Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $
Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for bot...
Ausführliche Beschreibung
Autor*in: |
Anastasi, A. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2018 |
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Schlagwörter: |
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Anmerkung: |
© The Author(s) 2018 |
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Übergeordnetes Werk: |
Enthalten in: Journal of high energy physics - Berlin : Springer, 1997, 2018(2018), 3 vom: 28. März |
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Übergeordnetes Werk: |
volume:2018 ; year:2018 ; number:3 ; day:28 ; month:03 |
Links: |
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DOI / URN: |
10.1007/JHEP03(2018)173 |
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Katalog-ID: |
SPR030554861 |
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245 | 1 | 0 | |a Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ |
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520 | |a Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. | ||
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700 | 1 | |a Babusci, D. |4 aut | |
700 | 1 | |a Berlowski, M. |4 aut | |
700 | 1 | |a Bloise, C. |4 aut | |
700 | 1 | |a Bossi, F. |4 aut | |
700 | 1 | |a Branchini, P. |4 aut | |
700 | 1 | |a Budano, A. |4 aut | |
700 | 1 | |a Balkeståhl, L. Caldeira |4 aut | |
700 | 1 | |a Cao, B. |4 aut | |
700 | 1 | |a Ceradini, F. |4 aut | |
700 | 1 | |a Ciambrone, P. |4 aut | |
700 | 1 | |a Curciarello, F. |4 aut | |
700 | 1 | |a Czerwinski, E. |4 aut | |
700 | 1 | |a D’Agostini, G. |4 aut | |
700 | 1 | |a Danè, E. |4 aut | |
700 | 1 | |a De Leo, V. |4 aut | |
700 | 1 | |a De Lucia, E. |4 aut | |
700 | 1 | |a De Santis, A. |4 aut | |
700 | 1 | |a De Simone, P. |4 aut | |
700 | 1 | |a Di Cicco, A. |4 aut | |
700 | 1 | |a Di Domenico, A. |4 aut | |
700 | 1 | |a Domenici, D. |4 aut | |
700 | 1 | |a D’Uffizi, A. |4 aut | |
700 | 1 | |a Fantini, A. |4 aut | |
700 | 1 | |a Fantini, G. |4 aut | |
700 | 1 | |a Fermani, P. |4 aut | |
700 | 1 | |a Fiore, S. |4 aut | |
700 | 1 | |a Gajos, A. |4 aut | |
700 | 1 | |a Gauzzi, P. |4 aut | |
700 | 1 | |a Giovannella, S. |4 aut | |
700 | 1 | |a Graziani, E. |4 aut | |
700 | 1 | |a Ivanov, V. L. |4 aut | |
700 | 1 | |a Johansson, T. |4 aut | |
700 | 1 | |a Kang, X. |4 aut | |
700 | 1 | |a Kisielewska-Kaminska, D. |4 aut | |
700 | 1 | |a Kozyrev, E. A. |4 aut | |
700 | 1 | |a Krzemien, W. |4 aut | |
700 | 1 | |a Kupsc, A. |4 aut | |
700 | 1 | |a Loffredo, S. |4 aut | |
700 | 1 | |a Lukin, P. A. |4 aut | |
700 | 1 | |a Mandaglio, G. |4 aut | |
700 | 1 | |a Martini, M. |4 aut | |
700 | 1 | |a Messi, R. |4 aut | |
700 | 1 | |a Miscetti, S. |4 aut | |
700 | 1 | |a Morello, G. |4 aut | |
700 | 1 | |a Moricciani, D. |4 aut | |
700 | 1 | |a Moskal, P. |4 aut | |
700 | 1 | |a Passeri, A. |4 aut | |
700 | 1 | |a Patera, V. |4 aut | |
700 | 1 | |a del Rio, E. Perez |4 aut | |
700 | 1 | |a Raha, N. |4 aut | |
700 | 1 | |a Santangelo, P. |4 aut | |
700 | 1 | |a Schioppa, M. |4 aut | |
700 | 1 | |a Selce, A. |4 aut | |
700 | 1 | |a Silarski, M. |4 aut | |
700 | 1 | |a Sirghi, F. |4 aut | |
700 | 1 | |a Solodov, E. P. |4 aut | |
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700 | 1 | |a Wolke, M. |4 aut | |
700 | 1 | |a Keshavarzi, A. |4 aut | |
700 | 1 | |a Müller, S.E. |4 aut | |
700 | 1 | |a Teubner, T. |4 aut | |
