Design of the Cryogen-Free Cryogenic System for the CUORE Experiment
Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Nucciotti, A. [verfasserIn] Schaeffer, D. [verfasserIn] Alessandria, F. [verfasserIn] Ardito, R. [verfasserIn] Barucci, M. [verfasserIn] Risegari, L. [verfasserIn] Ventura, G. [verfasserIn] Bucci, C. [verfasserIn] Frossati, G. [verfasserIn] Olcese, M. [verfasserIn] de Waard, A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2008 |
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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, 151(2008), 3-4 vom: 19. Jan., Seite 662-668 |
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| Übergeordnetes Werk: |
volume:151 ; year:2008 ; number:3-4 ; day:19 ; month:01 ; pages:662-668 |
| Links: |
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| DOI / URN: |
10.1007/s10909-008-9723-8 |
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| Katalog-ID: |
SPR014507781 |
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| 245 | 1 | 0 | |a Design of the Cryogen-Free Cryogenic System for the CUORE Experiment |
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| 520 | |a Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. | ||
| 650 | 4 | |a Dilution refrigerator |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Pulse tube |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Cryostat |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Double beta decay |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Schaeffer, D. |e verfasserin |4 aut | |
| 700 | 1 | |a Alessandria, F. |e verfasserin |4 aut | |
| 700 | 1 | |a Ardito, R. |e verfasserin |4 aut | |
| 700 | 1 | |a Barucci, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Risegari, L. |e verfasserin |4 aut | |
| 700 | 1 | |a Ventura, G. |e verfasserin |4 aut | |
| 700 | 1 | |a Bucci, C. |e verfasserin |4 aut | |
| 700 | 1 | |a Frossati, G. |e verfasserin |4 aut | |
| 700 | 1 | |a Olcese, M. |e verfasserin |4 aut | |
| 700 | 1 | |a de Waard, A. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Journal of low temperature physics |d Dordrecht : Springer Science + Business Media B.V., 1969 |g 151(2008), 3-4 vom: 19. Jan., Seite 662-668 |w (DE-627)320575411 |w (DE-600)2016984-X |x 1573-7357 |7 nnns |
| 773 | 1 | 8 | |g volume:151 |g year:2008 |g number:3-4 |g day:19 |g month:01 |g pages:662-668 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s10909-008-9723-8 |z lizenzpflichtig |3 Volltext |
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| 912 | |a GBV_ILN_2026 | ||
| 912 | |a GBV_ILN_2027 | ||
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| 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 | ||
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| 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 | ||
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| 912 | |a GBV_ILN_4242 | ||
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| 912 | |a GBV_ILN_4338 | ||
| 912 | |a GBV_ILN_4393 | ||
| 912 | |a GBV_ILN_4700 | ||
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| 952 | |d 151 |j 2008 |e 3-4 |b 19 |c 01 |h 662-668 | ||
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2008 |
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| publishDate |
2008 |
| allfields |
10.1007/s10909-008-9723-8 doi (DE-627)SPR014507781 (SPR)s10909-008-9723-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Nucciotti, A. verfasserin aut Design of the Cryogen-Free Cryogenic System for the CUORE Experiment 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. Dilution refrigerator (dpeaa)DE-He213 Pulse tube (dpeaa)DE-He213 Cryostat (dpeaa)DE-He213 Double beta decay (dpeaa)DE-He213 Schaeffer, D. verfasserin aut Alessandria, F. verfasserin aut Ardito, R. verfasserin aut Barucci, M. verfasserin aut Risegari, L. verfasserin aut Ventura, G. verfasserin aut Bucci, C. verfasserin aut Frossati, G. verfasserin aut Olcese, M. verfasserin aut de Waard, A. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 151(2008), 3-4 vom: 19. Jan., Seite 662-668 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:151 year:2008 number:3-4 day:19 month:01 pages:662-668 https://dx.doi.org/10.1007/s10909-008-9723-8 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_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 151 2008 3-4 19 01 662-668 |
| spelling |
10.1007/s10909-008-9723-8 doi (DE-627)SPR014507781 (SPR)s10909-008-9723-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Nucciotti, A. verfasserin aut Design of the Cryogen-Free Cryogenic System for the CUORE Experiment 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. Dilution refrigerator (dpeaa)DE-He213 Pulse tube (dpeaa)DE-He213 Cryostat (dpeaa)DE-He213 Double beta decay (dpeaa)DE-He213 Schaeffer, D. verfasserin aut Alessandria, F. verfasserin aut Ardito, R. verfasserin aut Barucci, M. verfasserin aut Risegari, L. verfasserin aut Ventura, G. verfasserin aut Bucci, C. verfasserin aut Frossati, G. verfasserin aut Olcese, M. verfasserin aut de Waard, A. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 151(2008), 3-4 vom: 19. Jan., Seite 662-668 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:151 year:2008 number:3-4 day:19 month:01 pages:662-668 https://dx.doi.org/10.1007/s10909-008-9723-8 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_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 151 2008 3-4 19 01 662-668 |
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10.1007/s10909-008-9723-8 doi (DE-627)SPR014507781 (SPR)s10909-008-9723-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Nucciotti, A. verfasserin aut Design of the Cryogen-Free Cryogenic System for the CUORE Experiment 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. Dilution refrigerator (dpeaa)DE-He213 Pulse tube (dpeaa)DE-He213 Cryostat (dpeaa)DE-He213 Double beta decay (dpeaa)DE-He213 Schaeffer, D. verfasserin aut Alessandria, F. verfasserin aut Ardito, R. verfasserin aut Barucci, M. verfasserin aut Risegari, L. verfasserin aut Ventura, G. verfasserin aut Bucci, C. verfasserin aut Frossati, G. verfasserin aut Olcese, M. verfasserin aut de Waard, A. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 151(2008), 3-4 vom: 19. Jan., Seite 662-668 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:151 year:2008 number:3-4 day:19 month:01 pages:662-668 https://dx.doi.org/10.1007/s10909-008-9723-8 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_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 151 2008 3-4 19 01 662-668 |
