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Inclusive quarkonium production at forward rapidity in pp collisions at Formula: see textTeV
by
Mitra, J
, Murray, S
, Ahammed, Z
, Moreno, L A P
, Fabbietti, L
, Gaardhøje, J J
, Bhat, I R
, Závada, P
, Nair, R
, Fuchs, U
, Jimenez Bustamante, R T
, Cheynis, B
, Cruz Albino, R
, Caliva, A
, Breitner, T
, Margutti, J
, Westerhoff, U
, Martínez García, G
, Evans, D
, Goméz Coral, D M
, Pluta, J
, Sano, M
, Agrawal, N
, Conesa Balbastre, G
, Hayashi, S
, Scapparone, E
, Bercuci, A
, Rami, F
, Cherney, M
, Zaviyalov, N
, Passfeld, A
, Pestov, Y
, Baral, R C
, Zaman, A
, Rathee, D
, Gotovac, S
, Wilk, G
, Chujo, T
, Manso, F
, Batyunya, B
, Hamagaki, H
, Altsybeev, I
, Kubera, A M
, Zardoshti, N
, Mühlheim, D
, Germain, M
, Jang, H J
, Röhrich, D
, Böttger, S
, Naru, M U
, Riggi, F
, Berenyi, D
, Kalweit, A
, Shangaraev, A
, Schweda, K
, Yoo, I-K
, Grelli, A
, Kluge, A
, Shabanov, A
, Cifarelli, L
, Giubellino, P
, Jadhav, M B
, Mishra, A N
, Barnaföldi, G G
, Płoskoń, M
, Kamin, J
, Sandoval, A
, Elia, D
, Nooren, G
, Lee, S
, Sultanov, R
, Glässel, P
, Ng, F
, Poljak, N
, Gonzalez, V
, Jusko, A
, Karavichev, O
, Melikyan, Y
, Suire, C
, Ricci, R A
, Shahoyan, R
, Yin, Z
, Lattuca, A
, Yushmanov, I
, Mohammadi, N
, Gladysz-Dziadus, E
, Kollegger, T
, Kučera, V
, Shigaki, K
, Chelnokov, V
, Kileng, B
, Chang, B
, Bedda, C
, Hippolyte, B
, Khan, P
, Vargyas, M
, Sinh
2016
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Inclusive quarkonium production at forward rapidity in pp collisions at Formula: see textTeV
by
Mitra, J
, Murray, S
, Ahammed, Z
, Moreno, L A P
, Fabbietti, L
, Gaardhøje, J J
, Bhat, I R
, Závada, P
, Nair, R
, Fuchs, U
, Jimenez Bustamante, R T
, Cheynis, B
, Cruz Albino, R
, Caliva, A
, Breitner, T
, Margutti, J
, Westerhoff, U
, Martínez García, G
, Evans, D
, Goméz Coral, D M
, Pluta, J
, Sano, M
, Agrawal, N
, Conesa Balbastre, G
, Hayashi, S
, Scapparone, E
, Bercuci, A
, Rami, F
, Cherney, M
, Zaviyalov, N
, Passfeld, A
, Pestov, Y
, Baral, R C
, Zaman, A
, Rathee, D
, Gotovac, S
, Wilk, G
, Chujo, T
, Manso, F
, Batyunya, B
, Hamagaki, H
, Altsybeev, I
, Kubera, A M
, Zardoshti, N
, Mühlheim, D
, Germain, M
, Jang, H J
, Röhrich, D
, Böttger, S
, Naru, M U
, Riggi, F
, Berenyi, D
, Kalweit, A
, Shangaraev, A
, Schweda, K
, Yoo, I-K
, Grelli, A
, Kluge, A
, Shabanov, A
, Cifarelli, L
, Giubellino, P
, Jadhav, M B
, Mishra, A N
, Barnaföldi, G G
, Płoskoń, M
, Kamin, J
, Sandoval, A
, Elia, D
, Nooren, G
, Lee, S
, Sultanov, R
, Glässel, P
, Ng, F
, Poljak, N
, Gonzalez, V
, Jusko, A
, Karavichev, O
, Melikyan, Y
, Suire, C
, Ricci, R A
, Shahoyan, R
, Yin, Z
, Lattuca, A
, Yushmanov, I
, Mohammadi, N
, Gladysz-Dziadus, E
, Kollegger, T
, Kučera, V
, Shigaki, K
, Chelnokov, V
, Kileng, B
, Chang, B
, Bedda, C
, Hippolyte, B
, Khan, P
, Vargyas, M
, Sinh
in
2016
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Inclusive quarkonium production at forward rapidity in pp collisions at Formula: see textTeV
by
Mitra, J
, Murray, S
, Ahammed, Z
, Moreno, L A P
, Fabbietti, L
, Gaardhøje, J J
, Bhat, I R
, Závada, P
, Nair, R
, Fuchs, U
, Jimenez Bustamante, R T
, Cheynis, B
, Cruz Albino, R
, Caliva, A
, Breitner, T
, Margutti, J
, Westerhoff, U
, Martínez García, G
, Evans, D
, Goméz Coral, D M
, Pluta, J
, Sano, M
, Agrawal, N
, Conesa Balbastre, G
, Hayashi, S
, Scapparone, E
, Bercuci, A
, Rami, F
, Cherney, M
, Zaviyalov, N
, Passfeld, A
, Pestov, Y
, Baral, R C
, Zaman, A
, Rathee, D
