Technical design of the phase I Mu3e experiment
The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We presen...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Arndt, K. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
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:1014 ; year:2021 ; day:21 ; month:10 ; pages:0 |
| Links: |
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| DOI / URN: |
10.1016/j.nima.2021.165679 |
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| Katalog-ID: |
ELV055379524 |
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| 520 | |a The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. | ||
| 520 | |a The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. | ||
| 650 | 7 | |a Muon decays |2 Elsevier | |
| 650 | 7 | |a Lepton flavour violation |2 Elsevier | |
| 650 | 7 | |a Scintillating fibres |2 Elsevier | |
| 650 | 7 | |a Scintillating tiles |2 Elsevier | |
| 650 | 7 | |a Monolithic pixel detector |2 Elsevier | |
| 700 | 1 | |a Augustin, H. |4 oth | |
| 700 | 1 | |a Baesso, P. |4 oth | |
| 700 | 1 | |a Berger, N. |4 oth | |
| 700 | 1 | |a Berg, F. |4 oth | |
| 700 | 1 | |a Betancourt, C. |4 oth | |
| 700 | 1 | |a Bortoletto, D. |4 oth | |
| 700 | 1 | |a Bravar, A. |4 oth | |
| 700 | 1 | |a Briggl, K. |4 oth | |
| 700 | 1 | |a vom Bruch, D. |4 oth | |
| 700 | 1 | |a Buonaura, A. |4 oth | |
| 700 | 1 | |a Cadoux, F. |4 oth | |
| 700 | 1 | |a Chavez Barajas, C. |4 oth | |
| 700 | 1 | |a Chen, H. |4 oth | |
| 700 | 1 | |a Clark, K. |4 oth | |
| 700 | 1 | |a Cooke, P. |4 oth | |
| 700 | 1 | |a Corrodi, S. |4 oth | |
| 700 | 1 | |a Damyanova, A. |4 oth | |
| 700 | 1 | |a Demets, Y. |4 oth | |
| 700 | 1 | |a Dittmeier, S. |4 oth | |
| 700 | 1 | |a Eckert, P. |4 oth | |
| 700 | 1 | |a Ehrler, F. |4 oth | |
| 700 | 1 | |a Fahrni, D. |4 oth | |
| 700 | 1 | |a Gagneur, S. |4 oth | |
| 700 | 1 | |a Gerritzen, L. |4 oth | |
| 700 | 1 | |a Goldstein, J. |4 oth | |
| 700 | 1 | |a Gottschalk, D. |4 oth | |
| 700 | 1 | |a Grab, C. |4 oth | |
| 700 | 1 | |a Gredig, R. |4 oth | |
| 700 | 1 | |a Groves, A. |4 oth | |
| 700 | 1 | |a Hammerich, J. |4 oth | |
| 700 | 1 | |a Hartenstein, U. |4 oth | |
| 700 | 1 | |a Hartmann, U. |4 oth | |
| 700 | 1 | |a Hayward, H. |4 oth | |
| 700 | 1 | |a Herkert, A. |4 oth | |
| 700 | 1 | |a Hesketh, G. |4 oth | |
| 700 | 1 | |a Hetzel, S. |4 oth | |
| 700 | 1 | |a Hildebrandt, M. |4 oth | |
| 700 | 1 | |a Hodge, Z. |4 oth | |
| 700 | 1 | |a Hofer, A. |4 oth | |
| 700 | 1 | |a Huang, Q.H. |4 oth | |
| 700 | 1 | |a Hughes, S. |4 oth | |
| 700 | 1 | |a Huth, L. |4 oth | |
| 700 | 1 | |a Immig, D.M. |4 oth | |
| 700 | 1 | |a Jones, T. |4 oth | |
| 700 | 1 | |a Jones, M. |4 oth | |
| 700 | 1 | |a Kästli, H.-C. |4 oth | |
| 700 | 1 | |a Köppel, M. |4 oth | |
| 700 | 1 | |a Kettle, P.-R. |4 oth | |
| 700 | 1 | |a Kiehn, M. |4 oth | |
| 700 | 1 | |a Kilani, S. |4 oth | |
| 700 | 1 | |a Klingenmeyer, H. |4 oth | |
| 700 | 1 | |a Knecht, A. |4 oth | |