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10.1007/JHEP03(2018)173 doi (DE-627)SPR030554861 (SPR)JHEP03(2018)173-e DE-627 ger DE-627 rakwb eng Anastasi, A. verfasserin aut Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2018 Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. e+-e- Experiments (dpeaa)DE-He213 Babusci, D. aut Berlowski, M. aut Bloise, C. aut Bossi, F. aut Branchini, P. aut Budano, A. aut Balkeståhl, L. Caldeira aut Cao, B. aut Ceradini, F. aut Ciambrone, P. aut Curciarello, F. aut Czerwinski, E. aut D’Agostini, G. aut Danè, E. aut De Leo, V. aut De Lucia, E. aut De Santis, A. aut De Simone, P. aut Di Cicco, A. aut Di Domenico, A. aut Domenici, D. aut D’Uffizi, A. aut Fantini, A. aut Fantini, G. aut Fermani, P. aut Fiore, S. aut Gajos, A. aut Gauzzi, P. aut Giovannella, S. aut Graziani, E. aut Ivanov, V. L. aut Johansson, T. aut Kang, X. aut Kisielewska-Kaminska, D. aut Kozyrev, E. A. aut Krzemien, W. aut Kupsc, A. aut Loffredo, S. aut Lukin, P. A. aut Mandaglio, G. aut Martini, M. aut Messi, R. aut Miscetti, S. aut Morello, G. aut Moricciani, D. aut Moskal, P. aut Passeri, A. aut Patera, V. aut del Rio, E. Perez aut Raha, N. aut Santangelo, P. aut Schioppa, M. aut Selce, A. aut Silarski, M. aut Sirghi, F. aut Solodov, E. P. aut Tortora, L. aut Venanzoni, G. aut Wislicki, W. aut Wolke, M. aut Keshavarzi, A. aut Müller, S.E. aut Teubner, T. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2018(2018), 3 vom: 28. März (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2018 year:2018 number:3 day:28 month:03 https://dx.doi.org/10.1007/JHEP03(2018)173 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2018 2018 3 28 03 |
spelling |
10.1007/JHEP03(2018)173 doi (DE-627)SPR030554861 (SPR)JHEP03(2018)173-e DE-627 ger DE-627 rakwb eng Anastasi, A. verfasserin aut Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2018 Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. e+-e- Experiments (dpeaa)DE-He213 Babusci, D. aut Berlowski, M. aut Bloise, C. aut Bossi, F. aut Branchini, P. aut Budano, A. aut Balkeståhl, L. Caldeira aut Cao, B. aut Ceradini, F. aut Ciambrone, P. aut Curciarello, F. aut Czerwinski, E. aut D’Agostini, G. aut Danè, E. aut De Leo, V. aut De Lucia, E. aut De Santis, A. aut De Simone, P. aut Di Cicco, A. aut Di Domenico, A. aut Domenici, D. aut D’Uffizi, A. aut Fantini, A. aut Fantini, G. aut Fermani, P. aut Fiore, S. aut Gajos, A. aut Gauzzi, P. aut Giovannella, S. aut Graziani, E. aut Ivanov, V. L. aut Johansson, T. aut Kang, X. aut Kisielewska-Kaminska, D. aut Kozyrev, E. A. aut Krzemien, W. aut Kupsc, A. aut Loffredo, S. aut Lukin, P. A. aut Mandaglio, G. aut Martini, M. aut Messi, R. aut Miscetti, S. aut Morello, G. aut Moricciani, D. aut Moskal, P. aut Passeri, A. aut Patera, V. aut del Rio, E. Perez aut Raha, N. aut Santangelo, P. aut Schioppa, M. aut Selce, A. aut Silarski, M. aut Sirghi, F. aut Solodov, E. P. aut Tortora, L. aut Venanzoni, G. aut Wislicki, W. aut Wolke, M. aut Keshavarzi, A. aut Müller, S.E. aut Teubner, T. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2018(2018), 3 vom: 28. März (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2018 year:2018 number:3 day:28 month:03 https://dx.doi.org/10.1007/JHEP03(2018)173 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2018 2018 3 28 03 |
allfields_unstemmed |
10.1007/JHEP03(2018)173 doi (DE-627)SPR030554861 (SPR)JHEP03(2018)173-e DE-627 ger DE-627 rakwb eng Anastasi, A. verfasserin aut Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2018 Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. e+-e- Experiments (dpeaa)DE-He213 Babusci, D. aut Berlowski, M. aut Bloise, C. aut Bossi, F. aut Branchini, P. aut Budano, A. aut Balkeståhl, L. Caldeira aut Cao, B. aut Ceradini, F. aut Ciambrone, P. aut Curciarello, F. aut Czerwinski, E. aut D’Agostini, G. aut Danè, E. aut De Leo, V. aut De Lucia, E. aut De Santis, A. aut De Simone, P. aut Di Cicco, A. aut Di Domenico, A. aut Domenici, D. aut D’Uffizi, A. aut Fantini, A. aut Fantini, G. aut Fermani, P. aut Fiore, S. aut Gajos, A. aut