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10.1007/s10909-008-9723-8 doi (DE-627)SPR014507781 (SPR)s10909-008-9723-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Nucciotti, A. verfasserin aut Design of the Cryogen-Free Cryogenic System for the CUORE Experiment 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. Dilution refrigerator (dpeaa)DE-He213 Pulse tube (dpeaa)DE-He213 Cryostat (dpeaa)DE-He213 Double beta decay (dpeaa)DE-He213 Schaeffer, D. verfasserin aut Alessandria, F. verfasserin aut Ardito, R. verfasserin aut Barucci, M. verfasserin aut Risegari, L. verfasserin aut Ventura, G. verfasserin aut Bucci, C. verfasserin aut Frossati, G. verfasserin aut Olcese, M. verfasserin aut de Waard, A. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 151(2008), 3-4 vom: 19. Jan., Seite 662-668 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:151 year:2008 number:3-4 day:19 month:01 pages:662-668 https://dx.doi.org/10.1007/s10909-008-9723-8 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_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 151 2008 3-4 19 01 662-668 |
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10.1007/s10909-008-9723-8 doi (DE-627)SPR014507781 (SPR)s10909-008-9723-8-e DE-627 ger DE-627 rakwb eng 530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Nucciotti, A. verfasserin aut Design of the Cryogen-Free Cryogenic System for the CUORE Experiment 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. Dilution refrigerator (dpeaa)DE-He213 Pulse tube (dpeaa)DE-He213 Cryostat (dpeaa)DE-He213 Double beta decay (dpeaa)DE-He213 Schaeffer, D. verfasserin aut Alessandria, F. verfasserin aut Ardito, R. verfasserin aut Barucci, M. verfasserin aut Risegari, L. verfasserin aut Ventura, G. verfasserin aut Bucci, C. verfasserin aut Frossati, G. verfasserin aut Olcese, M. verfasserin aut de Waard, A. verfasserin aut Enthalten in Journal of low temperature physics Dordrecht : Springer Science + Business Media B.V., 1969 151(2008), 3-4 vom: 19. Jan., Seite 662-668 (DE-627)320575411 (DE-600)2016984-X 1573-7357 nnns volume:151 year:2008 number:3-4 day:19 month:01 pages:662-668 https://dx.doi.org/10.1007/s10909-008-9723-8 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_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 151 2008 3-4 19 01 662-668 |
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Nucciotti, A. @@aut@@ Schaeffer, D. @@aut@@ Alessandria, F. @@aut@@ Ardito, R. @@aut@@ Barucci, M. @@aut@@ Risegari, L. @@aut@@ Ventura, G. @@aut@@ Bucci, C. @@aut@@ Frossati, G. @@aut@@ Olcese, M. @@aut@@ de Waard, A. @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR014507781</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111010852.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2008 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10909-008-9723-8</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR014507781</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10909-008-9723-8-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.09</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.30</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.60</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Nucciotti, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Design of the Cryogen-Free Cryogenic System for the CUORE Experiment</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2008</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. 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Nucciotti, A. |
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Nucciotti, A. ddc 530 bkl 33.09 bkl 33.30 bkl 33.60 misc Dilution refrigerator misc Pulse tube misc Cryostat misc Double beta decay Design of the Cryogen-Free Cryogenic System for the CUORE Experiment |
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530 ASE 33.09 bkl 33.30 bkl 33.60 bkl Design of the Cryogen-Free Cryogenic System for the CUORE Experiment Dilution refrigerator (dpeaa)DE-He213 Pulse tube (dpeaa)DE-He213 Cryostat (dpeaa)DE-He213 Double beta decay (dpeaa)DE-He213 |
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Nucciotti, A. Schaeffer, D. Alessandria, F. Ardito, R. Barucci, M. Risegari, L. Ventura, G. Bucci, C. Frossati, G. Olcese, M. de Waard, A. |
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Nucciotti, A. |
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design of the cryogen-free cryogenic system for the cuore experiment |
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Design of the Cryogen-Free Cryogenic System for the CUORE Experiment |
| abstract |
Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. |
| abstractGer |
Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. |
| abstract_unstemmed |
Abstract We present here the final design of the cryogenic system where the CUORE detector will be installed in 2010. It is a large cryogen-free cryostat cooled by pulse tubes and by a high-power dilution refrigerator. To avoid radioactive background, about 15000 kg of lead will be cooled to below 1 K and only few construction materials are acceptable. The detector assembly will have a total mass of about 1500 kg and must be cooled to less than 10 mK in a vibration-free environment. We discuss the adopted technical solutions, the results of the preliminary thermal analysis of the system, and its expected performance. |
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Design of the Cryogen-Free Cryogenic System for the CUORE Experiment |
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| score |
7.398756 |