, Gotovac, S
, Wilk, G
, Chujo, T
, Manso, F
, Batyunya, B
, Hamagaki, H
, Altsybeev, I
, Kubera, A M
, Zardoshti, N
, Mühlheim, D
, Germain, M
, Jang, H J
, Röhrich, D
, Böttger, S
, Naru, M U
, Riggi, F
, Berenyi, D
, Kalweit, A
, Shangaraev, A
, Schweda, K
, Yoo, I-K
, Grelli, A
, Kluge, A
, Shabanov, A
, Cifarelli, L
, Giubellino, P
, Jadhav, M B
, Mishra, A N
, Barnaföldi, G G
, Płoskoń, M
, Kamin, J
, Sandoval, A
, Elia, D
, Nooren, G
, Lee, S
, Sultanov, R
, Glässel, P
, Ng, F
, Poljak, N
, Gonzalez, V
, Jusko, A
, Karavichev, O
, Melikyan, Y
, Suire, C
, Ricci, R A
, Shahoyan, R
, Yin, Z
, Lattuca, A
, Yushmanov, I
, Mohammadi, N
, Gladysz-Dziadus, E
, Kollegger, T
, Kučera, V
, Shigaki, K
, Chelnokov, V
, Kileng, B
, Chang, B
, Bedda, C
, Hippolyte, B
, Khan, P
, Vargyas, M
, Sinh
2016
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Inclusive quarkonium production at forward rapidity in pp collisions at Formula: see textTeV
Journal Article
Inclusive quarkonium production at forward rapidity in pp collisions at Formula: see textTeV
2016
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Overview
We report on the inclusive production cross sections of [Formula: see text], [Formula: see text], [Formula: see text](1S), [Formula: see text](2S) and [Formula: see text](3S), measured at forward rapidity with the ALICE detector in [Formula: see text] collisions at a center-of-mass energy [Formula: see text] TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb[Formula: see text]. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum [Formula: see text] and rapidity y, over the [Formula: see text] ranges [Formula: see text] GeV/c for [Formula: see text], [Formula: see text] GeV/c for all other resonances, and for [Formula: see text]. The cross sections, integrated over [Formula: see text] and y, and assuming unpolarized quarkonia, are [Formula: see text] [Formula: see text]b, [Formula: see text] [Formula: see text]b, [Formula: see text] nb, [Formula: see text] nb and [Formula: see text] nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most [Formula: see text], with measurements performed by the LHCb collaboration in the same rapidity range.We report on the inclusive production cross sections of [Formula: see text], [Formula: see text], [Formula: see text](1S), [Formula: see text](2S) and [Formula: see text](3S), measured at forward rapidity with the ALICE detector in [Formula: see text] collisions at a center-of-mass energy [Formula: see text] TeV. The analysis is based on data collected at the LHC and corresponds to an integrated luminosity of 1.23 pb[Formula: see text]. Quarkonia are reconstructed in the dimuon-decay channel. The differential production cross sections are measured as a function of the transverse momentum [Formula: see text] and rapidity y, over the [Formula: see text] ranges [Formula: see text] GeV/c for [Formula: see text], [Formula: see text] GeV/c for all other resonances, and for [Formula: see text]. The cross sections, integrated over [Formula: see text] and y, and assuming unpolarized quarkonia, are [Formula: see text] [Formula: see text]b, [Formula: see text] [Formula: see text]b, [Formula: see text] nb, [Formula: see text] nb and [Formula: see text] nb, where the first uncertainty is statistical and the second one is systematic. These values agree, within at most [Formula: see text], with measurements performed by the LHCb collaboration in the same rapidity range.
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