Angular analysis of $B \to K^ e^+ e^-$ in the low-$q^2$ region with new electron identification at Belle

We perform an angular analysis of the $B\to K^* e^+ e^-$ decay for the dielectron mass squared, $q^2$, range of $0.0008$ to $1.1200 ~\text{GeV}^2 /c^4$ using the full Belle data set in the $K^{*0} \to K^+ \pi^-$ and $K^{*+} \to K_S^0 \pi^+$ channels, incorporating new methods of electron identificat...

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Hauptverfasser: Ferlewicz, D, Urquijo, P, Adamczyk, K, Aihara, H, Asner, D. M, Ayad, R, Banerjee, Sw, Behera, P, Bennett, J, Bessner, M, Bilka, T, Biswas, D, Bodrov, D, Campajola, M, Červenkov, D, Cheon, B. G, Cho, H. E, Choi, S. -K, Choi, Y, Choudhury, S, Das, S, De Pietro, G, Dhamija, R, Di Capua, F, Dingfelder, J, Doležal, Z, Dong, T. V, Ecker, P, Epifanov, D, Ferber, T, Garmash, A, Giri, A, Gu, T, Guan, Y, Hazra, S, Itoh, R, Jin, Y, Kaliyar, A. B, Kiesling, C, Kim, C. H, Kim, D. Y, Kim, K. -H, Kinoshita, K, Kodyš, P, Konno, T, Korobov, A, Korpar, S, Kou, E, Kovalenko, E, Križan, P, Kumar, R, Kwon, Y. -J, Lai, Y. -T, Lam, T, Lee, S. C, Levit, D, Lewis, P, Li, Y. B, Libby, J, Matvienko, D, Meier, F, Metzner, F, Miyabayashi, K, Mizuk, R, Nakamura, I, Natochii, A, Nishida, S, Ogawa, S, Ono, H, Pardi, S, Park, J, Passeri, A, Patra, S, Paul, S, Pedlar, T. K, Podobnik, T, Prim, M. T, Rout, N, Russo, G, Sandilya, S, Savinov, V, Seino, Y, Sevior, M. E, Shan, W, Sharma, C, Shwartz, B, Tamponi, U, Tenchini, F, Unno, Y, Ushiroda, Y, Varvell, K. E, Wang, E, Watanuki, S, Yan, W, Yelton, J, Yin, J. H, Yuan, L, Yusa, Y, Zhang, Z. P, Zhukova, V
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creator Ferlewicz, D
Urquijo, P
Adamczyk, K
Aihara, H
Asner, D. M
Ayad, R
Banerjee, Sw
Behera, P
Bennett, J
Bessner, M
Bilka, T
Biswas, D
Bodrov, D
Campajola, M
Červenkov, D
Cheon, B. G
Cho, H. E
Choi, S. -K
Choi, Y
Choudhury, S
Das, S
De Pietro, G
Dhamija, R
Di Capua, F
Dingfelder, J
Doležal, Z
Dong, T. V
Ecker, P
Epifanov, D
Ferber, T
Garmash, A
Giri, A
Gu, T
Guan, Y
Hazra, S
Itoh, R
Jin, Y
Kaliyar, A. B
Kiesling, C
Kim, C. H
Kim, D. Y
Kim, K. -H
Kinoshita, K
Kodyš, P
Konno, T
Korobov, A
Korpar, S
Kou, E
Kovalenko, E
Križan, P
Kumar, R
Kwon, Y. -J
Lai, Y. -T
Lam, T
Lee, S. C
Levit, D
Lewis, P
Li, Y. B
Libby, J
Matvienko, D
Meier, F
Metzner, F
Miyabayashi, K
Mizuk, R
Nakamura, I
Natochii, A
Nishida, S
Ogawa, S
Ono, H
Pardi, S
Park, J
Passeri, A
Patra, S
Paul, S
Pedlar, T. K
Podobnik, T
Prim, M. T
Rout, N
Russo, G
Sandilya, S
Savinov, V
Seino, Y
Sevior, M. E
Shan, W
Sharma, C
Shwartz, B
Tamponi, U
Tenchini, F
Unno, Y
Ushiroda, Y
Varvell, K. E
Wang, E
Watanuki, S
Yan, W
Yelton, J
Yin, J. H
Yuan, L
Yusa, Y
Zhang, Z. P
Zhukova, V