| 700 | 1 | |a Knight, A. |4 oth | |
| 700 | 1 | |a Kotlinski, B. |4 oth | |
| 700 | 1 | |a Kozlinskiy, A. |4 oth | |
| 700 | 1 | |a Leys, R. |4 oth | |
| 700 | 1 | |a Lockwood, G. |4 oth | |
| 700 | 1 | |a Loreti, A. |4 oth | |
| 700 | 1 | |a La Marra, D. |4 oth | |
| 700 | 1 | |a Müller, M. |4 oth | |
| 700 | 1 | |a Meier, B. |4 oth | |
| 700 | 1 | |a Meier Aeschbacher, F. |4 oth | |
| 700 | 1 | |a Meneses, A. |4 oth | |
| 700 | 1 | |a Metodiev, K. |4 oth | |
| 700 | 1 | |a Mtchedlishvili, A. |4 oth | |
| 700 | 1 | |a Muley, S. |4 oth | |
| 700 | 1 | |a Munwes, Y. |4 oth | |
| 700 | 1 | |a Noehte, L.O.S. |4 oth | |
| 700 | 1 | |a Owen, P. |4 oth | |
| 700 | 1 | |a Papa, A. |4 oth | |
| 700 | 1 | |a Paraskevas, I. |4 oth | |
| 700 | 1 | |a Perić, I. |4 oth | |
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| 700 | 1 | |a Plackett, R. |4 oth | |
| 700 | 1 | |a Pohl, M. |4 oth | |
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| 700 | 1 | |a Rompotis, N. |4 oth | |
| 700 | 1 | |a Rudzki, T. |4 oth | |
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| 700 | 1 | |a Schöning, A. |4 oth | |
| 700 | 1 | |a Schimassek, R. |4 oth | |
| 700 | 1 | |a Schultz-Coulon, H.-C. |4 oth | |
| 700 | 1 | |a Serra, N. |4 oth | |
| 700 | 1 | |a Shen, W. |4 oth | |
| 700 | 1 | |a Shipsey, I. |4 oth | |
| 700 | 1 | |a Shrestha, S. |4 oth | |
| 700 | 1 | |a Steinkamp, O. |4 oth | |
| 700 | 1 | |a Stoykov, A. |4 oth | |
| 700 | 1 | |a Straumann, U. |4 oth | |
| 700 | 1 | |a Streuli, S. |4 oth | |
| 700 | 1 | |a Stumpf, K. |4 oth | |
| 700 | 1 | |a Tata, N. |4 oth | |
| 700 | 1 | |a Velthuis, J. |4 oth | |
| 700 | 1 | |a Vigani, L. |4 oth | |
| 700 | 1 | |a Vilella-Figueras, E. |4 oth | |
| 700 | 1 | |a Vossebeld, J. |4 oth | |
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| 700 | 1 | |a Wasili, A. |4 oth | |
| 700 | 1 | |a Wauters, F. |4 oth | |
| 700 | 1 | |a Weber, A. |4 oth | |
| 700 | 1 | |a Wiedner, D. |4 oth | |
| 700 | 1 | |a Windelband, B. |4 oth | |
| 700 | 1 | |a Zhong, T. |4 oth | |
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10.1016/j.nima.2021.165679 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001518.pica (DE-627)ELV055379524 (ELSEVIER)S0168-9002(21)00664-1 DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Arndt, K. verfasserin aut Technical design of the phase I Mu3e experiment 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. Muon decays Elsevier Lepton flavour violation Elsevier Scintillating fibres Elsevier Scintillating tiles Elsevier Monolithic pixel detector Elsevier Augustin, H. oth Baesso, P. oth Berger, N. oth Berg, F. oth Betancourt, C. oth Bortoletto, D. oth Bravar, A. oth Briggl, K. oth vom Bruch, D. oth Buonaura, A. oth Cadoux, F. oth Chavez Barajas, C. oth Chen, H. oth Clark, K. oth Cooke, P. oth Corrodi, S. oth Damyanova, A. oth Demets, Y. oth Dittmeier, S. oth Eckert, P. oth Ehrler, F. oth Fahrni, D. oth Gagneur, S. oth Gerritzen, L. oth Goldstein, J. oth Gottschalk, D. oth Grab, C. oth Gredig, R. oth Groves, A. oth Hammerich, J. oth Hartenstein, U. oth Hartmann, U. oth Hayward, H. oth Herkert, A. oth Hesketh, G. oth Hetzel, S. oth Hildebrandt, M. oth Hodge, Z. oth Hofer, A. oth Huang, Q.H. oth Hughes, S. oth Huth, L. oth Immig, D.M. oth Jones, T. oth Jones, M. oth Kästli, H.