The ${Q^{p}_{\rm Weak}}$ experiment
Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measur...
Ausführliche Beschreibung
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| Autor*in: |
Androic, D. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media Dordrecht 2013 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Springer Netherlands, 1975, 214(2013), 1-3 vom: 13. Feb., Seite 21-30 |
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| Übergeordnetes Werk: |
volume:214 ; year:2013 ; number:1-3 ; day:13 ; month:02 ; pages:21-30 |
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| DOI / URN: |
10.1007/s10751-013-0782-0 |
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| Katalog-ID: |
OLC2076420703 |
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| 520 | |a Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. | ||
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10.1007/s10751-013-0782-0 doi (DE-627)OLC2076420703 (DE-He213)s10751-013-0782-0-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Androic, D. verfasserin aut The ${Q^{p}_{\rm Weak}}$ experiment 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media Dordrecht 2013 Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. Standard model Weak charge Parity violation Electron scattering New physics Armstrong, D. S. aut Asaturyan, A. aut Averett, T. aut Balewski, J. aut Beaufait, J. aut Beminiwattha, R. S. aut Benesch, J. aut Benmokhtar, F. aut Birchall, J. aut Carlini, R. D. aut Cornejo, J. C. aut Covrig, S. aut Dalton, M. M. aut Davis, C. A. aut Deconinck, W. aut Diefenbach, J. aut Dow, K. aut Dowd, J. F. aut Dunne, J. A. aut Dutta, D. aut Duvall, W. S. aut Elaasar, M. aut Falk, W. R. aut Finn, J. M. aut Forest, T. aut Gaskell, D. aut Gericke, M. T. W. aut Grames, J. aut Gray, V. M. aut Grimm, K. aut Guo, F. aut Hoskins, J. R. aut Johnston, K. aut Jones, D. aut Jones, M. aut Jones, R. aut Kargiantoulakis, M. aut King, P. M. aut Korkmaz, E. aut Kowalski, S. aut Leacock, J. aut Leckey, J. aut Lee, A. R. aut Lee, J. H. aut Lee, L. aut MacEwan, S. aut Mack, D. aut Magee, J. A. aut Mahurin, R. aut Mammei, J. aut Martin, J. aut McHugh, M. aut Meekins, D. aut Mei, J. aut Michaels, R. aut Micherdzinska, A. aut Myers, K. E. aut Mkrtchyan, A. aut Mkrtchyan, H. aut Narayan, A. aut Ndukum, L. Z. aut Nelyubin, V. aut Nuruzzaman, N. aut van Oers, W. T. H aut Opper, A. K. aut Page, S. A. aut Pan, J. aut Paschke, K. aut Phillips, S. K. aut Pitt, M. L. aut Poelker, M. aut Rajotte, J. F. aut Ramsay, W. D. aut Roche, J. aut Sawatzky, B. aut Seva, T. aut Shabestari, M. H. aut Silwal, R. aut Simicevic, N. aut Smith, G. aut Solvignon, P. aut Spayde, D. T. aut Subedi, A. aut Subedi, R. aut Suleiman, R. aut Tadevosyan, V. aut Tobias, W. A. aut Tvaskis, V. aut Waidyawansa, B. aut Wang, P. aut Wells, S. P. aut Wood, S. A. aut Yang, S. aut Young, R. D. aut Zhamkochyan, S. aut Zou, D. aut Enthalten in Hyperfine interactions Springer Netherlands, 1975 214(2013), 1-3 vom: 13. Feb., Seite 21-30 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:214 year:2013 number:1-3 day:13 month:02 pages:21-30 https://doi.org/10.1007/s10751-013-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2279 33.00 VZ AR 214 2013 1-3 13 02 21-30 |
