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Cited 80 time in webofscience Cited 101 time in scopus
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Charm hadrons from fragmentation and B decays in e(+)e(-) annihilation at root s=10.6 GeV

Authors
Seuster, R[Seuster, R]Abe, K[Abe, K]Aihara, H[Aihara, H]Asano, Y[Asano, Y]Aushev, T[Aushev, T]Bakich, AM[Bakich, AM]Barbero, M[Barbero, M]Bedny, I[Bedny, I]Bitenc, U[Bitenc, U]Bizjak, I[Bizjak, I]Bozek, A[Bozek, A]Bracko, M[Bracko, M]Brodzicka, J[Brodzicka, J]Chen, A[Chen, A]Cheon, BG[Cheon, BG]Choi, Y[Choi, Y]Chuvikov, A[Chuvikov, A]Cole, S[Cole, S]Dalseno, J[Dalseno, J]Danilov, M[Danilov, M]Dash, M[Dash, M]Dong, LY[Dong, LY]Dragic, J[Dragic, J]Drutskoy, A[Drutskoy, A]Eidelman, S[Eidelman, S]Fang, F[Fang, F]Gershon, T[Gershon, T]Go, A[Go, A]Gokhroo, G[Gokhroo, G]Golob, B[Golob, B]Gorisek, A[Gorisek, A]Hayasaka, K[Hayasaka, K]Hazumi, M[Hazumi, M]Hoshi, Y[Hoshi, Y]Hou, S[Hou, S]Hou, WS[Hou, WS]Iijima, T[Iijima, T]Ikado, K[Ikado, K]Itoh, R[Itoh, R]Iwasaki, Y[Iwasaki, Y]Kang, JH[Kang, JH]Kang, JS[Kang, JS]Kapusta, P[Kapusta, P]Katayama, N[Katayama, N]Kawai, H[Kawai, H]Kawasaki, T[Kawasaki, T]Khan, HR[Khan, HR]Kichimi, H[Kichimi, H]Kim, HJ[Kim, HJ]Kim, SM[Kim, SM]Krizan, P[Krizan, P]Krokovny, P[Krokovny, P]Kulasiri, R[Kulasiri, R]Kuo, CC[Kuo, CC]Kuzmin, A[Kuzmin, A]Kwon, YJ[Kwon, YJ]Lange, JS[Lange, JS]Lesiak, T[Lesiak, T]Li, J[Li, J]Lin, SW[Lin, SW]Mandl, F[Mandl, F]Mitaroff, W[Mitaroff, W]Miyake, H[Miyake, H]Miyazaki, Y[Miyazaki, Y]Mizuk, R[Mizuk, R]Nagamine, T[Nagamine, T]Nagasaka, Y[Nagasaka, Y]Nakano, E[Nakano, E]Nakao, M[Nakao, M]Nishida, S[Nishida, S]Nitoh, O[Nitoh, O]Ogawa, S[Ogawa, S]Ohshima, T[Ohshima, T]Okabe, T[Okabe, T]Okuno, S[Okuno, S]Olsen, SL[Olsen, SL]Onuki, Y[Onuki, Y]Ozaki, H[Ozaki, H]Pakhlov, P[Pakhlov, P]Palka, H[Palka, H]Park, CW[Park, CW]Park, H[Park, H]Park, KS[Park, KS]Pestotnik, R[Pestotnik, R]Piilonen, LE[Piilonen, LE]Sakai, Y[Sakai, Y]Sato, N[Sato, N]Schietinger, T[Schietinger, T]Schneider, O[Schneider, O]Schumann, J[Schumann, J]Schwanda, C[Schwanda, C]Sevior, ME[Sevior, ME]Shibuya, H[Shibuya, H]Sidorov, V[Sidorov, V]Somov, A[Somov, A]Soni, N[Soni, N]Stamen, R[Stamen, R]Stanic, S[Stanic, S]Staric, M[Staric, M]Suzuki, SY[Suzuki, SY]Takasaki, F[Takasaki, F]Tamai, K[Tamai, K]Tamura, N[Tamura, N]Tanaka, M[Tanaka, M]Taylor, GN[Taylor, GN]Teramoto, Y[Teramoto, Y]Tian, XC[Tian, XC]Uehara, S[Uehara, S]Uglov, T[Uglov, T]Ueno, K[Ueno, K]Uno, S[Uno, S]Urquijo, P[Urquijo, P]Varner, G[Varner, G]Wang, CC[Wang, CC]Wang, CH[Wang, CH]Wang, MZ[Wang, MZ]Xie, QL[Xie, QL]Yabsley, BD[Yabsley, BD]Yamaguchi, A[Yamaguchi, A]Yamashita, Y[Yamashita, Y]Yamauchi, M[Yamauchi, M]Ying, J[Ying, J]Yusa, Y[Yusa, Y]Zhang, LM[Zhang, LM]Zhang, ZP[Zhang, ZP]Zhilich, V[Zhilich, V]
Issue Date
Feb-2006
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW D, v.73, no.3
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW D
Volume
73
Number
3
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/87650
DOI
10.1103/PhysRevD.73.032002
ISSN
1550-7998
Abstract
We present an analysis of charm quark fragmentation at 10.6 GeV, based on a data sample of 103 fb(-1) collected by the Belle detector at the KEKB accelerator. We consider fragmentation into the main charmed hadron ground states, namely D-0,D+,D-s(+) and Lambda(c)(+), as well as the excited states D-*0 and D*+. The fragmentation functions are important to measure as they describe processes at a low energy scale, where calculations in perturbation theory lead to large uncertainties. Fragmentation functions can also be used as input distributions for Monte Carlo generators. Additionally, we determine the average number of these charmed hadrons produced per B decay at the Upsilon(4S) resonance and measure the distribution of their production angle in e(+)e(-) annihilation events and in B decays.
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