First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays
Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 a...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Resmi, P. K. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2019 |
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| Schlagwörter: |
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| Anmerkung: |
© The Author(s) 2019 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of high energy physics - Berlin : Springer, 1997, 2019(2019), 10 vom: 16. Okt. |
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| Übergeordnetes Werk: |
volume:2019 ; year:2019 ; number:10 ; day:16 ; month:10 |
| Links: |
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| DOI / URN: |
10.1007/JHEP10(2019)178 |
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| Katalog-ID: |
SPR030571790 |
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| 100 | 1 | |a Resmi, P. K. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays |
| 264 | 1 | |c 2019 | |
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| 500 | |a © The Author(s) 2019 | ||
| 520 | |a Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. | ||
| 650 | 4 | |a CKM angle gamma |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a CP violation |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a e+-e- Experiments |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a B physics |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Flavor physics |7 (dpeaa)DE-He213 | |
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2019 |
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10.1007/JHEP10(2019)178 doi (DE-627)SPR030571790 (SPR)JHEP10(2019)178-e DE-627 ger DE-627 rakwb eng Resmi, P. K. verfasserin aut First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2019 Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. CKM angle gamma (dpeaa)DE-He213 CP violation (dpeaa)DE-He213 e+-e- Experiments (dpeaa)DE-He213 B physics (dpeaa)DE-He213 Flavor physics (dpeaa)DE-He213 Libby, J. aut Trabelsi, K. aut Adachi, I. aut Aihara, H. aut Al Said, S. aut Asner, D. M. aut Aulchenko, V. aut Aushev, T. aut Babu, V. aut Badhrees, I. aut Bakich, A. M. aut Beleño, C. aut Bennett, J. aut Bhardwaj, V. aut Bhuyan, B. aut Bilka, T. aut Biswal, J. aut Bozek, A. aut Bračko, M. aut Campajola, M. aut Červenkov, D. aut Chen, A. aut Cheon, B. G. aut Cho, H. E. aut Cho, K. aut Choi, Y. aut Choudhury, S. aut Cinabro, D. aut Cunliffe, S. aut Dash, N. aut De Nardo, G. aut Di Capua, F. aut Di Carlo, S. aut Doležal, Z. aut Dong, T. V. aut Eidelman, S. aut Epifanov, D. aut Fast, J. E. aut Ferber, T. aut Fulsom, B. G. aut Garg, R. aut Gaur, V. aut Gabyshev, N. aut Garmash, A. aut Giri, A. aut Goldenzweig, P. aut Golob, B. aut Guan, Y. aut Hayasaka, K. aut Hayashii, H. aut Hou, W.-S. aut Huang, K. aut Iijima, T. aut Inami, K. aut Inguglia, G. aut Ishikawa, A. aut Itoh, R. aut Iwasaki, M. aut Iwasaki, Y. aut Jacobs, W. W. aut Jeon, H. B. aut Jin, Y. aut Joffe, D. aut Kaliyar, A. B. aut Kang, K. H. aut Karyan, G. aut Kawasaki, T. aut Kiesling, C. aut Kim, D. Y. aut Kim, K. T. aut Kim, S. H. aut Kinoshita, K. aut Kodyš, P. aut Kotchetkov, D. aut Krǐzan, P. aut Kroeger, R. aut Krokovny, P. aut Kuhr, T. aut Kumar, R. aut Kuzmin, A. aut Kwon, Y.