Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data
This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) t...
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Gespeichert in:
| Autor*in: |
Tornago, M. [verfasserIn] |
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E-Artikel |
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| Sprache: |
Englisch |
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2021transfer abstract |
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| Übergeordnetes Werk: |
Enthalten in: The efficacy of EEG-biofeedback for acute pain management, a randomized sham-controlled study of a tailored protocol - Ide, C.V. ELSEVIER, 2017, a journal on accelerators, instrumentation and techniques applied to research in nuclear and atomic physics, materials science and related fields in physics, Amsterdam |
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| Übergeordnetes Werk: |
volume:1003 ; year:2021 ; day:1 ; month:07 ; pages:0 |
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| DOI / URN: |
10.1016/j.nima.2021.165319 |
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ELV053864700 |
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| 520 | |a This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. | ||
| 520 | |a This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. | ||
| 650 | 7 | |a 4D tracking |2 Elsevier | |
| 650 | 7 | |a AC-coupled detectors |2 Elsevier | |
| 650 | 7 | |a LGAD |2 Elsevier | |
| 700 | 1 | |a Arcidiacono, R. |4 oth | |
| 700 | 1 | |a Cartiglia, N. |4 oth | |
| 700 | 1 | |a Costa, M. |4 oth | |
| 700 | 1 | |a Ferrero, M. |4 oth | |
| 700 | 1 | |a Mandurrino, M. |4 oth | |
| 700 | 1 | |a Siviero, F. |4 oth | |
| 700 | 1 | |a Sola, V. |4 oth | |
| 700 | 1 | |a Staiano, A. |4 oth | |
| 700 | 1 | |a Apresyan, A. |4 oth | |
| 700 | 1 | |a Di Petrillo, K. |4 oth | |
| 700 | 1 | |a Heller, R. |4 oth | |
| 700 | 1 | |a Los, S. |4 oth | |
| 700 | 1 | |a Borghi, G. |4 oth | |
| 700 | 1 | |a Boscardin, M. |4 oth | |
| 700 | 1 | |a Dalla Betta, G.-F. |4 oth | |
| 700 | 1 | |a Ficorella, F. |4 oth | |
| 700 | 1 | |a Pancheri, L. |4 oth | |
| 700 | 1 | |a Paternoster, G. |4 oth | |
| 700 | 1 | |a Sadrozinski, H. |4 oth | |
| 700 | 1 | |a Seiden, A. |4 oth | |
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10.1016/j.nima.2021.165319 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001379.pica (DE-627)ELV053864700 (ELSEVIER)S0168-9002(21)00303-X DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Tornago, M. verfasserin aut Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. 4D tracking Elsevier AC-coupled detectors Elsevier LGAD Elsevier Arcidiacono, R. oth Cartiglia, N. oth Costa, M. oth Ferrero, M. oth Mandurrino, M. oth Siviero, F. oth Sola, V. oth Staiano, A. oth Apresyan, A. oth Di Petrillo, K. oth Heller, R. oth Los, S. oth Borghi, G. oth Boscardin, M. oth Dalla Betta, G.-F. oth Ficorella, F. oth Pancheri, L. oth Paternoster, G. oth Sadrozinski, H. oth Seiden, A. oth Enthalten in North-Holland Publ. Co Ide, C.V. ELSEVIER The efficacy of EEG-biofeedback for acute pain management, a randomized sham-controlled study of a tailored protocol 2017 a journal on accelerators, instrumentation and techniques applied to research in nuclear and atomic physics, materials science and related fields in physics Amsterdam (DE-627)ELV000874671 volume:1003 year:2021 day:1 month:07 pages:0 https://doi.org/10.1016/j.nima.2021.165319 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1003 2021 1 0701 0 |
| spelling |
10.1016/j.nima.2021.165319 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001379.pica (DE-627)ELV053864700 (ELSEVIER)S0168-9002(21)00303-X DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Tornago, M. verfasserin aut Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. 4D tracking Elsevier AC-coupled detectors Elsevier LGAD Elsevier Arcidiacono, R. oth Cartiglia, N. oth Costa, M. oth Ferrero, M. oth Mandurrino, M. oth Siviero, F. oth Sola, V. oth Staiano, A. oth Apresyan, A. oth Di Petrillo, K. oth Heller, R. oth Los, S. oth Borghi, G. oth Boscardin, M. oth Dalla Betta, G.-F. oth Ficorella, F. oth Pancheri, L. oth Paternoster, G. oth Sadrozinski, H. oth Seiden, A. oth Enthalten in North-Holland Publ. Co Ide, C.V. ELSEVIER The efficacy of EEG-biofeedback for acute pain management, a randomized sham-controlled study of a tailored protocol 2017 a journal on accelerators, instrumentation and techniques applied to research in nuclear and atomic physics, materials science and related fields in physics Amsterdam (DE-627)ELV000874671 volume:1003 year:2021 day:1 month:07 pages:0 https://doi.org/10.1016/j.nima.2021.165319 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1003 2021 1 0701 0 |
| allfields_unstemmed |
10.1016/j.nima.2021.165319 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001379.pica (DE-627)ELV053864700 (ELSEVIER)S0168-9002(21)00303-X DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Tornago, M. verfasserin aut Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. 4D tracking Elsevier AC-coupled detectors Elsevier LGAD Elsevier Arcidiacono, R. oth Cartiglia, N. oth Costa, M. oth Ferrero, M. oth Mandurrino, M. oth Siviero, F. oth Sola, V. oth Staiano, A. oth Apresyan, A. oth Di Petrillo, K. oth Heller, R. oth Los, S. oth Borghi, G. oth Boscardin, M. oth Dalla Betta, G.-F. oth Ficorella, F. oth Pancheri, L. oth Paternoster, G. oth Sadrozinski, H. oth Seiden, A. oth Enthalten in North-Holland Publ. Co Ide, C.V. ELSEVIER The efficacy of EEG-biofeedback for acute pain management, a randomized sham-controlled study of a tailored protocol 2017 a journal on accelerators, instrumentation and techniques applied to research in nuclear and atomic physics, materials science and related fields in physics Amsterdam (DE-627)ELV000874671 volume:1003 year:2021 day:1 month:07 pages:0 https://doi.org/10.1016/j.nima.2021.165319 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1003 2021 1 0701 0 |