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10.1007/s10751-013-0782-0 doi (DE-627)OLC2076420703 (DE-He213)s10751-013-0782-0-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Androic, D. verfasserin aut The ${Q^{p}_{\rm Weak}}$ experiment 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media Dordrecht 2013 Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. Standard model Weak charge Parity violation Electron scattering New physics Armstrong, D. S. aut Asaturyan, A. aut Averett, T. aut Balewski, J. aut Beaufait, J. aut Beminiwattha, R. S. aut Benesch, J. aut Benmokhtar, F. aut Birchall, J. aut Carlini, R. D. aut Cornejo, J. C. aut Covrig, S. aut Dalton, M. M. aut Davis, C. A. aut Deconinck, W. aut Diefenbach, J. aut Dow, K. aut Dowd, J. F. aut Dunne, J. A. aut Dutta, D. aut Duvall, W. S. aut Elaasar, M. aut Falk, W. R. aut Finn, J. M. aut Forest, T. aut Gaskell, D. aut Gericke, M. T. W. aut Grames, J. aut Gray, V. M. aut Grimm, K. aut Guo, F. aut Hoskins, J. R. aut Johnston, K. aut Jones, D. aut Jones, M. aut Jones, R. aut Kargiantoulakis, M. aut King, P. M. aut Korkmaz, E. aut Kowalski, S. aut Leacock, J. aut Leckey, J. aut Lee, A. R. aut Lee, J. H. aut Lee, L. aut MacEwan, S. aut Mack, D. aut Magee, J. A. aut Mahurin, R. aut Mammei, J. aut Martin, J. aut McHugh, M. aut Meekins, D. aut Mei, J. aut Michaels, R. aut Micherdzinska, A. aut Myers, K. E. aut Mkrtchyan, A. aut Mkrtchyan, H. aut Narayan, A. aut Ndukum, L. Z. aut Nelyubin, V. aut Nuruzzaman, N. aut van Oers, W. T. H aut Opper, A. K. aut Page, S. A. aut Pan, J. aut Paschke, K. aut Phillips, S. K. aut Pitt, M. L. aut Poelker, M. aut Rajotte, J. F. aut Ramsay, W. D. aut Roche, J. aut Sawatzky, B. aut Seva, T. aut Shabestari, M. H. aut Silwal, R. aut Simicevic, N. aut Smith, G. aut Solvignon, P. aut Spayde, D. T. aut Subedi, A. aut Subedi, R. aut Suleiman, R. aut Tadevosyan, V. aut Tobias, W. A. aut Tvaskis, V. aut Waidyawansa, B. aut Wang, P. aut Wells, S. P. aut Wood, S. A. aut Yang, S. aut Young, R. D. aut Zhamkochyan, S. aut Zou, D. aut Enthalten in Hyperfine interactions Springer Netherlands, 1975 214(2013), 1-3 vom: 13. Feb., Seite 21-30 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:214 year:2013 number:1-3 day:13 month:02 pages:21-30 https://doi.org/10.1007/s10751-013-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2279 33.00 VZ AR 214 2013 1-3 13 02 21-30 |
| allfields_unstemmed |
10.1007/s10751-013-0782-0 doi (DE-627)OLC2076420703 (DE-He213)s10751-013-0782-0-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Androic, D. verfasserin aut The ${Q^{p}_{\rm Weak}}$ experiment 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media Dordrecht 2013 Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. Standard model Weak charge Parity violation Electron scattering New physics Armstrong, D. S. aut Asaturyan, A. aut Averett, T. aut Balewski, J. aut Beaufait, J. aut Beminiwattha, R. S. aut Benesch, J. aut Benmokhtar, F. aut Birchall, J. aut Carlini, R. D. aut Cornejo, J. C. aut Covrig, S. aut Dalton, M. M. aut Davis, C. A. aut Deconinck, W. aut Diefenbach, J. aut Dow, K. aut Dowd, J. F. aut Dunne, J. A. aut Dutta, D. aut Duvall, W. S. aut Elaasar, M. aut Falk, W. R. aut Finn, J. M. aut Forest, T. aut Gaskell, D. aut Gericke, M. T. W. aut Grames, J. aut Gray, V. M. aut Grimm, K. aut Guo, F. aut