-J. aut Lee, S. C. aut Li, Y. B. aut Lieret, K. aut Liventsev, D. aut Lu, P.-C. aut Luo, T. aut MacQueen, C. aut Masuda, M. aut Matsuda, T. aut Matvienko, D. aut Merola, M. aut Miyabayashi, K. aut Mizuk, R. aut Mohanty, G. B. aut Moon, H. K. aut Nakano, T. aut Nakao, M. aut Nath, K. J. aut Nayak, M. aut Niiyama, M. aut Nisar, N. K. aut Nishida, S. aut Nishimura, K. aut Ogawa, S. aut Ono, H. aut Onuki, Y. aut Pakhlov, P. aut Pakhlova, G. aut Pal, B. aut Pardi, S. aut Park, H. aut Pedlar, T. K. aut Pestotnik, R. aut Piilonen, L. E. aut Prencipe, E. aut Prim, M. T. aut Ritter, M. aut Röhrken, M. aut Russo, G. aut Sahoo, D. aut Sakai, Y. aut Sandilya, S. aut Santelj, L. aut Sanuki, T. aut Savinov, V. aut Schneider, O. aut Schnell, G. aut Schwanda, C. aut Schwartz, A. J. aut Seino, Y. aut Senyo, K. aut Sevior, M. E. aut Shebalin, V. aut Shen, C. P. aut Shiu, J.-G. aut Shwartz, B. aut Solovieva, E. aut Starič, M. aut Stottler, Z. S. aut Strube, J. F. aut Sumiyoshi, T. aut Takizawa, M. aut Tamponi, U. aut Tanida, K. aut Tenchini, F. aut Uchida, M. aut Uglov, T. aut Uno, S. aut Usov, Y. aut Van Tonder, R. aut Varner, G. aut Vinokurova, A. aut Vorobyev, V. aut Vossen, A. aut Wang, B. aut Wang, C. H. aut Wang, M.-Z. aut Wang, X. L. aut Watanuki, S. aut Won, E. aut Yang, S. B. aut Ye, H. aut Zhang, Z. P. aut Zhilich, V. aut Zhukova, V. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2019(2019), 10 vom: 16. Okt. (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2019 year:2019 number:10 day:16 month:10 https://dx.doi.org/10.1007/JHEP10(2019)178 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 2019 2019 10 16 10 |
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10.1007/JHEP10(2019)178 doi (DE-627)SPR030571790 (SPR)JHEP10(2019)178-e DE-627 ger DE-627 rakwb eng Resmi, P. K. verfasserin aut First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2019 Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. CKM angle gamma (dpeaa)DE-He213 CP violation (dpeaa)DE-He213 e+-e- Experiments (dpeaa)DE-He213 B physics (dpeaa)DE-He213 Flavor physics (dpeaa)DE-He213 Libby, J. aut Trabelsi, K. aut Adachi, I. aut Aihara, H. aut Al Said, S. aut Asner, D. M. aut Aulchenko, V. aut Aushev, T. aut Babu, V. aut Badhrees, I. aut Bakich, A. M. aut Beleño, C. aut Bennett, J. aut Bhardwaj, V. aut Bhuyan, B. aut Bilka, T. aut Biswal, J. aut Bozek, A. aut Bračko, M. aut Campajola, M. aut Červenkov, D. aut Chen, A. aut Cheon, B. G. aut Cho, H. E. aut Cho, K. aut Choi, Y. aut Choudhury, S. aut Cinabro, D. aut Cunliffe, S. aut Dash, N. aut De Nardo, G. aut Di Capua, F. aut Di Carlo, S. aut Doležal, Z. aut Dong, T. V. aut Eidelman, S. aut Epifanov, D. aut Fast, J. E. aut Ferber, T. aut Fulsom, B. G. aut Garg, R. aut Gaur, V. aut Gabyshev, N. aut Garmash, A. aut Giri, A. aut Goldenzweig, P. aut Golob, B. aut Guan, Y. aut Hayasaka, K. aut Hayashii, H. aut Hou, W.