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Radiation damage in the LHCb Vertex Locator
The LHCb Vertex Locator (VELO) is a silicon strip detector designed to reconstruct charged particle trajectories and vertices produced at the LHCb interaction region. During the first two years of data collection, the 84 VELO sensors have been exposed to a range of fluences up to a maximum value of...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1748-0221/8/08/P08002 http://cds.cern.ch/record/1518829 |
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author | Affolder, A. Akiba, K. Alexander, M. Ali, S. Artuso, M. Benton, J. van Beuzekom, M. Bjornstad, P.M. Bogdanova, G. Borghi, S. Bowcock, T.J.V. Brown, H. Buytaert, J. Casse, G. Collins, P. De Capua, S. Dossett, D. Eklund, L. Farinelli, C. Garofoli, J. Gersabeck, M. Gershon, T. Gordon, H. Harrison, J. Heijne, V. Hennessy, K. Hutchcroft, D. Jans, E. John, M. Ketel, T. Lafferty, G. Latham, T. Leflat, A. Liles, M. Moran, D. Mous, I. Oblakowska-Mucha, A. Parkes, C. Patel, G.D. Redford, S. Reid, M.M. Rinnert, K. Rodrigues, E. Schiller, M. Szumlak, T. Thomas, C. Velthuis, J. Volkov, V. Webber, A.D. Whitehead, M. Zverev, E. |
author_facet | Affolder, A. Akiba, K. Alexander, M. Ali, S. Artuso, M. Benton, J. van Beuzekom, M. Bjornstad, P.M. Bogdanova, G. Borghi, S. Bowcock, T.J.V. Brown, H. Buytaert, J. Casse, G. Collins, P. De Capua, S. Dossett, D. Eklund, L. Farinelli, C. Garofoli, J. Gersabeck, M. Gershon, T. Gordon, H. Harrison, J. Heijne, V. Hennessy, K. Hutchcroft, D. Jans, E. John, M. Ketel, T. Lafferty, G. Latham, T. Leflat, A. Liles, M. Moran, D. Mous, I. Oblakowska-Mucha, A. Parkes, C. Patel, G.D. Redford, S. Reid, M.M. Rinnert, K. Rodrigues, E. Schiller, M. Szumlak, T. Thomas, C. Velthuis, J. Volkov, V. Webber, A.D. Whitehead, M. Zverev, E. |
author_sort | Affolder, A. |
collection | CERN |
description | The LHCb Vertex Locator (VELO) is a silicon strip detector designed to reconstruct charged particle trajectories and vertices produced at the LHCb interaction region. During the first two years of data collection, the 84 VELO sensors have been exposed to a range of fluences up to a maximum value of approximately $\rm{45 \times 10^{12}\,1\,MeV}$ neutron equivalent ($\rm{1\,MeV\,n_{eq}}$). At the operational sensor temperature of approximately $-7\,^{\circ}\rm{C}$, the average rate of sensor current increase is 18$\mu$ A per $\rm{fb^{-1}}$, in excellent agreement with predictions. The silicon effective bandgap has been determined using current versus temperature scan data after irradiation, with an average value of $E_{g}=1.16\pm0.03\pm0.04\,\rm{eV}$ obtained. The first observation of n-on-n sensor type inversion at the LHC has been made, occurring at a fluence of around $15 \times 10 ^{12}$ of $1\,\rm{MeV\,n_{eq}}$. The only n-on-p sensors in use at the LHC have also been studied. With an initial fluence of approximately $\rm{3 \times 10^{12}\,1\,MeV\,n_{eq}}$, a decrease in the Effective Depletion Voltage (EDV) of around 25\,V is observed, attributed to oxygen induced removal of boron interstitial sites. Following this initial decrease, the EDV increases at a comparable rate to the type inverted n-on-n type sensors, with rates of $(1.43\pm 0.16) \times 10 ^{-12}\,\rm{V} / \, 1 \, \rm{MeV\,n_{eq}}$ and $(1.35\pm 0.25) \times 10 ^{-12}\,\rm{V} / \, 1 \, \rm{MeV\,n_{eq}}$ measured for n-on-p and n-on-n type sensors, respectively. A reduction in the charge collection efficiency due to an unexpected effect involving the second metal layer readout lines is observed. |