description We perform an angular analysis of the $B\to K^* e^+ e^-$ decay for the dielectron mass squared, $q^2$, range of $0.0008$ to $1.1200 ~\text{GeV}^2 /c^4$ using the full Belle data set in the $K^{*0} \to K^+ \pi^-$ and $K^{*+} \to K_S^0 \pi^+$ channels, incorporating new methods of electron identification to improve the statistical power of the data set. This analysis is sensitive to contributions from right-handed currents from physics beyond the Standard Model by constraining the Wilson coefficients $\mathcal{C}_7^{(\prime)}$. We perform a fit to the $B\to K^* e^+ e^-$ differential decay rate and measure the imaginary component of the transversality amplitude to be $A_T^{\rm Im} = -1.27 \pm 0.52 \pm 0.12$, and the $K^*$ transverse asymmetry to be $A_T^{(2)} = 0.52 \pm 0.53 \pm 0.11$, with $F_L$ and $A_T^{\rm Re}$ fixed to the Standard Model values. The resulting constraints on the value of $\mathcal{C}_7^{\prime}$ are consistent with the Standard Model within a $2\sigma$ confidence interval.
doi_str_mv 10.48550/arxiv.2404.00201
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M ; Ayad, R ; Banerjee, Sw ; Behera, P ; Bennett, J ; Bessner, M ; Bilka, T ; Biswas, D ; Bodrov, D ; Campajola, M ; Červenkov, D ; Cheon, B. G ; Cho, H. E ; Choi, S. -K ; Choi, Y ; Choudhury, S ; Das, S ; De Pietro, G ; Dhamija, R ; Di Capua, F ; Dingfelder, J ; Doležal, Z ; Dong, T. V ; Ecker, P ; Epifanov, D ; Ferber, T ; Garmash, A ; Giri, A ; Gu, T ; Guan, Y ; Hazra, S ; Itoh, R ; Jin, Y ; Kaliyar, A. B ; Kiesling, C ; Kim, C. H ; Kim, D. Y ; Kim, K. -H ; Kinoshita, K ; Kodyš, P ; Konno, T ; Korobov, A ; Korpar, S ; Kou, E ; Kovalenko, E ; Križan, P ; Kumar, R ; Kwon, Y. -J ; Lai, Y. -T ; Lam, T ; Lee, S. C ; Levit, D ; Lewis, P ; Li, Y. B ; Libby, J ; Matvienko, D ; Meier, F ; Metzner, F ; Miyabayashi, K ; Mizuk, R ; Nakamura, I ; Natochii, A ; Nishida, S ; Ogawa, S ; Ono, H ; Pardi, S ; Park, J ; Passeri, A ; Patra, S ; Paul, S ; Pedlar, T. K ; Podobnik, T ; Prim, M. T ; Rout, N ; Russo, G ; Sandilya, S ; Savinov, V ; Seino, Y ; Sevior, M. 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This analysis is sensitive to contributions from right-handed currents from physics beyond the Standard Model by constraining the Wilson coefficients $\mathcal{C}_7^{(\prime)}$. We perform a fit to the $B\to K^* e^+ e^-$ differential decay rate and measure the imaginary component of the transversality amplitude to be $A_T^{\rm Im} = -1.27 \pm 0.52 \pm 0.12$, and the $K^*$ transverse asymmetry to be $A_T^{(2)} = 0.52 \pm 0.53 \pm 0.11$, with $F_L$ and $A_T^{\rm Re}$ fixed to the Standard Model values. 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P</creatorcontrib><creatorcontrib>Zhukova, V</creatorcontrib><title>Angular analysis of $B \to K^ e^+ e^-$ in the low-$q^2$ region with new electron identification at Belle</title><description>We perform an angular analysis of the $B\to K^* e^+ e^-$ decay for the dielectron mass squared, $q^2$, range of $0.0008$ to $1.1200 ~\text{GeV}^2 /c^4$ using the full Belle data set in the $K^{*0} \to K^+ \pi^-$ and $K^{*+} \to K_S^0 \pi^+$ channels, incorporating new methods of electron