-S. aut Huang, K. aut Iijima, T. aut Inami, K. aut Inguglia, G. aut Ishikawa, A. aut Itoh, R. aut Iwasaki, M. aut Iwasaki, Y. aut Jacobs, W. W. aut Jeon, H. B. aut Jin, Y. aut Joffe, D. aut Kaliyar, A. B. aut Kang, K. H. aut Karyan, G. aut Kawasaki, T. aut Kiesling, C. aut Kim, D. Y. aut Kim, K. T. aut Kim, S. H. aut Kinoshita, K. aut Kodyš, P. aut Kotchetkov, D. aut Krǐzan, P. aut Kroeger, R. aut Krokovny, P. aut Kuhr, T. aut Kumar, R. aut Kuzmin, A. aut Kwon, Y.-J. aut Lee, S. C. aut Li, Y. B. aut Lieret, K. aut Liventsev, D. aut Lu, P.-C. aut Luo, T. aut MacQueen, C. aut Masuda, M. aut Matsuda, T. aut Matvienko, D. aut Merola, M. aut Miyabayashi, K. aut Mizuk, R. aut Mohanty, G. B. aut Moon, H. K. aut Nakano, T. aut Nakao, M. aut Nath, K. J. aut Nayak, M. aut Niiyama, M. aut Nisar, N. K. aut Nishida, S. aut Nishimura, K. aut Ogawa, S. aut Ono, H. aut Onuki, Y. aut Pakhlov, P. aut Pakhlova, G. aut Pal, B. aut Pardi, S. aut Park, H. aut Pedlar, T. K. aut Pestotnik, R. aut Piilonen, L. E. aut Prencipe, E. aut Prim, M. T. aut Ritter, M. aut Röhrken, M. aut Russo, G. aut Sahoo, D. aut Sakai, Y. aut Sandilya, S. aut Santelj, L. aut Sanuki, T. aut Savinov, V. aut Schneider, O. aut Schnell, G. aut Schwanda, C. aut Schwartz, A. J. aut Seino, Y. aut Senyo, K. aut Sevior, M. E. aut Shebalin, V. aut Shen, C. P. aut Shiu, J.-G. aut Shwartz, B. aut Solovieva, E. aut Starič, M. aut Stottler, Z. S. aut Strube, J. F. aut Sumiyoshi, T. aut Takizawa, M. aut Tamponi, U. aut Tanida, K. aut Tenchini, F. aut Uchida, M. aut Uglov, T. aut Uno, S. aut Usov, Y. aut Van Tonder, R. aut Varner, G. aut Vinokurova, A. aut Vorobyev, V. aut Vossen, A. aut Wang, B. aut Wang, C. H. aut Wang, M.-Z. aut Wang, X. L. aut Watanuki, S. aut Won, E. aut Yang, S. B. aut Ye, H. aut Zhang, Z. P. aut Zhilich, V. aut Zhukova, V. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2019(2019), 10 vom: 16. Okt. (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2019 year:2019 number:10 day:16 month:10 https://dx.doi.org/10.1007/JHEP10(2019)178 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 2019 2019 10 16 10 |
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10.1007/JHEP10(2019)178 doi (DE-627)SPR030571790 (SPR)JHEP10(2019)178-e DE-627 ger DE-627 rakwb eng Resmi, P. K. verfasserin aut First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2019 Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. CKM angle gamma (dpeaa)DE-He213 CP violation (dpeaa)DE-He213 e+-e- Experiments (dpeaa)DE-He213 B physics (dpeaa)DE-He213 Flavor physics (dpeaa)DE-He213 Libby, J. aut Trabelsi, K. aut Adachi, I. aut Aihara, H. aut Al Said, S. aut Asner, D. M. aut Aulchenko, V. aut Aushev, T. aut Babu, V. aut Badhrees, I. aut Bakich, A. M. aut Beleño, C. aut Bennett, J. aut Bhardwaj, V. aut Bhuyan, B. aut Bilka, T. aut Biswal, J. aut Bozek, A. aut Bračko, M. aut Campajola, M. aut Červenkov, D. aut Chen, A. aut Cheon, B. G. aut Cho, H. E. aut Cho, K. aut Choi, Y. aut Choudhury, S. aut Cinabro, D. aut Cunliffe, S. aut Dash, N. aut De Nardo, G. aut Di Capua, F. aut Di Carlo, S. aut Doležal, Z. aut Dong, T. V. aut Eidelman, S. aut Epifanov, D. aut Fast, J. E. aut Ferber, T. aut Fulsom, B. G. aut Garg, R. aut Gaur, V. aut Gabyshev, N. aut Garmash, A. aut Giri, A. aut Goldenzweig, P. aut Golob, B. aut Guan, Y. aut Hayasaka, K. aut Hayashii, H. aut Hou, W.