Gauzzi, P. aut Giovannella, S. aut Graziani, E. aut Ivanov, V. L. aut Johansson, T. aut Kang, X. aut Kisielewska-Kaminska, D. aut Kozyrev, E. A. aut Krzemien, W. aut Kupsc, A. aut Loffredo, S. aut Lukin, P. A. aut Mandaglio, G. aut Martini, M. aut Messi, R. aut Miscetti, S. aut Morello, G. aut Moricciani, D. aut Moskal, P. aut Passeri, A. aut Patera, V. aut del Rio, E. Perez aut Raha, N. aut Santangelo, P. aut Schioppa, M. aut Selce, A. aut Silarski, M. aut Sirghi, F. aut Solodov, E. P. aut Tortora, L. aut Venanzoni, G. aut Wislicki, W. aut Wolke, M. aut Keshavarzi, A. aut Müller, S.E. aut Teubner, T. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2018(2018), 3 vom: 28. März (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2018 year:2018 number:3 day:28 month:03 https://dx.doi.org/10.1007/JHEP03(2018)173 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2018 2018 3 28 03 |
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10.1007/JHEP03(2018)173 doi (DE-627)SPR030554861 (SPR)JHEP03(2018)173-e DE-627 ger DE-627 rakwb eng Anastasi, A. verfasserin aut Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2018 Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. e+-e- Experiments (dpeaa)DE-He213 Babusci, D. aut Berlowski, M. aut Bloise, C. aut Bossi, F. aut Branchini, P. aut Budano, A. aut Balkeståhl, L. Caldeira aut Cao, B. aut Ceradini, F. aut Ciambrone, P. aut Curciarello, F. aut Czerwinski, E. aut D’Agostini, G. aut Danè, E. aut De Leo, V. aut De Lucia, E. aut De Santis, A. aut De Simone, P. aut Di Cicco, A. aut Di Domenico, A. aut Domenici, D. aut D’Uffizi, A. aut Fantini, A. aut Fantini, G. aut Fermani, P. aut Fiore, S. aut Gajos, A. aut Gauzzi, P. aut Giovannella, S. aut Graziani, E. aut Ivanov, V. L. aut Johansson, T. aut Kang, X. aut Kisielewska-Kaminska, D. aut Kozyrev, E. A. aut Krzemien, W. aut Kupsc, A. aut Loffredo, S. aut Lukin, P. A. aut Mandaglio, G. aut Martini, M. aut Messi, R. aut Miscetti, S. aut Morello, G. aut Moricciani, D. aut Moskal, P. aut Passeri, A. aut Patera, V. aut del Rio, E. Perez aut Raha, N. aut Santangelo, P. aut Schioppa, M. aut Selce, A. aut Silarski, M. aut Sirghi, F. aut Solodov, E. P. aut Tortora, L. aut Venanzoni, G. aut Wislicki, W. aut Wolke, M. aut Keshavarzi, A. aut Müller, S.E. aut Teubner, T. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2018(2018), 3 vom: 28. März (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2018 year:2018 number:3 day:28 month:03 https://dx.doi.org/10.1007/JHEP03(2018)173 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2018 2018 3 28 03 |
allfieldsSound |
10.1007/JHEP03(2018)173 doi (DE-627)SPR030554861 (SPR)JHEP03(2018)173-e DE-627 ger DE-627 rakwb eng Anastasi, A. verfasserin aut Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ 2018 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2018 Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. e+-e- Experiments (dpeaa)DE-He213 Babusci, D. aut Berlowski, M. aut Bloise, C. aut Bossi, F. aut Branchini, P. aut Budano, A. aut Balkeståhl, L. Caldeira aut Cao, B. aut Ceradini, F. aut Ciambrone, P. aut Curciarello, F. aut Czerwinski, E. aut D’Agostini, G. aut Danè, E. aut De Leo, V. aut De Lucia, E. aut De Santis, A. aut De Simone, P. aut Di Cicco, A. aut Di Domenico, A. aut Domenici, D. aut D’Uffizi, A. aut Fantini, A. aut Fantini, G. aut Fermani, P. aut Fiore, S. aut Gajos, A. aut Gauzzi, P. aut Giovannella, S. aut Graziani, E. aut Ivanov, V. L. aut Johansson, T. aut Kang, X. aut Kisielewska-Kaminska, D. aut Kozyrev, E. A. aut Krzemien, W. aut Kupsc, A. aut Loffredo, S. aut Lukin, P. A. aut Mandaglio, G. aut Martini, M. aut Messi, R. aut Miscetti, S. aut Morello, G. aut Moricciani, D. aut Moskal, P. aut Passeri, A. aut Patera, V. aut del Rio, E. Perez aut Raha, N. aut Santangelo, P. aut Schioppa, M. aut Selce, A. aut Silarski, M. aut Sirghi, F. aut Solodov, E. P. aut Tortora, L. aut Venanzoni, G. aut Wislicki, W. aut Wolke, M. aut Keshavarzi, A. aut Müller, S.E. aut Teubner, T. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2018(2018), 3 vom: 28. März (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2018 year:2018 number:3 day:28 month:03 https://dx.doi.org/10.1007/JHEP03(2018)173 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2018 2018 3 28 03 |