Hoskins, J. R. aut Johnston, K. aut Jones, D. aut Jones, M. aut Jones, R. aut Kargiantoulakis, M. aut King, P. M. aut Korkmaz, E. aut Kowalski, S. aut Leacock, J. aut Leckey, J. aut Lee, A. R. aut Lee, J. H. aut Lee, L. aut MacEwan, S. aut Mack, D. aut Magee, J. A. aut Mahurin, R. aut Mammei, J. aut Martin, J. aut McHugh, M. aut Meekins, D. aut Mei, J. aut Michaels, R. aut Micherdzinska, A. aut Myers, K. E. aut Mkrtchyan, A. aut Mkrtchyan, H. aut Narayan, A. aut Ndukum, L. Z. aut Nelyubin, V. aut Nuruzzaman, N. aut van Oers, W. T. H aut Opper, A. K. aut Page, S. A. aut Pan, J. aut Paschke, K. aut Phillips, S. K. aut Pitt, M. L. aut Poelker, M. aut Rajotte, J. F. aut Ramsay, W. D. aut Roche, J. aut Sawatzky, B. aut Seva, T. aut Shabestari, M. H. aut Silwal, R. aut Simicevic, N. aut Smith, G. aut Solvignon, P. aut Spayde, D. T. aut Subedi, A. aut Subedi, R. aut Suleiman, R. aut Tadevosyan, V. aut Tobias, W. A. aut Tvaskis, V. aut Waidyawansa, B. aut Wang, P. aut Wells, S. P. aut Wood, S. A. aut Yang, S. aut Young, R. D. aut Zhamkochyan, S. aut Zou, D. aut Enthalten in Hyperfine interactions Springer Netherlands, 1975 214(2013), 1-3 vom: 13. Feb., Seite 21-30 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:214 year:2013 number:1-3 day:13 month:02 pages:21-30 https://doi.org/10.1007/s10751-013-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2279 33.00 VZ AR 214 2013 1-3 13 02 21-30 |
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10.1007/s10751-013-0782-0 doi (DE-627)OLC2076420703 (DE-He213)s10751-013-0782-0-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Androic, D. verfasserin aut The ${Q^{p}_{\rm Weak}}$ experiment 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media Dordrecht 2013 Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. Standard model Weak charge Parity violation Electron scattering New physics Armstrong, D. S. aut Asaturyan, A. aut Averett, T. aut Balewski, J. aut Beaufait, J. aut Beminiwattha, R. S. aut Benesch, J. aut Benmokhtar, F. aut Birchall, J. aut Carlini, R. D. aut Cornejo, J. C. aut Covrig, S. aut Dalton, M. M. aut Davis, C. A. aut Deconinck, W. aut Diefenbach, J. aut Dow, K. aut Dowd, J. F. aut Dunne, J. A. aut Dutta, D. aut Duvall, W. S. aut Elaasar, M. aut Falk, W. R. aut Finn, J. M. aut Forest, T. aut Gaskell, D. aut Gericke, M. T. W. aut Grames, J. aut Gray, V. M. aut Grimm, K. aut Guo, F. aut Hoskins, J. R. aut Johnston, K. aut Jones, D. aut Jones, M. aut Jones, R. aut Kargiantoulakis, M. aut King, P. M. aut Korkmaz, E. aut Kowalski, S. aut Leacock, J. aut Leckey, J. aut Lee, A. R. aut Lee, J. H. aut Lee, L. aut MacEwan, S. aut Mack, D. aut Magee, J. A. aut Mahurin, R. aut Mammei, J. aut Martin, J. aut McHugh, M. aut Meekins, D. aut Mei, J. aut Michaels, R. aut Micherdzinska, A. aut Myers, K. E. aut Mkrtchyan, A. aut Mkrtchyan, H. aut Narayan, A. aut Ndukum, L. Z. aut Nelyubin, V. aut Nuruzzaman, N. aut van Oers, W. T. H aut Opper, A. K. aut Page, S. A. aut Pan, J. aut Paschke, K. aut Phillips, S. K. aut Pitt, M. L. aut Poelker, M. aut Rajotte, J. F. aut Ramsay, W. D. aut Roche, J. aut Sawatzky, B. aut Seva, T. aut Shabestari, M. H. aut Silwal, R. aut Simicevic, N. aut Smith, G. aut Solvignon, P. aut Spayde, D. T. aut Subedi, A. aut Subedi, R. aut Suleiman, R. aut Tadevosyan, V. aut