-S. aut Huang, K. aut Iijima, T. aut Inami, K. aut Inguglia, G. aut Ishikawa, A. aut Itoh, R. aut Iwasaki, M. aut Iwasaki, Y. aut Jacobs, W. W. aut Jeon, H. B. aut Jin, Y. aut Joffe, D. aut Kaliyar, A. B. aut Kang, K. H. aut Karyan, G. aut Kawasaki, T. aut Kiesling, C. aut Kim, D. Y. aut Kim, K. T. aut Kim, S. H. aut Kinoshita, K. aut Kodyš, P. aut Kotchetkov, D. aut Krǐzan, P. aut Kroeger, R. aut Krokovny, P. aut Kuhr, T. aut Kumar, R. aut Kuzmin, A. aut Kwon, Y.-J. aut Lee, S. C. aut Li, Y. B. aut Lieret, K. aut Liventsev, D. aut Lu, P.-C. aut Luo, T. aut MacQueen, C. aut Masuda, M. aut Matsuda, T. aut Matvienko, D. aut Merola, M. aut Miyabayashi, K. aut Mizuk, R. aut Mohanty, G. B. aut Moon, H. K. aut Nakano, T. aut Nakao, M. aut Nath, K. J. aut Nayak, M. aut Niiyama, M. aut Nisar, N. K. aut Nishida, S. aut Nishimura, K. aut Ogawa, S. aut Ono, H. aut Onuki, Y. aut Pakhlov, P. aut Pakhlova, G. aut Pal, B. aut Pardi, S. aut Park, H. aut Pedlar, T. K. aut Pestotnik, R. aut Piilonen, L. E. aut Prencipe, E. aut Prim, M. T. aut Ritter, M. aut Röhrken, M. aut Russo, G. aut Sahoo, D. aut Sakai, Y. aut Sandilya, S. aut Santelj, L. aut Sanuki, T. aut Savinov, V. aut Schneider, O. aut Schnell, G. aut Schwanda, C. aut Schwartz, A. J. aut Seino, Y. aut Senyo, K. aut Sevior, M. E. aut Shebalin, V. aut Shen, C. P. aut Shiu, J.-G. aut Shwartz, B. aut Solovieva, E. aut Starič, M. aut Stottler, Z. S. aut Strube, J. F. aut Sumiyoshi, T. aut Takizawa, M. aut Tamponi, U. aut Tanida, K. aut Tenchini, F. aut Uchida, M. aut Uglov, T. aut Uno, S. aut Usov, Y. aut Van Tonder, R. aut Varner, G. aut Vinokurova, A. aut Vorobyev, V. aut Vossen, A. aut Wang, B. aut Wang, C. H. aut Wang, M.-Z. aut Wang, X. L. aut Watanuki, S. aut Won, E. aut Yang, S. B. aut Ye, H. aut Zhang, Z. P. aut Zhilich, V. aut Zhukova, V. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2019(2019), 10 vom: 16. Okt. (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2019 year:2019 number:10 day:16 month:10 https://dx.doi.org/10.1007/JHEP10(2019)178 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 2019 2019 10 16 10 |
| allfieldsGer |
10.1007/JHEP10(2019)178 doi (DE-627)SPR030571790 (SPR)JHEP10(2019)178-e DE-627 ger DE-627 rakwb eng Resmi, P. K. verfasserin aut First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2019 Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. CKM angle gamma (dpeaa)DE-He213 CP violation (dpeaa)DE-He213 e+-e- Experiments (dpeaa)DE-He213 B physics (dpeaa)DE-He213 Flavor physics (dpeaa)DE-He213 Libby, J. aut Trabelsi, K. aut Adachi, I. aut Aihara, H. aut Al Said, S. aut Asner, D. M. aut Aulchenko, V. aut Aushev, T. aut Babu, V. aut Badhrees, I. aut Bakich, A. M. aut Beleño, C. aut Bennett, J. aut Bhardwaj, V. aut Bhuyan, B. aut Bilka, T. aut Biswal, J. aut Bozek, A. aut Bračko, M. aut Campajola, M. aut Červenkov, D. aut Chen, A. aut Cheon, B. G. aut Cho, H. E. aut Cho, K. aut Choi, Y. aut Choudhury, S. aut Cinabro, D. aut Cunliffe, S. aut Dash, N. aut De Nardo, G. aut Di Capua, F. aut Di Carlo, S. aut Doležal, Z. aut Dong, T. V. aut Eidelman, S. aut Epifanov, D. aut Fast, J. E. aut Ferber, T. aut Fulsom, B. G. aut Garg, R. aut Gaur, V. aut Gabyshev, N. aut Garmash, A. aut Giri, A. aut Goldenzweig, P. aut Golob, B. aut Guan, Y. aut Hayasaka, K. aut Hayashii, H. aut Hou, W.