The Heavy Photon Search beamline and its performance
The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt...
Ausführliche Beschreibung
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Baltzell, N [verfasserIn] |
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Artikel |
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Englisch |
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2016 |
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Enthalten in: Nuclear instruments & methods in physics research / A - Amsterdam : North-Holland Publ. Co., 1984, (2016) |
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| Übergeordnetes Werk: |
year:2016 |
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| DOI / URN: |
10.1016/j.nima.2017.03.061 |
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| 520 | |a The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. | ||
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| 700 | 1 | |a Egiyan, H |4 oth | |
| 700 | 1 | |a Ehrhart, M |4 oth | |
| 700 | 1 | |a Field, C |4 oth | |
| 700 | 1 | |a Freyberger, A |4 oth | |
| 700 | 1 | |a Girod, F. -X |4 oth | |
| 700 | 1 | |a Holtrop, M |4 oth | |
| 700 | 1 | |a Jaros, J |4 oth | |
| 700 | 1 | |a Kalicy, G |4 oth | |
| 700 | 1 | |a Maruyama, T |4 oth | |
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10.1016/j.nima.2017.03.061 doi PQ20171228 (DE-627)OLC199494823X (DE-599)GBVOLC199494823X (PRQ)a1104-1389606e52066029dfeebd8e035db982445a030820c33ed8f95e33b46853dee60 (KEY)0136675020160000000000000000heavyphotonsearchbeamlineanditsperformance DE-627 ger DE-627 rakwb eng 530 DE-600 UA 5680. AVZ rvk Baltzell, N verfasserin aut The Heavy Photon Search beamline and its performance 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Egiyan, H oth Ehrhart, M oth Field, C oth Freyberger, A oth Girod, F. -X oth Holtrop, M oth Jaros, J oth Kalicy, G oth Maruyama, T oth McKinnon, B oth Moffeit, K oth Nelson, T oth Odian, A oth Oriunno, M oth Paremuzyan, R oth Stepanyan, S oth Tiefenback, M oth Uemura, S oth Ungaro, M oth Vance, H oth Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 (2016) (DE-627)129862134 (DE-600)283627-0 (DE-576)015173461 0167-5087 nnns year:2016 http://dx.doi.org/10.1016/j.nima.2017.03.061 Volltext http://arxiv.org/abs/1612.07821 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_170 UA 5680. AR 2016 |
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10.1016/j.nima.2017.03.061 doi PQ20171228 (DE-627)OLC199494823X (DE-599)GBVOLC199494823X (PRQ)a1104-1389606e52066029dfeebd8e035db982445a030820c33ed8f95e33b46853dee60 (KEY)0136675020160000000000000000heavyphotonsearchbeamlineanditsperformance DE-627 ger DE-627 rakwb eng 530 DE-600 UA 5680. AVZ rvk Baltzell, N verfasserin aut The Heavy Photon Search beamline and its performance 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Egiyan, H oth Ehrhart, M oth Field, C oth Freyberger, A oth Girod, F. -X oth Holtrop, M oth Jaros, J oth Kalicy, G oth Maruyama, T oth McKinnon, B oth Moffeit, K oth Nelson, T oth Odian, A oth Oriunno, M oth Paremuzyan, R oth Stepanyan, S oth Tiefenback, M oth Uemura, S oth Ungaro, M oth Vance, H oth Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 (2016) (DE-627)129862134 (DE-600)283627-0 (DE-576)015173461 0167-5087 nnns year:2016 http://dx.doi.org/10.1016/j.nima.2017.03.061 Volltext http://arxiv.org/abs/1612.07821 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_170 UA 5680. AR 2016 |
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10.1016/j.nima.2017.03.061 doi PQ20171228 (DE-627)OLC199494823X (DE-599)GBVOLC199494823X (PRQ)a1104-1389606e52066029dfeebd8e035db982445a030820c33ed8f95e33b46853dee60 (KEY)0136675020160000000000000000heavyphotonsearchbeamlineanditsperformance DE-627 ger DE-627 rakwb eng 530 DE-600 UA 5680. AVZ rvk Baltzell, N verfasserin aut The Heavy Photon Search beamline and its performance 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Egiyan, H oth Ehrhart, M oth Field, C oth Freyberger, A oth Girod, F. -X oth Holtrop, M oth Jaros, J oth Kalicy, G oth Maruyama, T oth McKinnon, B oth Moffeit, K oth Nelson, T oth Odian, A oth Oriunno, M oth Paremuzyan, R oth Stepanyan, S oth Tiefenback, M oth Uemura, S oth Ungaro, M oth Vance, H oth Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 (2016) (DE-627)129862134 (DE-600)283627-0 (DE-576)015173461 0167-5087 nnns year:2016 http://dx.doi.org/10.1016/j.nima.2017.03.061 Volltext http://arxiv.org/abs/1612.07821 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_170 UA 5680. AR 2016 |
