfasserin aut Nakayama, T. verfasserin aut Yamasaki, N. Y. verfasserin aut Maehata, K. verfasserin aut Mitsuda, K. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 184(2016), 1-2 vom: 22. März, Seite 250-256 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256 https://dx.doi.org/10.1007/s10909-016-1587-8 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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 184 2016 1-2 22 03 250-256
allfieldsGer	10.1007/s10909-016-1587-8 doi (DE-627)SPR014527235 (SPR)s10909-016-1587-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Kikuchi, T. verfasserin aut The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection. X-ray (dpeaa)DE-He213 Microcalorimeter (dpeaa)DE-He213 Dielectric material (dpeaa)DE-He213 Hoshino, M. verfasserin aut Nakayama, T. verfasserin aut Yamasaki, N. Y. verfasserin aut Maehata, K. verfasserin aut Mitsuda, K. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 184(2016), 1-2 vom: 22. März, Seite 250-256 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256 https://dx.doi.org/10.1007/s10909-016-1587-8 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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 184 2016 1-2 22 03 250-256
allfieldsSound	10.1007/s10909-016-1587-8 doi (DE-627)SPR014527235 (SPR)s10909-016-1587-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Kikuchi, T. verfasserin aut The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection. X-ray (dpeaa)DE-He213 Microcalorimeter (dpeaa)DE-He213 Dielectric material (dpeaa)DE-He213 Hoshino, M. verfasserin aut Nakayama, T. verfasserin aut Yamasaki, N. Y. verfasserin aut Maehata, K. verfasserin aut Mitsuda, K. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 184(2016), 1-2 vom: 22. März, Seite 250-256 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256 https://dx.doi.org/10.1007/s10909-016-1587-8 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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 184 2016 1-2 22 03 250-256
language	English
source	Enthalten in Journal of low temperature physics 184(2016), 1-2 vom: 22. März, Seite 250-256 volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256
sourceStr	Enthalten in Journal of low temperature physics 184(2016), 1-2 vom: 22. März, Seite 250-256 volume:184 year:2016 number:1-2 day:22 month:03 pages:250-256
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	X-ray Microcalorimeter Dielectric material
dewey-raw	530
isfreeaccess_bool	false
container_title	Journal of low temperature physics
authorswithroles_txt_mv	Kikuchi, T. @@aut@@ Hoshino, M. @@aut@@ Nakayama, T. @@aut@@ Yamasaki, N. Y. @@aut@@ Maehata, K. @@aut@@ Mitsuda, K. @@aut@@
publishDateDaySort_date	2016-03-22T00:00:00Z
hierarchy_top_id	320575411
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author	Kikuchi, T.
spellingShingle	Kikuchi, T. ddc 530 bkl 33.09 bkl 33.30 bkl 33.60 misc X-ray misc Microcalorimeter misc Dielectric material The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection
authorStr	Kikuchi, T.
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topic_title	530 ASE 33.09 bkl 33.30 bkl 33.60 bkl The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection X-ray (dpeaa)DE-He213 Microcalorimeter (dpeaa)DE-He213 Dielectric material (dpeaa)DE-He213
topic	ddc 530 bkl 33.09 bkl 33.30 bkl 33.60 misc X-ray misc Microcalorimeter misc Dielectric material
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title	The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection
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title_full	The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection
author_sort	Kikuchi, T.
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author_browse	Kikuchi, T. Hoshino, M. Nakayama, T. Yamasaki, N. Y. Maehata, K. Mitsuda, K.
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title_sort	design and characterization of dielectric microcalorimeters for x-ray photon detection
title_auth	The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection
abstract	Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection.
abstractGer	Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection.
abstract_unstemmed	Abstract The dielectric micro calorimeter (DMC) is a novel radiation detector utilizing a GHz resonator with dielectric thermometer (Sekiya et al. in J Low Temp Phys 167:435, 2012). The advantage of using a DMC is that the detection mechanism is based on a phonon mediation without Johnson noise and quasi-particle decay process. A large format array of DMCs can be easily multiplexed by a resonator circuit in the readout at GHz band width. We describe the design of a DMC as an X-ray photon counter. It is optimized to detect photon at 5.9 keV energy. We consider %$^{18}%$O-doped SrTiO%$_3%$ (STO18) and Nb-doped KTa%$_{(1-x)}%$Nb%$_{x}%$O%$_{3}%$ (KTN) as a candidate of dielectric thermometer. Dielectric materials which have sensitivity %$\alpha %$(= d%$\log {C_{\mathrm {el}}}/d\log {T}%$) are also ideal for our application. We check that both STO18 and KTN have %$\alpha {\sim } 10^{3}%$ at 100 mK. If we assume a DMC resonator operating at 100 mK, we need a Q value of a resonator to be 2000 for X-ray detection.
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container_issue	1-2
title_short	The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection
url	https://dx.doi.org/10.1007/s10909-016-1587-8
remote_bool	true
author2	Hoshino, M. Nakayama, T. Yamasaki, N. Y. Maehata, K. Mitsuda, K.
author2Str	Hoshino, M. Nakayama, T. Yamasaki, N. Y. Maehata, K. Mitsuda, K.
ppnlink	320575411
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doi_str	10.1007/s10909-016-1587-8
up_date	2024-07-04T02:07:29.833Z
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The Design and Characterization of Dielectric Microcalorimeters for X-ray Photon Detection

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