-S. aut Huang, K. aut Iijima, T. aut Inami, K. aut Inguglia, G. aut Ishikawa, A. aut Itoh, R. aut Iwasaki, M. aut Iwasaki, Y. aut Jacobs, W. W. aut Jeon, H. B. aut Jin, Y. aut Joffe, D. aut Kaliyar, A. B. aut Kang, K. H. aut Karyan, G. aut Kawasaki, T. aut Kiesling, C. aut Kim, D. Y. aut Kim, K. T. aut Kim, S. H. aut Kinoshita, K. aut Kodyš, P. aut Kotchetkov, D. aut Krǐzan, P. aut Kroeger, R. aut Krokovny, P. aut Kuhr, T. aut Kumar, R. aut Kuzmin, A. aut Kwon, Y.-J. aut Lee, S. C. aut Li, Y. B. aut Lieret, K. aut Liventsev, D. aut Lu, P.-C. aut Luo, T. aut MacQueen, C. aut Masuda, M. aut Matsuda, T. aut Matvienko, D. aut Merola, M. aut Miyabayashi, K. aut Mizuk, R. aut Mohanty, G. B. aut Moon, H. K. aut Nakano, T. aut Nakao, M. aut Nath, K. J. aut Nayak, M. aut Niiyama, M. aut Nisar, N. K. aut Nishida, S. aut Nishimura, K. aut Ogawa, S. aut Ono, H. aut Onuki, Y. aut Pakhlov, P. aut Pakhlova, G. aut Pal, B. aut Pardi, S. aut Park, H. aut Pedlar, T. K. aut Pestotnik, R. aut Piilonen, L. E. aut Prencipe, E. aut Prim, M. T. aut Ritter, M. aut Röhrken, M. aut Russo, G. aut Sahoo, D. aut Sakai, Y. aut Sandilya, S. aut Santelj, L. aut Sanuki, T. aut Savinov, V. aut Schneider, O. aut Schnell, G. aut Schwanda, C. aut Schwartz, A. J. aut Seino, Y. aut Senyo, K. aut Sevior, M. E. aut Shebalin, V. aut Shen, C. P. aut Shiu, J.-G. aut Shwartz, B. aut Solovieva, E. aut Starič, M. aut Stottler, Z. S. aut Strube, J. F. aut Sumiyoshi, T. aut Takizawa, M. aut Tamponi, U. aut Tanida, K. aut Tenchini, F. aut Uchida, M. aut Uglov, T. aut Uno, S. aut Usov, Y. aut Van Tonder, R. aut Varner, G. aut Vinokurova, A. aut Vorobyev, V. aut Vossen, A. aut Wang, B. aut Wang, C. H. aut Wang, M.-Z. aut Wang, X. L. aut Watanuki, S. aut Won, E. aut Yang, S. B. aut Ye, H. aut Zhang, Z. P. aut Zhilich, V. aut Zhukova, V. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2019(2019), 10 vom: 16. Okt. (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2019 year:2019 number:10 day:16 month:10 https://dx.doi.org/10.1007/JHEP10(2019)178 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 2019 2019 10 16 10 |
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10.1007/JHEP10(2019)178 doi (DE-627)SPR030571790 (SPR)JHEP10(2019)178-e DE-627 ger DE-627 rakwb eng Resmi, P. K. verfasserin aut First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2019 Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. CKM angle gamma (dpeaa)DE-He213 CP violation (dpeaa)DE-He213 e+-e- Experiments (dpeaa)DE-He213 B physics (dpeaa)DE-He213 Flavor physics (dpeaa)DE-He213 Libby, J. aut Trabelsi, K. aut Adachi, I. aut Aihara, H. aut Al Said, S. aut Asner, D. M. aut Aulchenko, V. aut Aushev, T. aut Babu, V. aut Badhrees, I. aut Bakich, A. M. aut Beleño, C. aut Bennett, J. aut Bhardwaj, V. aut Bhuyan, B. aut Bilka, T. aut Biswal, J. aut Bozek, A. aut