-C. oth Köppel, M. oth Kettle, P.-R. oth Kiehn, M. oth Kilani, S. oth Klingenmeyer, H. oth Knecht, A. oth Knight, A. oth Kotlinski, B. oth Kozlinskiy, A. oth Leys, R. oth Lockwood, G. oth Loreti, A. oth La Marra, D. oth Müller, M. oth Meier, B. oth Meier Aeschbacher, F. oth Meneses, A. oth Metodiev, K. oth Mtchedlishvili, A. oth Muley, S. oth Munwes, Y. oth Noehte, L.O.S. oth Owen, P. oth Papa, A. oth Paraskevas, I. oth Perić, I. oth Perrevoort, A.-K. oth Plackett, R. oth Pohl, M. oth Ritt, S. oth Robmann, P. oth Rompotis, N. oth Rudzki, T. oth Rutar, G. oth Schöning, A. oth Schimassek, R. oth Schultz-Coulon, H.-C. oth Serra, N. oth Shen, W. oth Shipsey, I. oth Shrestha, S. oth Steinkamp, O. oth Stoykov, A. oth Straumann, U. oth Streuli, S. oth Stumpf, K. oth Tata, N. oth Velthuis, J. oth Vigani, L. oth Vilella-Figueras, E. oth Vossebeld, J. oth Wallny, R. oth Wasili, A. oth Wauters, F. oth Weber, A. oth Wiedner, D. oth Windelband, B. oth Zhong, T. 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:1014 year:2021 day:21 month:10 pages:0 https://doi.org/10.1016/j.nima.2021.165679 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1014 2021 21 1021 0 |
| spelling |
10.1016/j.nima.2021.165679 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001518.pica (DE-627)ELV055379524 (ELSEVIER)S0168-9002(21)00664-1 DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Arndt, K. verfasserin aut Technical design of the phase I Mu3e experiment 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. Muon decays Elsevier Lepton flavour violation Elsevier Scintillating fibres Elsevier Scintillating tiles Elsevier Monolithic pixel detector Elsevier Augustin, H. oth Baesso, P. oth Berger, N. oth Berg, F. oth Betancourt, C. oth Bortoletto, D. oth Bravar, A. oth Briggl, K. oth vom Bruch, D. oth Buonaura, A. oth Cadoux, F. oth Chavez Barajas, C. oth Chen, H. oth Clark, K. oth Cooke, P. oth Corrodi, S. oth Damyanova, A. oth Demets, Y. oth Dittmeier, S. oth Eckert, P. oth Ehrler, F. oth Fahrni, D. oth Gagneur, S. oth Gerritzen, L. oth Goldstein, J. oth Gottschalk, D. oth Grab, C. oth Gredig, R. oth Groves, A. oth Hammerich, J. oth Hartenstein, U. oth Hartmann, U. oth Hayward, H. oth Herkert, A. oth Hesketh, G. oth Hetzel, S. oth Hildebrandt, M. oth Hodge, Z. oth Hofer, A. oth Huang, Q.H. oth Hughes, S. oth Huth, L. oth Immig, D.M. oth Jones, T. oth Jones, M. oth Kästli, H.-C. oth Köppel, M. oth Kettle, P.