BibTex format
@inproceedings{Tada:2024,
author = {Tada, T and Nakano, Y and Koshio, Y and Abe, K and Bronner, C and Hayato, Y and Hiraide, K and Hosokawa, K and Ieki, K and Ikeda, M and Kameda, J and Kanemura, Y and Kaneshima, R and Kashiwagi, Y and Kataoka, Y and Miki, S and Mine, S and Miura, M and Moriyama, S and Nakano, Y and Nakahata, M and Nakayama, S and Noguchi, Y and Sato, K and Sekiya, H and Shiba, H and Shimizu, K and Shiozawa, M and Sonoda, Y and Suzuki, Y and Takeda, A and Takemoto, Y and Tanaka, H and Yano, T and Han, S and Kajita, T and Okumura, K and Tashiro, T and Tomiya, T and Wang, X and Yoshida, S and Fernandez, P and Labarga, L and Ospina, N and Zaldivar, B and Pointon, BW and Kearns, E and Raaf, JL and Wan, L and Wester, T and Bian, J and Griskevich, NJ and Locke, S and Smy, MB and Sobel, HW and Takhistov, V and Yankelevich, A and Hill, J and Lee, SH and Moon, DH and Park, RG and Bodur, B and Scholberg, K and Walter, CW and Beauchêne, A and Drapier, O and Giampaolo, A and Mueller, TA and Santos, AD and Paga},
title = {Measurement of the kaon to pion production ratio with the Super-Kamiokande},
year = {2024}
}
RIS format (EndNote, RefMan)
TY - CPAPER
AB - Cosmic-ray muons are generated from the decay of mesons which are secondary particles produced via hadronic interaction between primary cosmic-ray particles and atmospheric nuclei at the upper the atmosphere. The mesons such pions and kaons mostly decay into muons immediately, reflecting the details of the hadronic interactions depending on their energy and lifetime. The modulation of the cosmic-ray muon rate as well as the flux and the atmospheric kaon-to-pion production ratio are important to determine the flux and energy of the atmospheric neutrino. In particular, the kaon-to-pion production ratio r<inf>K/π</inf> is measured with the correlation coefficient α<inf>T</inf> between the cosmic-ray muon rate in the underground detector and the atmospheric temperature. As a result, we obtained the correlation coefficient r<inf>K/π</inf> = 0.85 ± 0.01 (statistical uncertainty only) and r<inf>K/π</inf> = 0.12 ± 0.03 (statistical uncertainty only) using the data taken in 10 years at the Super-Kamiokande detector. In this article, we report the current status of measurement of the modulation of the comic-ray muon and the atmospheric kaon-to-pion production ratio.
AU - Tada,T
AU - Nakano,Y
AU - Koshio,Y
AU - Abe,K
AU - Bronner,C
AU - Hayato,Y
AU - Hiraide,K
AU - Hosokawa,K
AU - Ieki,K
AU - Ikeda,M
AU - Kameda,J
AU - Kanemura,Y
AU - Kaneshima,R
AU - Kashiwagi,Y
AU - Kataoka,Y
AU - Miki,S
AU - Mine,S
AU - Miura,M
AU - Moriyama,S
AU - Nakano,Y
AU - Nakahata,M
AU - Nakayama,S
AU - Noguchi,Y
AU - Sato,K
AU - Sekiya,H
AU - Shiba,H
AU - Shimizu,K
AU - Shiozawa,M
AU - Sonoda,Y
AU - Suzuki,Y
AU - Takeda,A
AU - Takemoto,Y
AU - Tanaka,H
AU - Yano,T
AU - Han,S
AU - Kajita,T
AU - Okumura,K
AU - Tashiro,T
AU - Tomiya,T
AU - Wang,X
AU - Yoshida,S
AU - Fernandez,P
AU - Labarga,L
AU - Ospina,N
AU - Zaldivar,B
AU - Pointon,BW
AU - Kearns,E
AU - Raaf,JL
AU - Wan,L
AU - Wester,T
AU - Bian,J
AU - Griskevich,NJ
AU - Locke,S
AU - Smy,MB
AU - Sobel,HW
AU - Takhistov,V
AU - Yankelevich,A
AU - Hill,J
AU - Lee,SH
AU - Moon,DH
AU - Park,RG
AU - Bodur,B
AU - Scholberg,K
AU - Walter,CW
AU - Beauchêne,A
AU - Drapier,O
AU - Giampaolo,A
AU - Mueller,TA
AU - Santos,AD
AU - Paganini,P
AU - Quilain,B
AU - Nakamura,T
AU - Jang,JS
AU - Machado,LN
AU - Learned,JG
AU - Choi,K
AU - Iovine,N
AU - Cao,S
AU - Anthony,LHV
AU - Martin,D
AU - Prouse,NW
AU - Scott,M
AU - Sztuc,AA
AU - Uchida,Y
AU - Berardi,V
AU - Catanesi,MG
AU - Radicioni,E
AU - Calabria,NF
AU - Langella,A
AU - De,Rosa G
AU - Collazuol,G
AU - Iacob,F
AU - Mattiazzi,M
AU - Ludovici,L
AU - Gonin,M
AU - Pronost,G
AU - Fujisawa,C
AU - Maekawa,Y
AU - Nishimura,Y
AU - Okazaki,R
PY - 2024///
TI - Measurement of the kaon to pion production ratio with the Super-Kamiokande
ER -