Authors
K Abe, P Hamacher-Baumann, E Mazzucato, C Densham, H Kakuno, HM O'Keeffe, A Zalewska, S Joshi, J Holeczek, T Daret, T Maruyama, S Emery-Schrenk, S Aoki, HT Israel, M Reh, M Ikeda, D Munford, MO Wascko, P Mehta, M Laveder, H Sobel, M Grassi, S Nakayama, T Nakaya, N Akhlaq, L Magaletti, J-F Laporte, S Mine, A De Roeck, D Last, M Shiozawa, S Zsoldos, X Lu, K Takifuji, S Manly, M Kawaue, K Kowalik, W Okinaga, S Dolan, M Yokoyama, AJ Finch, C Giganti, S Kuribayashi, M Friend, M Scott, A Bubak, S Hassani, ED Zimmerman, M Gonin, A Bravar, A Dergacheva, Y Nagai, L Mellet, C Vilela, D Sgalaberna, W Li, AK Ichikawa, Y Nishimura, D Wark, MJ Wilking, L Wan, WGS Vinning, A Ershova, ET Atkin, S Fedotov, M Lamers James, Y Hayato, T Kikawa, M Vagins, P Dunne, G Barr, Y Oyama, A Khotjantsev, G Erofeev, K Skwarczynski, Y Lee, A Rubbia, A Nakamura, B Popov, M Zito, AC Kaboth, MD Fitton, L Lavitola, V Matveev, YS Prabhu, K Nagai, S Suvorov, D Douqa, J McElwee, J Lagoda, Y Yoshimoto, S Bordoni, C Dalmazzone, T Nakadaira, T Honjo, RP Litchfield, A Suzuki, J Dumarchez, D Carabadjac, V Berardi, X Zhao, FJP Soler, DGR Martin, A Blanchet, T Holvey, J Kameda, SJ Jenkins, A Ali, C Pidcott, M Ishitsuka, SL Cartwright, F Sánchez, VV Tereshchenko, N Ospina, L Berns, O Mineev, K Nakagiri, E Villa, K Sakashita, JA Caballero, G Vasseur, Y Takeuchi, J Xia, J Zalipska, A Holin, D Payne, S Roth, S Tairafune, R Wendell, A Cudd, E Rondio, L Cook, E Kearns, E Radicioni, D Cherdack, G Eurin, T Kajita, KR Long, A Chvirova, L Marti-Magro, T Nosek, M Martini, LF Thompson, V Paolone, M Batkiewicz-Kwasniak, Y Furui, K Porwit, Y Fujii, K Mahn, T Wachala
Publication date
2023/8/31
Issue
arXiv: 2308.16606
Description
Charged current coherent pion production in (anti) neutrino-nucleus scattering,(−) ν µ+ A→ µ−(+)+ π+(−)+ A, is a process in which a neutrino scatters coherently off a target nucleus. This process leaves the nucleus in its ground state, with the W-boson fluctuating to a charged meson (usually a pion) in the final state. No quantum numbers are exchanged with the nucleus and the magnitude of the square of the four-momentum transfer to the nucleus, denoted as| t|, must be small to maintain coherence. The interaction results in an unchanged nucleus, a lepton and pion in the final state and no other particles. The most common theoretical description of this process is based on Adler’s partially conserved axial vector current (PCAC) theorem [1], which connects the for-
Scholar articles
K Abe, P Hamacher-Baumann, E Mazzucato… - 2023