identification to improve the statistical power of the data set. This analysis is sensitive to contributions from right-handed currents from physics beyond the Standard Model by constraining the Wilson coefficients $\mathcal{C}_7^{(\prime)}$. We perform a fit to the $B\to K^* e^+ e^-$ differential decay rate and measure the imaginary component of the transversality amplitude to be $A_T^{\rm Im} = -1.27 \pm 0.52 \pm 0.12$, and the $K^*$ transverse asymmetry to be $A_T^{(2)} = 0.52 \pm 0.53 \pm 0.11$, with $F_L$ and $A_T^{\rm Re}$ fixed to the Standard Model values. The resulting constraints on the value of $\mathcal{C}_7^{\prime}$ are consistent with the Standard Model within a $2\sigma$ confidence interval.</description><subject>Physics - High Energy Physics - Experiment</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotj71OwzAYRbMwoMIDMPEN2VCC7fgvY1vxU1GJpSNK9CWxG0vGgcQQ-va0heHqSldHVzpJckNJzrUQ5B7HH_edM054Tggj9DLpl2H_5XEEDOgPk5tgsJCu4C0O8FKBqe6OyVJwAWJvwA9zln5WLIXR7N0QYHaxh2BmMN60cTwurjMhOutajCcAI6yM9-YqubDoJ3P934tk9_iwWz9n29enzXq5zVAqmmmpiKANEtZ0lCG2QkuOVBdCGoWltNYKqVVptbQcC0GV6EjLFJKC264pi0Vy-3d7Vq0_RveO46E-Kddn5eIXcghPLw</recordid><startdate>20240329</startdate><enddate>20240329</enddate><creator>Ferlewicz, D</creator><creator>Urquijo, P</creator><creator>Adamczyk, K</creator><creator>Aihara, H</creator><creator>Asner, D. 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B</creatorcontrib><creatorcontrib>Libby, J</creatorcontrib><creatorcontrib>Matvienko, D</creatorcontrib><creatorcontrib>Meier, F</creatorcontrib><creatorcontrib>Metzner, F</creatorcontrib><creatorcontrib>Miyabayashi, K</creatorcontrib><creatorcontrib>Mizuk, R</creatorcontrib><creatorcontrib>Nakamura, I</creatorcontrib><creatorcontrib>Natochii, A</creatorcontrib><creatorcontrib>Nishida, S</creatorcontrib><creatorcontrib>Ogawa, S</creatorcontrib><creatorcontrib>Ono, H</creatorcontrib><creatorcontrib>Pardi, S</creatorcontrib><creatorcontrib>Park, J</creatorcontrib><creatorcontrib>Passeri, A</creatorcontrib><creatorcontrib>Patra, S</creatorcontrib><creatorcontrib>Paul, S</creatorcontrib><creatorcontrib>Pedlar, T. K</creatorcontrib><creatorcontrib>Podobnik, T</creatorcontrib><creatorcontrib>Prim, M. 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P</creatorcontrib><creatorcontrib>Zhukova, V</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Ferlewicz, D</au><au>Urquijo, P</au><au>Adamczyk, K</au><au>Aihara, H</au><au>Asner, D. M</au><au>Ayad, R</au><au>Banerjee, Sw</au><au>Behera, P</au><au>Bennett, J</au><au>Bessner, M</au><au>Bilka, T</au><au>Biswas, D</au><au>Bodrov, D</au><au>Campajola, M</au><au>Červenkov, D</au><au>Cheon, B. G</au><au>Cho, H. E</au><au>Choi, S. -K</au><au>Choi, Y</au><au>Choudhury, S</au><au>Das, S</au><au>De Pietro, G</au><au>Dhamija, R</au><au>Di