id | cern-1518829 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-15188292022-08-10T20:27:41Zdoi:10.1088/1748-0221/8/08/P08002http://cds.cern.ch/record/1518829engAffolder, A.Akiba, K.Alexander, M.Ali, S.Artuso, M.Benton, J.van Beuzekom, M.Bjornstad, P.M.Bogdanova, G.Borghi, S.Bowcock, T.J.V.Brown, H.Buytaert, J.Casse, G.Collins, P.De Capua, S.Dossett, D.Eklund, L.Farinelli, C.Garofoli, J.Gersabeck, M.Gershon, T.Gordon, H.Harrison, J.Heijne, V.Hennessy, K.Hutchcroft, D.Jans, E.John, M.Ketel, T.Lafferty, G.Latham, T.Leflat, A.Liles, M.Moran, D.Mous, I.Oblakowska-Mucha, A.Parkes, C.Patel, G.D.Redford, S.Reid, M.M.Rinnert, K.Rodrigues, E.Schiller, M.Szumlak, T.Thomas, C.Velthuis, J.Volkov, V.Webber, A.D.Whitehead, M.Zverev, E.Radiation damage in the LHCb Vertex LocatorDetectors and Experimental TechniquesThe LHCb Vertex Locator (VELO) is a silicon strip detector designed to reconstruct charged particle trajectories and vertices produced at the LHCb interaction region. During the first two years of data collection, the 84 VELO sensors have been exposed to a range of fluences up to a maximum value of approximately $\rm{45 \times 10^{12}\,1\,MeV}$ neutron equivalent ($\rm{1\,MeV\,n_{eq}}$). At the operational sensor temperature of approximately $-7\,^{\circ}\rm{C}$, the average rate of sensor current increase is 18$\mu$ A per $\rm{fb^{-1}}$, in excellent agreement with predictions. The silicon effective bandgap has been determined using current versus temperature scan data after irradiation, with an average value of $E_{g}=1.16\pm0.03\pm0.04\,\rm{eV}$ obtained. The first observation of n-on-n sensor type inversion at the LHC has been made, occurring at a fluence of around $15 \times 10 ^{12}$ of $1\,\rm{MeV\,n_{eq}}$. The only n-on-p sensors in use at the LHC have also been studied. With an initial fluence of approximately $\rm{3 \times 10^{12}\,1\,MeV\,n_{eq}}$, a decrease in the Effective Depletion Voltage (EDV) of around 25\,V is observed, attributed to oxygen induced removal of boron interstitial sites. Following this initial decrease, the EDV increases at a comparable rate to the type inverted n-on-n type sensors, with rates of $(1.43\pm 0.16) \times 10 ^{-12}\,\rm{V} / \, 1 \, \rm{MeV\,n_{eq}}$ and $(1.35\pm 0.25) \times 10 ^{-12}\,\rm{V} / \, 1 \, \rm{MeV\,n_{eq}}$ measured for n-on-p and n-on-n type sensors, respectively. A reduction in the charge collection efficiency due to an unexpected effect involving the second metal layer readout lines is observed.The LHCb Vertex Locator (VELO) is a silicon strip detector designed toreconstruct charged particle trajectories and vertices produced at the LHCbinteraction region. During the first two years of data collection, the 84 VELOsensors have been exposed to a range of fluences up to a maximum value ofapproximately 45 × 1012 1 MeV neutron equivalent(1 MeV neq). At the operational sensor temperature of approximately−7 °C, the average rate of sensor current increase is18 μA per fb−1, in excellent agreement withpredictions. The silicon effective bandgap has been determined using currentversus temperature scan data after irradiation, with an average value ofEg = 1.16±0.03±0.04 eV obtained. The first observation ofn+-on-n sensor type inversion at the LHC has been made, occurring at a fluenceof around 15 × 1012 of 1 MeV neq. The only n+-on-psensors in use at the LHC have also been studied. With an initial fluence ofapproximately 3 × 1012 1 MeV neq, a decrease in