Bračko, M. aut Campajola, M. aut Červenkov, D. aut Chen, A. aut Cheon, B. G. aut Cho, H. E. aut Cho, K. aut Choi, Y. aut Choudhury, S. aut Cinabro, D. aut Cunliffe, S. aut Dash, N. aut De Nardo, G. aut Di Capua, F. aut Di Carlo, S. aut Doležal, Z. aut Dong, T. V. aut Eidelman, S. aut Epifanov, D. aut Fast, J. E. aut Ferber, T. aut Fulsom, B. G. aut Garg, R. aut Gaur, V. aut Gabyshev, N. aut Garmash, A. aut Giri, A. aut Goldenzweig, P. aut Golob, B. aut Guan, Y. aut Hayasaka, K. aut Hayashii, H. aut Hou, W.-S. aut Huang, K. aut Iijima, T. aut Inami, K. aut Inguglia, G. aut Ishikawa, A. aut Itoh, R. aut Iwasaki, M. aut Iwasaki, Y. aut Jacobs, W. W. aut Jeon, H. B. aut Jin, Y. aut Joffe, D. aut Kaliyar, A. B. aut Kang, K. H. aut Karyan, G. aut Kawasaki, T. aut Kiesling, C. aut Kim, D. Y. aut Kim, K. T. aut Kim, S. H. aut Kinoshita, K. aut Kodyš, P. aut Kotchetkov, D. aut Krǐzan, P. aut Kroeger, R. aut Krokovny, P. aut Kuhr, T. aut Kumar, R. aut Kuzmin, A. aut Kwon, Y.-J. aut Lee, S. C. aut Li, Y. B. aut Lieret, K. aut Liventsev, D. aut Lu, P.-C. aut Luo, T. aut MacQueen, C. aut Masuda, M. aut Matsuda, T. aut Matvienko, D. aut Merola, M. aut Miyabayashi, K. aut Mizuk, R. aut Mohanty, G. B. aut Moon, H. K. aut Nakano, T. aut Nakao, M. aut Nath, K. J. aut Nayak, M. aut Niiyama, M. aut Nisar, N. K. aut Nishida, S. aut Nishimura, K. aut Ogawa, S. aut Ono, H. aut Onuki, Y. aut Pakhlov, P. aut Pakhlova, G. aut Pal, B. aut Pardi, S. aut Park, H. aut Pedlar, T. K. aut Pestotnik, R. aut Piilonen, L. E. aut Prencipe, E. aut Prim, M. T. aut Ritter, M. aut Röhrken, M. aut Russo, G. aut Sahoo, D. aut Sakai, Y. aut Sandilya, S. aut Santelj, L. aut Sanuki, T. aut Savinov, V. aut Schneider, O. aut Schnell, G. aut Schwanda, C. aut Schwartz, A. J. aut Seino, Y. aut Senyo, K. aut Sevior, M. E. aut Shebalin, V. aut Shen, C. P. aut Shiu, J.-G. aut Shwartz, B. aut Solovieva, E. aut Starič, M. aut Stottler, Z. S. aut Strube, J. F. aut Sumiyoshi, T. aut Takizawa, M. aut Tamponi, U. aut Tanida, K. aut Tenchini, F. aut Uchida, M. aut Uglov, T. aut Uno, S. aut Usov, Y. aut Van Tonder, R. aut Varner, G. aut Vinokurova, A. aut Vorobyev, V. aut Vossen, A. aut Wang, B. aut Wang, C. H. aut Wang, M.-Z. aut Wang, X. L. aut Watanuki, S. aut Won, E. aut Yang, S. B. aut Ye, H. aut Zhang, Z. P. aut Zhilich, V. aut Zhukova, V. aut Enthalten in Journal of high energy physics Berlin : Springer, 1997 2019(2019), 10 vom: 16. Okt. (DE-627)320910571 (DE-600)2027350-2 1029-8479 nnns volume:2019 year:2019 number:10 day:16 month:10 https://dx.doi.org/10.1007/JHEP10(2019)178 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 2019 2019 10 16 10 |
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englisch |