Capua, F</au><au>Dingfelder, J</au><au>Doležal, Z</au><au>Dong, T. V</au><au>Ecker, P</au><au>Epifanov, D</au><au>Ferber, T</au><au>Garmash, A</au><au>Giri, A</au><au>Gu, T</au><au>Guan, Y</au><au>Hazra, S</au><au>Itoh, R</au><au>Jin, Y</au><au>Kaliyar, A. B</au><au>Kiesling, C</au><au>Kim, C. H</au><au>Kim, D. Y</au><au>Kim, K. -H</au><au>Kinoshita, K</au><au>Kodyš, P</au><au>Konno, T</au><au>Korobov, A</au><au>Korpar, S</au><au>Kou, E</au><au>Kovalenko, E</au><au>Križan, P</au><au>Kumar, R</au><au>Kwon, Y. -J</au><au>Lai, Y. -T</au><au>Lam, T</au><au>Lee, S. C</au><au>Levit, D</au><au>Lewis, P</au><au>Li, Y. B</au><au>Libby, J</au><au>Matvienko, D</au><au>Meier, F</au><au>Metzner, F</au><au>Miyabayashi, K</au><au>Mizuk, R</au><au>Nakamura, I</au><au>Natochii, A</au><au>Nishida, S</au><au>Ogawa, S</au><au>Ono, H</au><au>Pardi, S</au><au>Park, J</au><au>Passeri, A</au><au>Patra, S</au><au>Paul, S</au><au>Pedlar, T. K</au><au>Podobnik, T</au><au>Prim, M. T</au><au>Rout, N</au><au>Russo, G</au><au>Sandilya, S</au><au>Savinov, V</au><au>Seino, Y</au><au>Sevior, M. E</au><au>Shan, W</au><au>Sharma, C</au><au>Shwartz, B</au><au>Tamponi, U</au><au>Tenchini, F</au><au>Unno, Y</au><au>Ushiroda, Y</au><au>Varvell, K. E</au><au>Wang, E</au><au>Watanuki, S</au><au>Yan, W</au><au>Yelton, J</au><au>Yin, J. H</au><au>Yuan, L</au><au>Yusa, Y</au><au>Zhang, Z. P</au><au>Zhukova, V</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Angular analysis of $B \to K^ e^+ e^-$ in the low-$q^2$ region with new electron identification at Belle</atitle><date>2024-03-29</date><risdate>2024</risdate><abstract>We perform an angular analysis of the $B\to K^* e^+ e^-$ decay for the dielectron mass squared, $q^2$, range of $0.0008$ to $1.1200 ~\text{GeV}^2 /c^4$ using the full Belle data set in the $K^{*0} \to K^+ \pi^-$ and $K^{*+} \to K_S^0 \pi^+$ channels, incorporating new methods of electron identification to improve the statistical power of the data set. This analysis is sensitive to contributions from right-handed currents from physics beyond the Standard Model by constraining the Wilson coefficients $\mathcal{C}_7^{(\prime)}$. We perform a fit to the $B\to K^* e^+ e^-$ differential decay rate and measure the imaginary component of the transversality amplitude to be $A_T^{\rm Im} = -1.27 \pm 0.52 \pm 0.12$, and the $K^*$ transverse asymmetry to be $A_T^{(2)} = 0.52 \pm 0.53 \pm 0.11$, with $F_L$ and $A_T^{\rm Re}$ fixed to the Standard Model values. The resulting constraints on the value of $\mathcal{C}_7^{\prime}$ are consistent with the Standard Model within a $2\sigma$ confidence interval.</abstract><doi>10.48550/arxiv.2404.00201</doi><oa>free_for_read</oa></addata></record>
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identifier DOI: 10.48550/arxiv.2404.00201
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subjects Physics - High Energy Physics - Experiment
title Angular analysis of $B \to K^ e^+ e^-$ in the low-$q^2$ region with new electron identification at Belle
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