-R. oth Kiehn, M. oth Kilani, S. oth Klingenmeyer, H. oth Knecht, A. oth Knight, A. oth Kotlinski, B. oth Kozlinskiy, A. oth Leys, R. oth Lockwood, G. oth Loreti, A. oth La Marra, D. oth Müller, M. oth Meier, B. oth Meier Aeschbacher, F. oth Meneses, A. oth Metodiev, K. oth Mtchedlishvili, A. oth Muley, S. oth Munwes, Y. oth Noehte, L.O.S. oth Owen, P. oth Papa, A. oth Paraskevas, I. oth Perić, I. oth Perrevoort, A.-K. oth Plackett, R. oth Pohl, M. oth Ritt, S. oth Robmann, P. oth Rompotis, N. oth Rudzki, T. oth Rutar, G. oth Schöning, A. oth Schimassek, R. oth Schultz-Coulon, H.-C. oth Serra, N. oth Shen, W. oth Shipsey, I. oth Shrestha, S. oth Steinkamp, O. oth Stoykov, A. oth Straumann, U. oth Streuli, S. oth Stumpf, K. oth Tata, N. oth Velthuis, J. oth Vigani, L. oth Vilella-Figueras, E. oth Vossebeld, J. oth Wallny, R. oth Wasili, A. oth Wauters, F. oth Weber, A. oth Wiedner, D. oth Windelband, B. oth Zhong, T. 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:1014 year:2021 day:21 month:10 pages:0 https://doi.org/10.1016/j.nima.2021.165679 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1014 2021 21 1021 0 |
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10.1016/j.nima.2021.165679 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001518.pica (DE-627)ELV055379524 (ELSEVIER)S0168-9002(21)00664-1 DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Arndt, K. verfasserin aut Technical design of the phase I Mu3e experiment 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. Muon decays Elsevier Lepton flavour violation Elsevier Scintillating fibres Elsevier Scintillating tiles Elsevier Monolithic pixel detector Elsevier Augustin, H. oth Baesso, P. oth Berger, N. oth Berg, F. oth Betancourt, C. oth Bortoletto, D. oth Bravar, A. oth Briggl, K. oth vom Bruch, D. oth Buonaura, A. oth Cadoux, F. oth Chavez Barajas, C. oth Chen, H. oth Clark, K. oth Cooke, P. oth Corrodi, S. oth Damyanova, A. oth Demets, Y. oth Dittmeier, S. oth Eckert, P. oth Ehrler, F. oth Fahrni, D. oth Gagneur, S. oth Gerritzen, L. oth Goldstein, J. oth Gottschalk, D. oth Grab, C. oth Gredig, R. oth Groves, A. oth Hammerich, J. oth Hartenstein, U. oth Hartmann, U. oth Hayward, H. oth Herkert, A. oth Hesketh, G. oth Hetzel, S. oth Hildebrandt, M. oth Hodge, Z. oth Hofer, A. oth Huang, Q.H. oth Hughes, S. oth Huth, L. oth Immig, D.M. oth Jones, T. oth Jones, M. oth Kästli, H.-C. oth Köppel, M. oth Kettle, P.-R. oth Kiehn, M. oth Kilani, S. oth Klingenmeyer, H. oth Knecht, A. oth Knight, A. oth Kotlinski, B. oth Kozlinskiy, A. oth Leys, R. oth Lockwood, G. oth Loreti, A. oth La Marra, D. oth Müller, M. oth Meier, B. oth Meier Aeschbacher, F. oth Meneses, A. oth Metodiev, K. oth Mtchedlishvili, A. oth Muley, S. oth Munwes, Y. oth Noehte, L.O.S. oth Owen, P. oth Papa, A. oth Paraskevas, I. oth Perić, I. oth Perrevoort, A.-K. oth Plackett, R. oth Pohl, M. oth Ritt, S. oth Robmann, P. oth Rompotis, N. oth Rudzki, T. oth Rutar, G. oth Schöning, A. oth Schimassek, R. oth Schultz-Coulon, H.-C. oth Serra, N. oth Shen, W. oth Shipsey, I. oth Shrestha, S. oth Steinkamp, O. oth Stoykov, A. oth Straumann, U. oth Streuli, S. oth Stumpf, K. oth Tata, N. oth Velthuis, J. oth Vigani, L. oth Vilella-Figueras, E. oth Vossebeld, J. oth Wallny, R. oth Wasili, A. oth Wauters, F. oth Weber, A. oth Wiedner, D. oth Windelband, B. oth Zhong, T. 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:1014 year:2021 day:21 month:10 pages:0 https://doi.org/10.1016/j.nima.2021.165679 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1014 2021 21 1021 0 |