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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">SPR030571790</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331092649.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/JHEP10(2019)178</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR030571790</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)JHEP10(2019)178-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">Resmi, P. K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s) 2019</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">CKM angle gamma</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">CP violation</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">e+-e- Experiments</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">B physics</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Flavor physics</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Libby, J.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Trabelsi, K.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Adachi, I.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Aihara, H.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Al Said, S.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Asner, D. 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Resmi, P. K. |
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Resmi, P. K. misc CKM angle gamma misc CP violation misc e+-e- Experiments misc B physics misc Flavor physics First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays |
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First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays CKM angle gamma (dpeaa)DE-He213 CP violation (dpeaa)DE-He213 e+-e- Experiments (dpeaa)DE-He213 B physics (dpeaa)DE-He213 Flavor physics (dpeaa)DE-He213 |
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First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays |
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First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays |
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Resmi, P. K. Libby, J. Trabelsi, K. Adachi, I. Aihara, H. Al Said, S. Asner, D. M. Aulchenko, V. Aushev, T. Babu, V. Badhrees, I. Bakich, A. M. Beleño, C. Bennett, J. Bhardwaj, V. Bhuyan, B. Bilka, T. Biswal, J. Bozek, A. Bračko, M. Campajola, M. Červenkov, D. Chen, A. Cheon, B. G. Cho, H. E. Cho, K. Choi, Y. Choudhury, S. Cinabro, D. Cunliffe, S. Dash, N. De Nardo, G. Di Capua, F. Di Carlo, S. Doležal, Z. Dong, T. V. Eidelman, S. Epifanov, D. Fast, J. E. Ferber, T. Fulsom, B. G. Garg, R. Gaur, V. Gabyshev, N. Garmash, A. Giri, A. Goldenzweig, P. Golob, B. Guan, Y. Hayasaka, K. Hayashii, H. Hou, W.-S. Huang, K. Iijima, T. Inami, K. Inguglia, G. Ishikawa, A. Itoh, R. Iwasaki, M. Iwasaki, Y. Jacobs, W. W. Jeon, H. B. Jin, Y. Joffe, D. Kaliyar, A. B. Kang, K. H. Karyan, G. Kawasaki, T. Kiesling, C. Kim, D. Y. Kim, K. T. Kim, S. H. Kinoshita, K. Kodyš, P. Kotchetkov, D. Krǐzan, P. Kroeger, R. Krokovny, P. Kuhr, T. Kumar, R. Kuzmin, A. Kwon, Y.-J. Lee, S. C. Li, Y. B. Lieret, K. Liventsev, D. Lu, P.-C. Luo, T. MacQueen, C. Masuda, M. Matsuda, T. Matvienko, D. Merola, M. Miyabayashi, K. Mizuk, R. Mohanty, G. B. Moon, H. K. Nakano, T. Nakao, M. Nath, K. J. Nayak, M. Niiyama, M. Nisar, N. K. Nishida, S. Nishimura, K. Ogawa, S. Ono, H. Onuki, Y. Pakhlov, P. Pakhlova, G. Pal, B. Pardi, S. Park, H. Pedlar, T. K. Pestotnik, R. Piilonen, L. E. Prencipe, E. Prim, M. T. Ritter, M. Röhrken, M. Russo, G. Sahoo, D. Sakai, Y. Sandilya, S. Santelj, L. Sanuki, T. Savinov, V. Schneider, O. Schnell, G. Schwanda, C. Schwartz, A. J. Seino, Y. Senyo, K. Sevior, M. E. Shebalin, V. Shen, C. P. Shiu, J.