A new collimated multichannel modular detection system based on Silicon Drift Detectors
After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multi...
Ausführliche Beschreibung
Autor*in: |
Cirrincione, D. [verfasserIn] Antonelli, M. [verfasserIn] Aquilanti, G. [verfasserIn] Bellutti, P. [verfasserIn] Bertuccio, G. [verfasserIn] Borghi, G. [verfasserIn] Cautero, G. [verfasserIn] Ficorella, F. [verfasserIn] Gandola, M. [verfasserIn] Giuressi, D. [verfasserIn] Mele, F. [verfasserIn] Menk, R.H. [verfasserIn] Olivi, L. [verfasserIn] Orzan, G. [verfasserIn] Pepponi, G. [verfasserIn] Picciotto, A. [verfasserIn] Rashevskaya, I. [verfasserIn] Rachevski, A. [verfasserIn] Stebel, L. [verfasserIn] Zampa, G. [verfasserIn] Zampa, N. [verfasserIn] Zorzi, N. [verfasserIn] Vacchi, A. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2023 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Nuclear instruments & methods in physics research / A - Amsterdam : North-Holland Publ. Co., 1984, 1049 |
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Übergeordnetes Werk: |
volume:1049 |
DOI / URN: |
10.1016/j.nima.2023.168118 |
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Katalog-ID: |
ELV00929936X |
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245 | 1 | 0 | |a A new collimated multichannel modular detection system based on Silicon Drift Detectors |
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520 | |a After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. | ||
650 | 4 | |a X-ray spectroscopy | |
650 | 4 | |a Silicon Drift Detectors | |
650 | 4 | |a XRF | |
650 | 4 | |a XAFS | |
650 | 4 | |a Detection system | |
650 | 4 | |a Collimation | |
700 | 1 | |a Antonelli, M. |e verfasserin |0 (orcid)0000-0003-3400-6710 |4 aut | |
700 | 1 | |a Aquilanti, G. |e verfasserin |4 aut | |
700 | 1 | |a Bellutti, P. |e verfasserin |4 aut | |
700 | 1 | |a Bertuccio, G. |e verfasserin |4 aut | |
700 | 1 | |a Borghi, G. |e verfasserin |0 (orcid)0000-0001-8488-4728 |4 aut | |
700 | 1 | |a Cautero, G. |e verfasserin |4 aut | |
700 | 1 | |a Ficorella, F. |e verfasserin |4 aut | |
700 | 1 | |a Gandola, M. |e verfasserin |4 aut | |
700 | 1 | |a Giuressi, D. |e verfasserin |0 (orcid)0000-0003-3169-7261 |4 aut | |
700 | 1 | |a Mele, F. |e verfasserin |4 aut | |
700 | 1 | |a Menk, R.H. |e verfasserin |4 aut | |
700 | 1 | |a Olivi, L. |e verfasserin |4 aut | |
700 | 1 | |a Orzan, G. |e verfasserin |4 aut | |
700 | 1 | |a Pepponi, G. |e verfasserin |0 (orcid)0000-0002-7397-1946 |4 aut | |
700 | 1 | |a Picciotto, A. |e verfasserin |4 aut | |
700 | 1 | |a Rashevskaya, I. |e verfasserin |4 aut | |
700 | 1 | |a Rachevski, A. |e verfasserin |0 (orcid)0000-0002-2723-6297 |4 aut | |
700 | 1 | |a Stebel, L. |e verfasserin |4 aut | |
700 | 1 | |a Zampa, G. |e verfasserin |0 (orcid)0000-0003-0238-4469 |4 aut | |
700 | 1 | |a Zampa, N. |e verfasserin |0 (orcid)0000-0003-3842-993X |4 aut | |
700 | 1 | |a Zorzi, N. |e verfasserin |0 (orcid)0000-0002-6650-3925 |4 aut | |
700 | 1 | |a Vacchi, A. |e verfasserin |0 (orcid)0000-0003-3855-5856 |4 aut | |
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10.1016/j.nima.2023.168118 doi (DE-627)ELV00929936X (ELSEVIER)S0168-9002(23)00108-0 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Cirrincione, D. verfasserin (orcid)0000-0002-2861-0738 aut A new collimated multichannel modular detection system based on Silicon Drift Detectors 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. X-ray spectroscopy Silicon Drift Detectors XRF XAFS Detection system Collimation Antonelli, M. verfasserin (orcid)0000-0003-3400-6710 aut Aquilanti, G. verfasserin aut Bellutti, P. verfasserin aut Bertuccio, G. verfasserin aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Cautero, G. verfasserin