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10.1016/j.nima.2021.165679 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001518.pica (DE-627)ELV055379524 (ELSEVIER)S0168-9002(21)00664-1 DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Arndt, K. verfasserin aut Technical design of the phase I Mu3e experiment 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. Muon decays Elsevier Lepton flavour violation Elsevier Scintillating fibres Elsevier Scintillating tiles Elsevier Monolithic pixel detector Elsevier Augustin, H. oth Baesso, P. oth Berger, N. oth Berg, F. oth Betancourt, C. oth Bortoletto, D. oth Bravar, A. oth Briggl, K. oth vom Bruch, D. oth Buonaura, A. oth Cadoux, F. oth Chavez Barajas, C. oth Chen, H. oth Clark, K. oth Cooke, P. oth Corrodi, S. oth Damyanova, A. oth Demets, Y. oth Dittmeier, S. oth Eckert, P. oth Ehrler, F. oth Fahrni, D. oth Gagneur, S. oth Gerritzen, L. oth Goldstein, J. oth Gottschalk, D. oth Grab, C. oth Gredig, R. oth Groves, A. oth Hammerich, J. oth Hartenstein, U. oth Hartmann, U. oth Hayward, H. oth Herkert, A. oth Hesketh, G. oth Hetzel, S. oth Hildebrandt, M. oth Hodge, Z. oth Hofer, A. oth Huang, Q.H. oth Hughes, S. oth Huth, L. oth Immig, D.M. oth Jones, T. oth Jones, M. oth Kästli, H.-C. oth Köppel, M. oth Kettle, P.-R. oth Kiehn, M. oth Kilani, S. oth Klingenmeyer, H. oth Knecht, A. oth Knight, A. oth Kotlinski, B. oth Kozlinskiy, A. oth Leys, R. oth Lockwood, G. oth Loreti, A. oth La Marra, D. oth Müller, M. oth Meier, B. oth Meier Aeschbacher, F. oth Meneses, A. oth Metodiev, K. oth Mtchedlishvili, A. oth Muley, S. oth Munwes, Y. oth Noehte, L.O.S. oth Owen, P. oth Papa, A. oth Paraskevas, I. oth Perić, I. oth Perrevoort, A.-K. oth Plackett, R. oth Pohl, M. oth Ritt, S. oth Robmann, P. oth Rompotis, N. oth Rudzki, T. oth Rutar, G. oth Schöning, A. oth Schimassek, R. oth Schultz-Coulon, H.-C. oth Serra, N. oth Shen, W. oth Shipsey, I. oth Shrestha, S. oth Steinkamp, O. oth Stoykov, A. oth Straumann, U. oth Streuli, S. oth Stumpf, K. oth Tata, N. oth Velthuis, J. oth Vigani, L. oth Vilella-Figueras, E. oth Vossebeld, J. oth Wallny, R. oth Wasili, A. oth Wauters, F. oth Weber, A. oth Wiedner, D. oth Windelband, B. oth Zhong, T. 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:1014 year:2021 day:21 month:10 pages:0 https://doi.org/10.1016/j.nima.2021.165679 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1014 2021 21 1021 0 |