| allfieldsGer |
10.1016/j.nima.2021.165319 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001379.pica (DE-627)ELV053864700 (ELSEVIER)S0168-9002(21)00303-X DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Tornago, M. verfasserin aut Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. 4D tracking Elsevier AC-coupled detectors Elsevier LGAD Elsevier Arcidiacono, R. oth Cartiglia, N. oth Costa, M. oth Ferrero, M. oth Mandurrino, M. oth Siviero, F. oth Sola, V. oth Staiano, A. oth Apresyan, A. oth Di Petrillo, K. oth Heller, R. oth Los, S. oth Borghi, G. oth Boscardin, M. oth Dalla Betta, G.-F. oth Ficorella, F. oth Pancheri, L. oth Paternoster, G. oth Sadrozinski, H. oth Seiden, A. oth Enthalten in North-Holland Publ. Co Ide, C.V. ELSEVIER The efficacy of EEG-biofeedback for acute pain management, a randomized sham-controlled study of a tailored protocol 2017 a journal on accelerators, instrumentation and techniques applied to research in nuclear and atomic physics, materials science and related fields in physics Amsterdam (DE-627)ELV000874671 volume:1003 year:2021 day:1 month:07 pages:0 https://doi.org/10.1016/j.nima.2021.165319 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1003 2021 1 0701 0 |
| allfieldsSound |
10.1016/j.nima.2021.165319 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001379.pica (DE-627)ELV053864700 (ELSEVIER)S0168-9002(21)00303-X DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Tornago, M. verfasserin aut Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. 4D tracking Elsevier AC-coupled detectors Elsevier LGAD Elsevier Arcidiacono, R. oth Cartiglia, N. oth Costa, M. oth Ferrero, M. oth Mandurrino, M. oth Siviero, F. oth Sola, V. oth Staiano, A. oth Apresyan, A. oth Di Petrillo, K. oth Heller, R. oth Los, S. oth Borghi, G. oth Boscardin, M. oth Dalla Betta, G.-F. oth Ficorella, F. oth Pancheri, L. oth Paternoster, G. oth Sadrozinski, H. oth Seiden, A. oth Enthalten in North-Holland Publ. Co Ide, C.V. ELSEVIER The efficacy of EEG-biofeedback for acute pain management, a randomized sham-controlled study of a tailored protocol 2017 a journal on accelerators, instrumentation and techniques applied to research in nuclear and atomic physics, materials science and related fields in physics Amsterdam (DE-627)ELV000874671 volume:1003 year:2021 day:1 month:07 pages:0 https://doi.org/10.1016/j.nima.2021.165319 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1003 2021 1 0701 0 |
| language |
English |
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Resistive AC-Coupled Silicon Detectors: Principles of operation and first results from a combined analysis of beam test and laser data |
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This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. |
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This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. |
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This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain. |
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The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p silicon sensor based on the Low-Gain Avalanche Diode (LGAD) technology, where the n + implant has been designed to be resistive, and the read-out is obtained via AC-coupling. The truly innovative feature of RSD is that the signal generated by an impinging particle is shared isotropically among multiple read-out pads without the need for floating electrodes or an external magnetic field. Careful tuning of the coupling oxide thickness and the n + doping profile is at the basis of the successful functioning of this device. Several RSD matrices with different pad width-pitch geometries have been extensively tested with a laser setup in the Laboratory for Innovative Silicon Sensors in Torino, while a smaller set of devices have been tested at the Fermilab Test Beam Facility with a 120 GeV/c proton beam. The measured spatial resolution ranges between 2 . 5 μ m for 70–100 pad-pitch geometry and 17 μ m with 200–500 matrices, a factor of 10 better than what is achievable in binary read-out ( b i n s i z e ∕ 12 ). Beam test data show a temporal resolution of ∼ 40 ps for 200 μ m pitch devices, in line with the best performances of LGAD sensors at the same gain.</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">4D tracking</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">AC-coupled detectors</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">LGAD</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Arcidiacono, R.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Cartiglia, N.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Costa, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ferrero, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mandurrino, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Siviero, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sola, V.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Staiano, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Apresyan, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Di Petrillo, K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Heller, R.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Los, S.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Borghi, G.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Boscardin, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Dalla Betta, G.-F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ficorella, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Pancheri, L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Paternoster, G.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sadrozinski, H.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Seiden, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="n">North-Holland Publ. 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