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Anastasi, A. @@aut@@ Babusci, D. @@aut@@ Berlowski, M. @@aut@@ Bloise, C. @@aut@@ Bossi, F. @@aut@@ Branchini, P. @@aut@@ Budano, A. @@aut@@ Balkeståhl, L. Caldeira @@aut@@ Cao, B. @@aut@@ Ceradini, F. @@aut@@ Ciambrone, P. @@aut@@ Curciarello, F. @@aut@@ Czerwinski, E. @@aut@@ D’Agostini, G. @@aut@@ Danè, E. @@aut@@ De Leo, V. @@aut@@ De Lucia, E. @@aut@@ De Santis, A. @@aut@@ De Simone, P. @@aut@@ Di Cicco, A. @@aut@@ Di Domenico, A. @@aut@@ Domenici, D. @@aut@@ D’Uffizi, A. @@aut@@ Fantini, A. @@aut@@ Fantini, G. @@aut@@ Fermani, P. @@aut@@ Fiore, S. @@aut@@ Gajos, A. @@aut@@ Gauzzi, P. @@aut@@ Giovannella, S. @@aut@@ Graziani, E. @@aut@@ Ivanov, V. L. @@aut@@ Johansson, T. @@aut@@ Kang, X. @@aut@@ Kisielewska-Kaminska, D. @@aut@@ Kozyrev, E. A. @@aut@@ Krzemien, W. @@aut@@ Kupsc, A. @@aut@@ Loffredo, S. @@aut@@ Lukin, P. A. @@aut@@ Mandaglio, G. @@aut@@ Martini, M. @@aut@@ Messi, R. @@aut@@ Miscetti, S. @@aut@@ Morello, G. @@aut@@ Moricciani, D. @@aut@@ Moskal, P. @@aut@@ Passeri, A. @@aut@@ Patera, V. @@aut@@ del Rio, E. Perez @@aut@@ Raha, N. @@aut@@ Santangelo, P. @@aut@@ Schioppa, M. @@aut@@ Selce, A. @@aut@@ Silarski, M. @@aut@@ Sirghi, F. @@aut@@ Solodov, E. P. @@aut@@ Tortora, L. @@aut@@ Venanzoni, G. @@aut@@ Wislicki, W. @@aut@@ Wolke, M. @@aut@@ Keshavarzi, A. @@aut@@ Müller, S.E. @@aut@@ Teubner, T. @@aut@@ |
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Anastasi, A. |
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Anastasi, A. misc e+-e- Experiments Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ |
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Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ e+-e- Experiments (dpeaa)DE-He213 |
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Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ |
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Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ |
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Anastasi, A. Babusci, D. Berlowski, M. Bloise, C. Bossi, F. Branchini, P. Budano, A. Balkeståhl, L. Caldeira Cao, B. Ceradini, F. Ciambrone, P. Curciarello, F. Czerwinski, E. D’Agostini, G. Danè, E. De Leo, V. De Lucia, E. De Santis, A. De Simone, P. Di Cicco, A. Di Domenico, A. Domenici, D. D’Uffizi, A. Fantini, A. Fantini, G. Fermani, P. Fiore, S. Gajos, A. Gauzzi, P. Giovannella, S. Graziani, E. Ivanov, V. L. Johansson, T. Kang, X. Kisielewska-Kaminska, D. Kozyrev, E. A. Krzemien, W. Kupsc, A. Loffredo, S. Lukin, P. A. Mandaglio, G. Martini, M. Messi, R. Miscetti, S. Morello, G. Moricciani, D. Moskal, P. Passeri, A. Patera, V. del Rio, E. Perez Raha, N. Santangelo, P. Schioppa, M. Selce, A. Silarski, M. Sirghi, F. Solodov, E. P. Tortora, L. Venanzoni, G. Wislicki, W. Wolke, M. Keshavarzi, A. Müller, S.E. Teubner, T. |
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2018 |
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Elektronische Aufsätze |
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Anastasi, A. |
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10.1007/JHEP03(2018)173 |
title_sort |
combination of kloe σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ gev^{2} $ |
