An improved search for the electric dipole moment of the τ lepton

A bstract We report a measurement of the electric dipole moment of the τ lepton ( dτ ) using an 833 fb − 1 data sample collected near the Υ(4 S ) resonance, with the Belle detector at the KEKB asymmetric-energy e + e − collider. Using an optimal observable method, we obtain the real and imaginary pa...

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Veröffentlicht in:The journal of high energy physics 2022-04, Vol.2022 (4), p.110-17, Article 110
Hauptverfasser: Inami, K., Asner, D. M., Aulchenko, V., Aushev, T., Ayad, R., Bahinipati, S., Bessner, M., Bhuyan, B., Bilka, T., Biswal, J., Bobrov, A., Bonvicini, G., Bozek, A., Cheon, B. G., Cho, H. E., Cho, K., Choi, Y., Das, S., De Nardo, G., Dhamija, R., Di Capua, F., Doležal, Z., Dong, T. V., Eidelman, S., Epifanov, D., Ferber, T., Garg, R., Gaur, V., Gabyshev, N., Golob, B., Greenwald, D., Gudkova, K., Hadjivasiliou, C., Hartbrich, O., Hayashii, H., Hou, W.-S., Iijima, T., Itoh, R., Jang, E.-J., Joo, C. W., Joo, K. K., Kato, Y., Kichimi, H., Kim, S. H., Kim, Y.-K., Kimmel, T. D., Kodyš, P., Konno, T., Križan, P., Kroeger, R., Krokovny, P., Kulasiri, R., Kumar, M., Kumara, K., Lalwani, K., Lange, J. S., Li, C. H., Li, L. K., Li, Y. B., Gioi, L. Li, Libby, J., Masuda, M., Matvienko, D., Metzner, F., Mizuk, R., Mohanty, G. B., Mohanty, S., Moon, T. J., Nayak, L., Nayak, M., Pardi, S., Pedlar, T. K., Podobnik, T., Prencipe, E., Rabusov, A., Rostomyan, A., Russo, G., Sahoo, D., Sandilya, S., Savinov, V., Schnell, G., Schwanda, C., Senyo, K., Sevior, M. E., Sharma, C., Solovieva, E., Strube, J. F., Sutcliffe, W., Tenchini, F., Trabelsi, K., Uchida, M., Uehara, S., Uno, S., Vinokurova, A., Wang, C. H., Watanabe, M., Watanuki, S., Zhang, Z. P., Zhilich, V., Zhukova, V.
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Sprache:eng
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Zusammenfassung:A bstract We report a measurement of the electric dipole moment of the τ lepton ( dτ ) using an 833 fb − 1 data sample collected near the Υ(4 S ) resonance, with the Belle detector at the KEKB asymmetric-energy e + e − collider. Using an optimal observable method, we obtain the real and imaginary parts of d τ as Re( d τ ) = ( − 0 . 62 ± 0 . 63) × 10 − 17 e cm and Im( d τ ) = ( − 0 . 40 ± 0 . 32) × 10 − 17 e cm, respectively. These results are consistent with null electric dipole moment at the present level of experimental sensitivity and improve the sensitivity by about a factor of three.
ISSN:1029-8479
1126-6708
1029-8479
DOI:10.1007/JHEP04(2022)110