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Production of KFormula: see text(892)Formula: see text and Formula: see text(1020) in p-Pb collisions at Formula: see text = 5.02 TeV
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
, Incani, E
, 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
, Balasubramanian, S
, 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
, 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
2016
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Production of KFormula: see text(892)Formula: see text and Formula: see text(1020) in p-Pb collisions at Formula: see text = 5.02 TeV
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
, Incani, E
, 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
, Balasubramanian, S
, 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
, 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
in
2016
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Production of KFormula: see text(892)Formula: see text and Formula: see text(1020) in p-Pb collisions at Formula: see text = 5.02 TeV
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
, Incani, E
, 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
, Balasubramanian, S
, 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
, 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
2016
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Production of KFormula: see text(892)Formula: see text and Formula: see text(1020) in p-Pb collisions at Formula: see text = 5.02 TeV
Journal Article
Production of KFormula: see text(892)Formula: see text and Formula: see text(1020) in p-Pb collisions at Formula: see text = 5.02 TeV
2016
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Overview
The production of K[Formula: see text](892)[Formula: see text] and [Formula: see text](1020) mesons has been measured in p-Pb collisions at [Formula: see text][Formula: see text] 5.02 TeV. K[Formula: see text] and [Formula: see text] are reconstructed via their decay into charged hadrons with the ALICE detector in the rapidity range [Formula: see text]. The transverse momentum spectra, measured as a function of the multiplicity, have a p[Formula: see text] range from 0 to 15 GeV/c for K[Formula: see text] and from 0.3 to 21 GeV/c for [Formula: see text]. Integrated yields, mean transverse momenta and particle ratios are reported and compared with results in pp collisions at [Formula: see text][Formula: see text] 7 TeV and Pb-Pb collisions at [Formula: see text][Formula: see text] 2.76 TeV. In Pb-Pb and p-Pb collisions, K[Formula: see text] and [Formula: see text] probe the hadronic phase of the system and contribute to the study of particle formation mechanisms by comparison with other identified hadrons. For this purpose, the mean transverse momenta and the differential proton-to-[Formula: see text] ratio are discussed as a function of the multiplicity of the event. The short-lived K[Formula: see text] is measured to investigate re-scattering effects, believed to be related to the size of the system and to the lifetime of the hadronic phase.The production of K[Formula: see text](892)[Formula: see text] and [Formula: see text](1020) mesons has been measured in p-Pb collisions at [Formula: see text][Formula: see text] 5.02 TeV. K[Formula: see text] and [Formula: see text] are reconstructed via their decay into charged hadrons with the ALICE detector in the rapidity range [Formula: see text]. The transverse momentum spectra, measured as a function of the multiplicity, have a p[Formula: see text] range from 0 to 15 GeV/c for K[Formula: see text] and from 0.3 to 21 GeV/c for [Formula: see text]. Integrated yields, mean transverse momenta and particle ratios are reported and compared with results in pp collisions at [Formula: see text][Formula: see text] 7 TeV and Pb-Pb collisions at [Formula: see text][Formula: see text] 2.76 TeV. In Pb-Pb and p-Pb collisions, K[Formula: see text] and [Formula: see text] probe the hadronic phase of the system and contribute to the study of particle formation mechanisms by comparison with other identified hadrons. For this purpose, the mean transverse momenta and the differential proton-to-[Formula: see text] ratio are discussed as a function of the multiplicity of the event. The short-lived K[Formula: see text] is measured to investigate re-scattering effects, believed to be related to the size of the system and to the lifetime of the hadronic phase.
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