Tobias, W. A. aut Tvaskis, V. aut Waidyawansa, B. aut Wang, P. aut Wells, S. P. aut Wood, S. A. aut Yang, S. aut Young, R. D. aut Zhamkochyan, S. aut Zou, D. aut Enthalten in Hyperfine interactions Springer Netherlands, 1975 214(2013), 1-3 vom: 13. Feb., Seite 21-30 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:214 year:2013 number:1-3 day:13 month:02 pages:21-30 https://doi.org/10.1007/s10751-013-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2279 33.00 VZ AR 214 2013 1-3 13 02 21-30 |
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10.1007/s10751-013-0782-0 doi (DE-627)OLC2076420703 (DE-He213)s10751-013-0782-0-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Androic, D. verfasserin aut The ${Q^{p}_{\rm Weak}}$ experiment 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media Dordrecht 2013 Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. Standard model Weak charge Parity violation Electron scattering New physics Armstrong, D. S. aut Asaturyan, A. aut Averett, T. aut Balewski, J. aut Beaufait, J. aut Beminiwattha, R. S. aut Benesch, J. aut Benmokhtar, F. aut Birchall, J. aut Carlini, R. D. aut Cornejo, J. C. aut Covrig, S. aut Dalton, M. M. aut Davis, C. A. aut Deconinck, W. aut Diefenbach, J. aut Dow, K. aut Dowd, J. F. aut Dunne, J. A. aut Dutta, D. aut Duvall, W. S. aut Elaasar, M. aut Falk, W. R. aut Finn, J. M. aut Forest, T. aut Gaskell, D. aut Gericke, M. T. W. aut Grames, J. aut Gray, V. M. aut Grimm, K. aut Guo, F. aut Hoskins, J. R. aut Johnston, K. aut Jones, D. aut Jones, M. aut Jones, R. aut Kargiantoulakis, M. aut King, P. M. aut Korkmaz, E. aut Kowalski, S. aut Leacock, J. aut Leckey, J. aut Lee, A. R. aut Lee, J. H. aut Lee, L. aut MacEwan, S. aut Mack, D. aut Magee, J. A. aut Mahurin, R. aut Mammei, J. aut Martin, J. aut McHugh, M. aut Meekins, D. aut Mei, J. aut Michaels, R. aut Micherdzinska, A. aut Myers, K. E. aut Mkrtchyan, A. aut Mkrtchyan, H. aut Narayan, A. aut Ndukum, L. Z. aut Nelyubin, V. aut Nuruzzaman, N. aut van Oers, W. T. H aut Opper, A. K. aut Page, S. A. aut Pan, J. aut Paschke, K. aut Phillips, S. K. aut Pitt, M. L. aut Poelker, M. aut Rajotte, J. F. aut Ramsay, W. D. aut Roche, J. aut Sawatzky, B. aut Seva, T. aut Shabestari, M. H. aut Silwal, R. aut Simicevic, N. aut Smith, G. aut Solvignon, P. aut Spayde, D. T. aut Subedi, A. aut Subedi, R. aut Suleiman, R. aut Tadevosyan, V. aut Tobias, W. A. aut Tvaskis, V. aut Waidyawansa, B. aut Wang, P. aut Wells, S. P. aut Wood, S. A. aut Yang, S. aut Young, R. D. aut Zhamkochyan, S. aut Zou, D. aut Enthalten in Hyperfine interactions Springer Netherlands, 1975 214(2013), 1-3 vom: 13. Feb., Seite 21-30 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:214 year:2013 number:1-3 day:13 month:02 pages:21-30 https://doi.org/10.1007/s10751-013-0782-0 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2279 33.00 VZ AR 214 2013 1-3 13 02 21-30 |