title_auth |
Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ |
abstract |
Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. © The Author(s) 2018 |
abstractGer |
Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. © The Author(s) 2018 |
abstract_unstemmed |
Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. Data vectors and covariance matrices are available at http://www.lnf.infn.it/kloe/ppg/ppg_2017/ppg_2017.html. © The Author(s) 2018 |
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Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $ |
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Babusci, D. Berlowski, M. Bloise, C. Bossi, F. Branchini, P. Budano, A. Balkeståhl, L. Caldeira Cao, B. Ceradini, F. Ciambrone, P. Curciarello, F. Czerwinski, E. D’Agostini, G. Danè, E. De Leo, V. De Lucia, E. De Santis, A. De Simone, P. Di Cicco, A. Di Domenico, A. Domenici, D. D’Uffizi, A. Fantini, A. Fantini, G. Fermani, P. Fiore, S. Gajos, A. Gauzzi, P. Giovannella, S. Graziani, E. Ivanov, V. L. Johansson, T. Kang, X. Kisielewska-Kaminska, D. Kozyrev, E. A. Krzemien, W. Kupsc, A. Loffredo, S. Lukin, P. A. Mandaglio, G. Martini, M. Messi, R. Miscetti, S. Morello, G. Moricciani, D. Moskal, P. Passeri, A. Patera, V. del Rio, E. Perez Raha, N. Santangelo, P. Schioppa, M. Selce, A. Silarski, M. Sirghi, F. Solodov, E. P. Tortora, L. Venanzoni, G. Wislicki, W. Wolke, M. Keshavarzi, A. Müller, S.E. Teubner, T. |
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Babusci, D. Berlowski, M. Bloise, C. Bossi, F. Branchini, P. Budano, A. Balkeståhl, L. Caldeira Cao, B. Ceradini, F. Ciambrone, P. Curciarello, F. Czerwinski, E. D’Agostini, G. Danè, E. De Leo, V. De Lucia, E. De Santis, A. De Simone, P. Di Cicco, A. Di Domenico, A. Domenici, D. D’Uffizi, A. Fantini, A. Fantini, G. Fermani, P. Fiore, S. Gajos, A. Gauzzi, P. Giovannella, S. Graziani, E. Ivanov, V. L. Johansson, T. Kang, X. Kisielewska-Kaminska, D. Kozyrev, E. A. Krzemien, W. Kupsc, A. Loffredo, S. Lukin, P. A. Mandaglio, G. Martini, M. Messi, R. Miscetti, S. Morello, G. Moricciani, D. Moskal, P. Passeri, A. Patera, V. del Rio, E. Perez Raha, N. Santangelo, P. Schioppa, M. Selce, A. Silarski, M. Sirghi, F. Solodov, E. P. Tortora, L. Venanzoni, G. Wislicki, W. Wolke, M. Keshavarzi, A. Müller, S.E. Teubner, T. |
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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">SPR030554861</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331092453.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2018 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/JHEP03(2018)173</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR030554861</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)JHEP03(2018)173-e</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="100" ind1="1" ind2=" "><subfield code="a">Anastasi, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Combination of KLOE σ (e+e− → $ π^{+} %$ π^{−} $γ(γ)) measurements and determination of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}} %$ in the energy range 0.10 < s < 0.95 $ GeV^{2} $</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018</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">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s) 2018</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The three precision measurements of the cross section σ(e+e− → π+π−γ(γ)) using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for σ(e+e− → π+π−γ(γ)). We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range 0.10 < s < 0.95 $ GeV^{2} $ of %$ {a}_{\mu}^{\pi^{+}{\pi}^{-}}=\left(489.8\pm {1.7}_{\mathrm{stat}}\pm {4.8}_{\mathrm{sys}}\right)\times {10}^{-10} %$. 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