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10.1016/j.nima.2017.03.061 doi PQ20171228 (DE-627)OLC199494823X (DE-599)GBVOLC199494823X (PRQ)a1104-1389606e52066029dfeebd8e035db982445a030820c33ed8f95e33b46853dee60 (KEY)0136675020160000000000000000heavyphotonsearchbeamlineanditsperformance DE-627 ger DE-627 rakwb eng 530 DE-600 UA 5680. AVZ rvk Baltzell, N verfasserin aut The Heavy Photon Search beamline and its performance 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Egiyan, H oth Ehrhart, M oth Field, C oth Freyberger, A oth Girod, F. -X oth Holtrop, M oth Jaros, J oth Kalicy, G oth Maruyama, T oth McKinnon, B oth Moffeit, K oth Nelson, T oth Odian, A oth Oriunno, M oth Paremuzyan, R oth Stepanyan, S oth Tiefenback, M oth Uemura, S oth Ungaro, M oth Vance, H oth Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 (2016) (DE-627)129862134 (DE-600)283627-0 (DE-576)015173461 0167-5087 nnns year:2016 http://dx.doi.org/10.1016/j.nima.2017.03.061 Volltext http://arxiv.org/abs/1612.07821 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_170 UA 5680. AR 2016 |
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10.1016/j.nima.2017.03.061 doi PQ20171228 (DE-627)OLC199494823X (DE-599)GBVOLC199494823X (PRQ)a1104-1389606e52066029dfeebd8e035db982445a030820c33ed8f95e33b46853dee60 (KEY)0136675020160000000000000000heavyphotonsearchbeamlineanditsperformance DE-627 ger DE-627 rakwb eng 530 DE-600 UA 5680. AVZ rvk Baltzell, N verfasserin aut The Heavy Photon Search beamline and its performance 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. Instrumentation and Detectors Nuclear Experiment Physics High Energy Physics Experiment Egiyan, H oth Ehrhart, M oth Field, C oth Freyberger, A oth Girod, F. -X oth Holtrop, M oth Jaros, J oth Kalicy, G oth Maruyama, T oth McKinnon, B oth Moffeit, K oth Nelson, T oth Odian, A oth Oriunno, M oth Paremuzyan, R oth Stepanyan, S oth Tiefenback, M oth Uemura, S oth Ungaro, M oth Vance, H oth Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 (2016) (DE-627)129862134 (DE-600)283627-0 (DE-576)015173461 0167-5087 nnns year:2016 http://dx.doi.org/10.1016/j.nima.2017.03.061 Volltext http://arxiv.org/abs/1612.07821 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_70 GBV_ILN_170 UA 5680. AR 2016 |
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The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. |
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The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. |
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The Heavy Photon Search (HPS) is an experiment to search for a hidden sector photon, aka a heavy photon or dark photon, in fixed target electroproduction at the Thomas Jefferson National Accelerator Facility (JLab). The HPS experiment searches for the e^+e^- decay of the heavy photon with bump hunt and detached vertex strategies using a compact, large acceptance forward spectrometer, consisting of a silicon microstrip detector (SVT) for tracking and vertexing, and a PbWO_4 electromagnetic calorimeter for energy measurement and fast triggering. To achieve large acceptance and good vertexing resolution, the first layer of silicon detectors is placed just 10 cm downstream of the target with the sensor edges only 500 \mum above and below the beam. Placing the SVT in such close proximity to the beam puts stringent requirements on the beam profile and beam position stability. As part of an approved engineering run, HPS took data in 2015 and 2016 at 1.05 GeV and 2.3 GeV beam energies, respectively. This paper describes the beam line and its performance during that data taking. |
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