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10.1016/j.nima.2021.165679 doi /cbs_pica/cbs_olc/import_discovery/elsevier/einzuspielen/GBV00000000001518.pica (DE-627)ELV055379524 (ELSEVIER)S0168-9002(21)00664-1 DE-627 ger DE-627 rakwb eng 610 VZ 44.90 bkl Arndt, K. verfasserin aut Technical design of the phase I Mu3e experiment 2021transfer abstract nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. Muon decays Elsevier Lepton flavour violation Elsevier Scintillating fibres Elsevier Scintillating tiles Elsevier Monolithic pixel detector Elsevier Augustin, H. oth Baesso, P. oth Berger, N. oth Berg, F. oth Betancourt, C. oth Bortoletto, D. oth Bravar, A. oth Briggl, K. oth vom Bruch, D. oth Buonaura, A. oth Cadoux, F. oth Chavez Barajas, C. oth Chen, H. oth Clark, K. oth Cooke, P. oth Corrodi, S. oth Damyanova, A. oth Demets, Y. oth Dittmeier, S. oth Eckert, P. oth Ehrler, F. oth Fahrni, D. oth Gagneur, S. oth Gerritzen, L. oth Goldstein, J. oth Gottschalk, D. oth Grab, C. oth Gredig, R. oth Groves, A. oth Hammerich, J. oth Hartenstein, U. oth Hartmann, U. oth Hayward, H. oth Herkert, A. oth Hesketh, G. oth Hetzel, S. oth Hildebrandt, M. oth Hodge, Z. oth Hofer, A. oth Huang, Q.H. oth Hughes, S. oth Huth, L. oth Immig, D.M. oth Jones, T. oth Jones, M. oth Kästli, H.-C. oth Köppel, M. oth Kettle, P.-R. oth Kiehn, M. oth Kilani, S. oth Klingenmeyer, H. oth Knecht, A. oth Knight, A. oth Kotlinski, B. oth Kozlinskiy, A. oth Leys, R. oth Lockwood, G. oth Loreti, A. oth La Marra, D. oth Müller, M. oth Meier, B. oth Meier Aeschbacher, F. oth Meneses, A. oth Metodiev, K. oth Mtchedlishvili, A. oth Muley, S. oth Munwes, Y. oth Noehte, L.O.S. oth Owen, P. oth Papa, A. oth Paraskevas, I. oth Perić, I. oth Perrevoort, A.-K. oth Plackett, R. oth Pohl, M. oth Ritt, S. oth Robmann, P. oth Rompotis, N. oth Rudzki, T. oth Rutar, G. oth Schöning, A. oth Schimassek, R. oth Schultz-Coulon, H.-C. oth Serra, N. oth Shen, W. oth Shipsey, I. oth Shrestha, S. oth Steinkamp, O. oth Stoykov, A. oth Straumann, U. oth Streuli, S. oth Stumpf, K. oth Tata, N. oth Velthuis, J. oth Vigani, L. oth Vilella-Figueras, E. oth Vossebeld, J. oth Wallny, R. oth Wasili, A. oth Wauters, F. oth Weber, A. oth Wiedner, D. oth Windelband, B. oth Zhong, T. 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:1014 year:2021 day:21 month:10 pages:0 https://doi.org/10.1016/j.nima.2021.165679 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 44.90 Neurologie VZ AR 1014 2021 21 1021 0 |
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Technical design of the phase I Mu3e experiment |
| abstract |
The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. |
| abstractGer |
The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. |
| abstract_unstemmed |
The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ → e e e at branching fractions above 1 0 − 16 . A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2 ⋅ 1 0 − 15 . We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 1 0 8 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements. |