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Androic, D. Armstrong, D. S. Asaturyan, A. Averett, T. Balewski, J. Beaufait, J. Beminiwattha, R. S. Benesch, J. Benmokhtar, F. Birchall, J. Carlini, R. D. Cornejo, J. C. Covrig, S. Dalton, M. M. Davis, C. A. Deconinck, W. Diefenbach, J. Dow, K. Dowd, J. F. Dunne, J. A. Dutta, D. Duvall, W. S. Elaasar, M. Falk, W. R. Finn, J. M. Forest, T. Gaskell, D. Gericke, M. T. W. Grames, J. Gray, V. M. Grimm, K. Guo, F. Hoskins, J. R. Johnston, K. Jones, D. Jones, M. Jones, R. Kargiantoulakis, M. King, P. M. Korkmaz, E. Kowalski, S. Leacock, J. Leckey, J. Lee, A. R. Lee, J. H. Lee, L. MacEwan, S. Mack, D. Magee, J. A. Mahurin, R. Mammei, J. Martin, J. McHugh, M. Meekins, D. Mei, J. Michaels, R. Micherdzinska, A. Myers, K. E. Mkrtchyan, A. Mkrtchyan, H. Narayan, A. Ndukum, L. Z. Nelyubin, V. Nuruzzaman, N. van Oers, W. T. H Opper, A. K. Page, S. A. Pan, J. Paschke, K. Phillips, S. K. Pitt, M. L. Poelker, M. Rajotte, J. F. Ramsay, W. D. Roche, J. Sawatzky, B. Seva, T. Shabestari, M. H. Silwal, R. Simicevic, N. Smith, G. Solvignon, P. Spayde, D. T. Subedi, A. Subedi, R. Suleiman, R. Tadevosyan, V. Tobias, W. A. Tvaskis, V. Waidyawansa, B. Wang, P. Wells, S. P. Wood, S. A. Yang, S. Young, R. D. Zhamkochyan, S. Zou, D. |
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Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. © Springer Science+Business Media Dordrecht 2013 |
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Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. © Springer Science+Business Media Dordrecht 2013 |
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Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. This paper provides an overview of the physics and the experiment, as well as a brief look at some preliminary diagnostic and analysis data. © Springer Science+Business Media Dordrecht 2013 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2076420703</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503074013.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2013 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10751-013-0782-0</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076420703</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s10751-013-0782-0-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Androic, D.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">The ${Q^{p}_{\rm Weak}}$ experiment</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2013</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Springer Science+Business Media Dordrecht 2013</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In May 2012, the $Q^{p}_{\rm Weak}$ collaboration completed a two year measurement program to determine the weak charge of the proton ${Q^{p}_W} = ( 1 - 4\sin^2{\theta_{W}})$ at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment was designed to produce a 4.0 % measurement of the weak charge, via a 2.5 % measurement of the parity violating asymmetry in the number of elastically scattered 1.165 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3 % measurement of the weak mixing angle at a momentum transfer of Q2 = 0.026 $ GeV^{2} $, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, $Q^{p}_{\rm Weak}$ will also provide a high precision determination of the weak charges of the up and down quarks. At the proposed precision, a significant deviation from the Standard Model prediction could be a signal of new physics at mass scales up to ≃ 6 TeV, whereas agreement would place new and significant constraints on possible Standard Model extensions at mass scales up to ≃ 2 TeV. 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