aut Ficorella, F. verfasserin aut Gandola, M. verfasserin aut Giuressi, D. verfasserin (orcid)0000-0003-3169-7261 aut Mele, F. verfasserin aut Menk, R.H. verfasserin aut Olivi, L. verfasserin aut Orzan, G. verfasserin aut Pepponi, G. verfasserin (orcid)0000-0002-7397-1946 aut Picciotto, A. verfasserin aut Rashevskaya, I. verfasserin aut Rachevski, A. verfasserin (orcid)0000-0002-2723-6297 aut Stebel, L. verfasserin aut Zampa, G. verfasserin (orcid)0000-0003-0238-4469 aut Zampa, N. verfasserin (orcid)0000-0003-3842-993X aut Zorzi, N. verfasserin (orcid)0000-0002-6650-3925 aut Vacchi, A. verfasserin (orcid)0000-0003-3855-5856 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1049 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1049 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.05 Experimentalphysik 33.07 Spektroskopie 33.40 Kernphysik AR 1049 |
spelling |
10.1016/j.nima.2023.168118 doi (DE-627)ELV00929936X (ELSEVIER)S0168-9002(23)00108-0 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Cirrincione, D. verfasserin (orcid)0000-0002-2861-0738 aut A new collimated multichannel modular detection system based on Silicon Drift Detectors 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. X-ray spectroscopy Silicon Drift Detectors XRF XAFS Detection system Collimation Antonelli, M. verfasserin (orcid)0000-0003-3400-6710 aut Aquilanti, G. verfasserin aut Bellutti, P. verfasserin aut Bertuccio, G. verfasserin aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Cautero, G. verfasserin aut Ficorella, F. verfasserin aut Gandola, M. verfasserin aut Giuressi, D. verfasserin (orcid)0000-0003-3169-7261 aut Mele, F. verfasserin aut Menk, R.H. verfasserin aut Olivi, L. verfasserin aut Orzan, G. verfasserin aut Pepponi, G. verfasserin (orcid)0000-0002-7397-1946 aut Picciotto, A. verfasserin aut Rashevskaya, I. verfasserin aut Rachevski, A. verfasserin (orcid)0000-0002-2723-6297 aut Stebel, L. verfasserin aut Zampa, G. verfasserin (orcid)0000-0003-0238-4469 aut Zampa, N. verfasserin (orcid)0000-0003-3842-993X aut Zorzi, N. verfasserin (orcid)0000-0002-6650-3925 aut Vacchi, A. verfasserin (orcid)0000-0003-3855-5856 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1049 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1049 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.05 Experimentalphysik 33.07 Spektroskopie 33.40 Kernphysik AR 1049 |
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10.1016/j.nima.2023.168118 doi (DE-627)ELV00929936X (ELSEVIER)S0168-9002(23)00108-0 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Cirrincione, D. verfasserin (orcid)0000-0002-2861-0738 aut A new collimated multichannel modular detection system based on Silicon Drift Detectors 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. X-ray spectroscopy Silicon Drift Detectors XRF XAFS Detection system Collimation Antonelli, M. verfasserin (orcid)0000-0003-3400-6710 aut Aquilanti, G. verfasserin aut Bellutti, P. verfasserin aut Bertuccio, G. verfasserin aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Cautero, G. verfasserin aut Ficorella, F. verfasserin aut Gandola, M. verfasserin aut Giuressi, D. verfasserin (orcid)0000-0003-3169-7261 aut Mele, F. verfasserin aut Menk, R.H. verfasserin aut Olivi, L. verfasserin aut Orzan, G. verfasserin aut Pepponi, G. verfasserin (orcid)0000-0002-7397-1946 aut Picciotto, A. verfasserin aut Rashevskaya, I. verfasserin aut Rachevski, A. verfasserin (orcid)0000-0002-2723-6297 aut Stebel, L. verfasserin aut Zampa, G. verfasserin (orcid)0000-0003-0238-4469 aut Zampa, N. verfasserin (orcid)0000-0003-3842-993X aut Zorzi, N. verfasserin (orcid)0000-0002-6650-3925 aut Vacchi, A. verfasserin (orcid)0000-0003-3855-5856 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1049 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1049 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.05 Experimentalphysik 33.07 Spektroskopie 33.40 Kernphysik AR 1049 |