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| title_short |
Technical design of the phase I Mu3e experiment |
| url |
https://doi.org/10.1016/j.nima.2021.165679 |
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Augustin, H. Baesso, P. Berger, N. Berg, F. Betancourt, C. Bortoletto, D. Bravar, A. Briggl, K. vom Bruch, D. Buonaura, A. Cadoux, F. Chavez Barajas, C. Chen, H. Clark, K. Cooke, P. Corrodi, S. Damyanova, A. Demets, Y. Dittmeier, S. Eckert, P. Ehrler, F. Fahrni, D. Gagneur, S. Gerritzen, L. Goldstein, J. Gottschalk, D. Grab, C. Gredig, R. Groves, A. Hammerich, J. Hartenstein, U. Hartmann, U. Hayward, H. Herkert, A. Hesketh, G. Hetzel, S. Hildebrandt, M. Hodge, Z. Hofer, A. Huang, Q.H. Hughes, S. Huth, L. Immig, D.M. Jones, T. Jones, M. Kästli, H.-C. Köppel, M. Kettle, P.-R. Kiehn, M. Kilani, S. Klingenmeyer, H. Knecht, A. Knight, A. Kotlinski, B. Kozlinskiy, A. Leys, R. Lockwood, G. Loreti, A. La Marra, D. Müller, M. Meier, B. Meier Aeschbacher, F. Meneses, A. Metodiev, K. Mtchedlishvili, A. Muley, S. Munwes, Y. Noehte, L.O.S. Owen, P. Papa, A. Paraskevas, I. Perić, I. Perrevoort, A.-K. Plackett, R. Pohl, M. Ritt, S. Robmann, P. Rompotis, N. Rudzki, T. Rutar, G. Schöning, A. Schimassek, R. Schultz-Coulon, H.-C. Serra, N. Shen, W. Shipsey, I. Shrestha, S. Steinkamp, O. Stoykov, A. Straumann, U. Streuli, S. Stumpf, K. Tata, N. Velthuis, J. Vigani, L. Vilella-Figueras, E. Vossebeld, J. Wallny, R. Wasili, A. Wauters, F. Weber, A. Wiedner, D. Windelband, B. Zhong, T. |
| author2Str |
Augustin, H. Baesso, P. Berger, N. Berg, F. Betancourt, C. Bortoletto, D. Bravar, A. Briggl, K. vom Bruch, D. Buonaura, A. Cadoux, F. Chavez Barajas, C. Chen, H. Clark, K. Cooke, P. Corrodi, S. Damyanova, A. Demets, Y. Dittmeier, S. Eckert, P. Ehrler, F. Fahrni, D. Gagneur, S. Gerritzen, L. Goldstein, J. Gottschalk, D. Grab, C. Gredig, R. Groves, A. Hammerich, J. Hartenstein, U. Hartmann, U. Hayward, H. Herkert, A. Hesketh, G. Hetzel, S. Hildebrandt, M. Hodge, Z. Hofer, A. Huang, Q.H. Hughes, S. Huth, L. Immig, D.M. Jones, T. Jones, M. Kästli, H.-C. Köppel, M. Kettle, P.-R. Kiehn, M. Kilani, S. Klingenmeyer, H. Knecht, A. Knight, A. Kotlinski, B. Kozlinskiy, A. Leys, R. Lockwood, G. Loreti, A. La Marra, D. Müller, M. Meier, B. Meier Aeschbacher, F. Meneses, A. Metodiev, K. Mtchedlishvili, A. Muley, S. Munwes, Y. Noehte, L.O.S. Owen, P. Papa, A. Paraskevas, I. Perić, I. Perrevoort, A.-K. Plackett, R. Pohl, M. Ritt, S. Robmann, P. Rompotis, N. Rudzki, T. Rutar, G. Schöning, A. Schimassek, R. Schultz-Coulon, H.-C. Serra, N. Shen, W. Shipsey, I. Shrestha, S. Steinkamp, O. Stoykov, A. Straumann, U. Streuli, S. Stumpf, K. Tata, N. Velthuis, J. Vigani, L. Vilella-Figueras, E. Vossebeld, J. Wallny, R. Wasili, A. Wauters, F. Weber, A. Wiedner, D. Windelband, B. Zhong, T. |
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| doi_str |
10.1016/j.nima.2021.165679 |
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