theEffective Depletion Voltage (EDV) of around 25 V is observed. Following this initialdecrease, the EDV increases at a comparable rate to the typeinverted n+-on-n type sensors, with rates of (1.43±0.16) × 10−12 V/ 1 MeV neq and (1.35±0.25) × 10−12 V/ 1 MeV neq measured for n+-on-p andn+-on-n type sensors, respectively. A reduction in the charge collectionefficiency due to an unexpected effect involving the second metal layer readoutlines is observed.The LHCb Vertex Locator (VELO) is a silicon strip detector designed to reconstruct charged particle trajectories and vertices produced at the LHCb interaction region. During the first two years of data collection, the 84 VELO sensors have been exposed to a range of fluences up to a maximum value of approximately $\rm{45 \times 10^{12}\,1\,MeV}$ neutron equivalent ($\rm{1\,MeV\,n_{eq}}$). At the operational sensor temperature of approximately $-7\,^{\circ}\rm{C}$, the average rate of sensor current increase is $18\,\upmu\rm{A}$ per $\rm{fb^{-1}}$, in excellent agreement with predictions. The silicon effective bandgap has been determined using current versus temperature scan data after irradiation, with an average value of $E_{g}=1.16\pm0.03\pm0.04\,\rm{eV}$ obtained. The first observation of n-on-n sensor type inversion at the LHC has been made, occurring at a fluence of around $15 \times 10 ^{12}$ of $1\,\rm{MeV\,n_{eq}}$. The only n-on-p sensors in use at the LHC have also been studied. With an initial fluence of approximately $\rm{3 \times 10^{12}\,1\,MeV\,n_{eq}}$, a decrease in the Effective Depletion Voltage (EDV) of around 25\,V is observed, attributed to oxygen induced removal of boron interstitial sites. Following this initial decrease, the EDV increases at a comparable rate to the type inverted n-on-n type sensors, with rates of $(1.43\pm 0.16) \times 10 ^{-12}\,\rm{V} / \, 1 \, \rm{MeV\,n_{eq}}$ and $(1.35\pm 0.25) \times 10 ^{-12}\,\rm{V} / \, 1 \, \rm{MeV\,n_{eq}}$ measured for n-on-p and n-on-n type sensors, respectively. A reduction in the charge collection efficiency due to an unexpected effect involving the second metal layer readout lines is observed.CERN-LHCB-DP-2012-005arXiv:1302.5259CERN-LHCB-DP-2012-005LHCB-DP-2012-005oai:cds.cern.ch:15188292013-02-22 |
spellingShingle | Detectors and Experimental Techniques Affolder, A. Akiba, K. Alexander, M. Ali, S. Artuso, M. Benton, J. van Beuzekom, M. Bjornstad, P.M. Bogdanova, G. Borghi, S. Bowcock, T.J.V. Brown, H. Buytaert, J. Casse, G. Collins, P. De Capua, S. Dossett, D. Eklund, L. Farinelli, C. Garofoli, J. Gersabeck, M. Gershon, T. Gordon, H. Harrison, J. Heijne, V. Hennessy, K. Hutchcroft, D. Jans, E. John, M. Ketel, T. Lafferty, G. Latham, T. Leflat, A. Liles, M. Moran, D. Mous, I. Oblakowska-Mucha, A. Parkes, C. Patel, G.D. Redford, S. Reid, M.M. Rinnert, K. Rodrigues, E. Schiller, M. Szumlak, T. Thomas, C. Velthuis, J. Volkov, V. Webber, A.D. Whitehead, M. Zverev, E. Radiation damage in the LHCb Vertex Locator |
title | Radiation damage in the LHCb Vertex Locator |
title_full | Radiation damage in the LHCb Vertex Locator |
title_fullStr | Radiation damage in the LHCb Vertex Locator |
title_full_unstemmed | Radiation damage in the LHCb Vertex Locator |
title_short | Radiation damage in the LHCb Vertex Locator |
title_sort | radiation damage in the lhcb vertex locator |
topic | Detectors and Experimental Techniques |
url | https://dx.doi.org/10.1088/1748-0221/8/08/P08002 http://cds.cern.ch/record/1518829 |
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