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10.1016/j.nima.2023.168118 doi (DE-627)ELV00929936X (ELSEVIER)S0168-9002(23)00108-0 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Cirrincione, D. verfasserin (orcid)0000-0002-2861-0738 aut A new collimated multichannel modular detection system based on Silicon Drift Detectors 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. X-ray spectroscopy Silicon Drift Detectors XRF XAFS Detection system Collimation Antonelli, M. verfasserin (orcid)0000-0003-3400-6710 aut Aquilanti, G. verfasserin aut Bellutti, P. verfasserin aut Bertuccio, G. verfasserin aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Cautero, G. verfasserin aut Ficorella, F. verfasserin aut Gandola, M. verfasserin aut Giuressi, D. verfasserin (orcid)0000-0003-3169-7261 aut Mele, F. verfasserin aut Menk, R.H. verfasserin aut Olivi, L. verfasserin aut Orzan, G. verfasserin aut Pepponi, G. verfasserin (orcid)0000-0002-7397-1946 aut Picciotto, A. verfasserin aut Rashevskaya, I. verfasserin aut Rachevski, A. verfasserin (orcid)0000-0002-2723-6297 aut Stebel, L. verfasserin aut Zampa, G. verfasserin (orcid)0000-0003-0238-4469 aut Zampa, N. verfasserin (orcid)0000-0003-3842-993X aut Zorzi, N. verfasserin (orcid)0000-0002-6650-3925 aut Vacchi, A. verfasserin (orcid)0000-0003-3855-5856 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1049 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1049 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.05 Experimentalphysik 33.07 Spektroskopie 33.40 Kernphysik AR 1049 |
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10.1016/j.nima.2023.168118 doi (DE-627)ELV00929936X (ELSEVIER)S0168-9002(23)00108-0 DE-627 ger DE-627 rda eng 530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl Cirrincione, D. verfasserin (orcid)0000-0002-2861-0738 aut A new collimated multichannel modular detection system based on Silicon Drift Detectors 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. X-ray spectroscopy Silicon Drift Detectors XRF XAFS Detection system Collimation Antonelli, M. verfasserin (orcid)0000-0003-3400-6710 aut Aquilanti, G. verfasserin aut Bellutti, P. verfasserin aut Bertuccio, G. verfasserin aut Borghi, G. verfasserin (orcid)0000-0001-8488-4728 aut Cautero, G. verfasserin aut Ficorella, F. verfasserin aut Gandola, M. verfasserin aut Giuressi, D. verfasserin (orcid)0000-0003-3169-7261 aut Mele, F. verfasserin aut Menk, R.H. verfasserin aut Olivi, L. verfasserin aut Orzan, G. verfasserin aut Pepponi, G. verfasserin (orcid)0000-0002-7397-1946 aut Picciotto, A. verfasserin aut Rashevskaya, I. verfasserin aut Rachevski, A. verfasserin (orcid)0000-0002-2723-6297 aut Stebel, L. verfasserin aut Zampa, G. verfasserin (orcid)0000-0003-0238-4469 aut Zampa, N. verfasserin (orcid)0000-0003-3842-993X aut Zorzi, N. verfasserin (orcid)0000-0002-6650-3925 aut Vacchi, A. verfasserin (orcid)0000-0003-3855-5856 aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 1049 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:1049 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_65 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.05 Experimentalphysik 33.07 Spektroskopie 33.40 Kernphysik AR 1049 |
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Cirrincione, D. @@aut@@ Antonelli, M. @@aut@@ Aquilanti, G. @@aut@@ Bellutti, P. @@aut@@ Bertuccio, G. @@aut@@ Borghi, G. @@aut@@ Cautero, G. @@aut@@ Ficorella, F. @@aut@@ Gandola, M. @@aut@@ Giuressi, D. @@aut@@ Mele, F. @@aut@@ Menk, R.H. @@aut@@ Olivi, L. @@aut@@ Orzan, G. @@aut@@ Pepponi, G. @@aut@@ Picciotto, A. @@aut@@ Rashevskaya, I. @@aut@@ Rachevski, A. @@aut@@ Stebel, L. @@aut@@ Zampa, G. @@aut@@ Zampa, N. @@aut@@ Zorzi, N. @@aut@@ Vacchi, A. @@aut@@ |