-G. Shwartz, B. Solovieva, E. Starič, M. Stottler, Z. S. Strube, J. F. Sumiyoshi, T. Takizawa, M. Tamponi, U. Tanida, K. Tenchini, F. Uchida, M. Uglov, T. Uno, S. Usov, Y. Van Tonder, R. Varner, G. Vinokurova, A. Vorobyev, V. Vossen, A. Wang, B. Wang, C. H. Wang, M.-Z. Wang, X. L. Watanuki, S. Won, E. Yang, S. B. Ye, H. Zhang, Z. P. Zhilich, V. Zhukova, V. |
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Elektronische Aufsätze |
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Resmi, P. K. |
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10.1007/JHEP10(2019)178 |
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first measurement of the ckm angle ϕ3 with b±→ d(%$ {k}_{\mathrm{s}}^0 %$π+π−π0) k± decays |
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First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays |
| abstract |
Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. © The Author(s) 2019 |
| abstractGer |
Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. © The Author(s) 2019 |
| abstract_unstemmed |
Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. The 95% confidence interval on ϕ3 is (−29.7, 109.5)°, which is consistent with the current world average. © The Author(s) 2019 |
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First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays |
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10.1007/JHEP10(2019)178 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR030571790</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331092649.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201007s2019 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/JHEP10(2019)178</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR030571790</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)JHEP10(2019)178-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Resmi, P. K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">First measurement of the CKM angle ϕ3 with B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2019</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s) 2019</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We present the first model-independent measurement of the CKM unitarity triangle angle ϕ3 using B±→ D(%$ {K}_{\mathrm{S}}^0 %$π+π−π0) K± decays, where D indicates either a D0 or %$ \overline{D} %$0 meson. Measurements of the strong-phase difference of the D →%$ {K}_{\mathrm{S}}^0 %$π+π−π0 amplitude obtained from CLEO-c data are used as input. This analysis is based on the full Belle data set of 772 × $ 10^{6} $B%$ \overline{B} %$ events collected at the Υ(4S) resonance. We obtain ϕ3 = (%$ {5.7}_{-8.8}^{+10.2} %$±3.5±5.7)° and the suppressed amplitude ratio rB = 0.323±0.147±0.023±0.051. Here the first uncertainty is statistical, the second is the experimental systematic, and the third is due to the precision of the strong-phase parameters measured from CLEO-c data. 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