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Cirrincione, D. |
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Cirrincione, D. ddc 530 bkl 33.05 bkl 33.07 bkl 33.40 misc X-ray spectroscopy misc Silicon Drift Detectors misc XRF misc XAFS misc Detection system misc Collimation A new collimated multichannel modular detection system based on Silicon Drift Detectors |
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530 DE-600 33.05 bkl 33.07 bkl 33.40 bkl A new collimated multichannel modular detection system based on Silicon Drift Detectors X-ray spectroscopy Silicon Drift Detectors XRF XAFS Detection system Collimation |
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Cirrincione, D. Antonelli, M. Aquilanti, G. Bellutti, P. Bertuccio, G. Borghi, G. Cautero, G. Ficorella, F. Gandola, M. Giuressi, D. Mele, F. Menk, R.H. Olivi, L. Orzan, G. Pepponi, G. Picciotto, A. Rashevskaya, I. Rachevski, A. Stebel, L. Zampa, G. Zampa, N. Zorzi, N. Vacchi, A. |
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10.1016/j.nima.2023.168118 |
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a new collimated multichannel modular detection system based on silicon drift detectors |
title_auth |
A new collimated multichannel modular detection system based on Silicon Drift Detectors |
abstract |
After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. |
abstractGer |
After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. |
abstract_unstemmed |
After the manufacture and delivery of a state-of-the-art detection system for the XRF-XAFS beamline of the synchrotron light source SESAME, a new and improved detection system was realized. This new multichannel modular detection system based on Silicon Drift Detectors consists of 8 monolithic multipixel arrays, each comprising 8 SDD cells with a total area of 570 mm 2 . As the previous one, this 64 channels integrated detection system includes ultra-low-noise front-end electronics, dedicated acquisition system, digital filtering, temperature control and stabilization. With respect to the SESAME version, the new instrument implements a tungsten collimation system yielding a total collimated sensitive area of 500 mm 2 . Optimized to work in an energy range of 3–30 keV, the system shows an overall energy resolution (sum of its 64 cells) below 180 eV FWHM at the 5.9 Mn K α line at room temperature. We highlight the system performance and in particular the peak to background ratio, before and after the collimation of the sensors. |
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title_short |
A new collimated multichannel modular detection system based on Silicon Drift Detectors |
remote_bool |
true |
author2 |
Antonelli, M. Aquilanti, G. Bellutti, P. Bertuccio, G. Borghi, G. Cautero, G. Ficorella, F. Gandola, M. Giuressi, D. Mele, F. Menk, R.H. Olivi, L. Orzan, G. Pepponi, G. Picciotto, A. Rashevskaya, I. Rachevski, A. Stebel, L. Zampa, G. Zampa, N. Zorzi, N. Vacchi, A. |
author2Str |
Antonelli, M. Aquilanti, G. Bellutti, P. Bertuccio, G. Borghi, G. Cautero, G. Ficorella, F. Gandola, M. Giuressi, D. Mele, F. Menk, R.H. Olivi, L. Orzan, G. Pepponi, G. Picciotto, A. Rashevskaya, I. Rachevski, A. Stebel, L. Zampa, G. Zampa, N. Zorzi, N. Vacchi, A. |
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266014666 |
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doi_str |
10.1016/j.nima.2023.168118 |
up_date |
2024-07-06T22:41:30.013Z |
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