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Production of Formula: see text and Formula: see text mesons up to high transverse momentum in pp collisions at 2.76 TeV
by
Mitra, J
, Murray, S
, Ahammed, Z
, Corral, G Herrera
, Moreno, L A P
, Fabbietti, L
, Gaardhøje, J J
, Bhat, I R
, Závada, P
, Nair, R
, Fuchs, U
, Cheynis, B
, Caliva, A
, Zmeskal, J
, Kundu, S
, Margutti, J
, Camejo, A Batista
, Herrmann, F
, Westerhoff, U
, Buhler, P
, Evans, D
, Pluta, J
, Agrawal, N
, 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
, Poppenborg, H
, Tello, A Villatoro
, Germain, M
, Vigolo, S
, Mihaylov, D L
, Röhrich, D
, Naru, M U
, Riggi, F
, Berenyi, D
, Kalweit, A
, Shangaraev, A
, Schweda, K
, Yoo, I-K
, Grelli, A
, Hornung, S
, Kluge, A
, Morales, Y Corrales
, Shabanov, A
, Cifarelli, L
, Trzeciak, B A
, Giubellino, P
, Jadhav, M B
, Mishra, A N
, Barnaföldi, G G
, 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
, Anson, C
, Ricci, R A
, Shahoyan, R
, Yin, Z
, Lattuca, A
, Mohammadi, N
, Gladysz-Dziadus, E
, Kollegger, T
, Kučera, V
, Shigaki, K
, Kileng, B
, Degenhardt, H F
, Chang, B
, Bedda, C
, Hipp
2017
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Production of Formula: see text and Formula: see text mesons up to high transverse momentum in pp collisions at 2.76 TeV
by
Mitra, J
, Murray, S
, Ahammed, Z
, Corral, G Herrera
, Moreno, L A P
, Fabbietti, L
, Gaardhøje, J J
, Bhat, I R
, Závada, P
, Nair, R
, Fuchs, U
, Cheynis, B
, Caliva, A
, Zmeskal, J
, Kundu, S
, Margutti, J
, Camejo, A Batista
, Herrmann, F
, Westerhoff, U
, Buhler, P
, Evans, D
, Pluta, J
, Agrawal, N
, 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
, Poppenborg, H
, Tello, A Villatoro
, Germain, M
, Vigolo, S
, Mihaylov, D L
, Röhrich, D
, Naru, M U
, Riggi, F
, Berenyi, D
, Kalweit, A
, Shangaraev, A
, Schweda, K
, Yoo, I-K
, Grelli, A
, Hornung, S
, Kluge, A
, Morales, Y Corrales
, Shabanov, A
, Cifarelli, L
, Trzeciak, B A
, Giubellino, P
, Jadhav, M B
, Mishra, A N
, Barnaföldi, G G
, 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
, Anson, C
, Ricci, R A
, Shahoyan, R
, Yin, Z
, Lattuca, A
, Mohammadi, N
, Gladysz-Dziadus, E
, Kollegger, T
, Kučera, V
, Shigaki, K
, Kileng, B
, Degenhardt, H F
, Chang, B
, Bedda, C
, Hipp
in
2017
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Production of Formula: see text and Formula: see text mesons up to high transverse momentum in pp collisions at 2.76 TeV
by
Mitra, J
, Murray, S
, Ahammed, Z
, Corral, G Herrera
, Moreno, L A P
, Fabbietti, L
, Gaardhøje, J J
, Bhat, I R
, Závada, P
, Nair, R
, Fuchs, U
, Cheynis, B
, Caliva, A
, Zmeskal, J
, Kundu, S
, Margutti, J
, Camejo, A Batista
, Herrmann, F
, Westerhoff, U
, Buhler, P
, Evans, D
, Pluta, J
, Agrawal, N
, 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
, Poppenborg, H
, Tello, A Villatoro
, Germain, M
, Vigolo, S
, Mihaylov, D L
, Röhrich, D
, Naru, M U
, Riggi, F
, Berenyi, D
, Kalweit, A
, Shangaraev, A
, Schweda, K
, Yoo, I-K
, Grelli, A
, Hornung, S
, Kluge, A
, Morales, Y Corrales
, Shabanov, A
, Cifarelli, L
, Trzeciak, B A
, Giubellino, P
, Jadhav, M B
, Mishra, A N
, Barnaföldi, G G
, 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
, Anson, C
, Ricci, R A
, Shahoyan, R
, Yin, Z
, Lattuca, A
, Mohammadi, N
, Gladysz-Dziadus, E
, Kollegger, T
, Kučera, V
, Shigaki, K
, Kileng, B
, Degenhardt, H F
, Chang, B
, Bedda, C
, Hipp
2017
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Production of Formula: see text and Formula: see text mesons up to high transverse momentum in pp collisions at 2.76 TeV
Journal Article
Production of Formula: see text and Formula: see text mesons up to high transverse momentum in pp collisions at 2.76 TeV
2017
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Overview
The invariant differential cross sections for inclusive [Formula: see text] and [Formula: see text] mesons at midrapidity were measured in pp collisions at [Formula: see text] TeV for transverse momenta [Formula: see text] GeV/c and [Formula: see text] GeV/c, respectively, using the ALICE detector. This large range in [Formula: see text] was achieved by combining various analysis techniques and different triggers involving the electromagnetic calorimeter (EMCal). In particular, a new single-cluster, shower-shape based method was developed for the identification of high-[Formula: see text] neutral pions, which exploits that the showers originating from their decay photons overlap in the EMCal. Above 4 GeV/[Formula: see text], the measured cross sections are found to exhibit a similar power-law behavior with an exponent of about 6.3. Next-to-leading-order perturbative QCD calculations differ from the measured cross sections by about 30% for the [Formula: see text], and between 30-50% for the [Formula: see text] meson, while generator-level simulations with PYTHIA 8.2 describe the data to better than 10-30%, except at [Formula: see text] GeV/[Formula: see text]. The new data can therefore be used to further improve the theoretical description of [Formula: see text] and [Formula: see text] meson production.The invariant differential cross sections for inclusive [Formula: see text] and [Formula: see text] mesons at midrapidity were measured in pp collisions at [Formula: see text] TeV for transverse momenta [Formula: see text] GeV/c and [Formula: see text] GeV/c, respectively, using the ALICE detector. This large range in [Formula: see text] was achieved by combining various analysis techniques and different triggers involving the electromagnetic calorimeter (EMCal). In particular, a new single-cluster, shower-shape based method was developed for the identification of high-[Formula: see text] neutral pions, which exploits that the showers originating from their decay photons overlap in the EMCal. Above 4 GeV/[Formula: see text], the measured cross sections are found to exhibit a similar power-law behavior with an exponent of about 6.3. Next-to-leading-order perturbative QCD calculations differ from the measured cross sections by about 30% for the [Formula: see text], and between 30-50% for the [Formula: see text] meson, while generator-level simulations with PYTHIA 8.2 describe the data to better than 10-30%, except at [Formula: see text] GeV/[Formula: see text]. The new data can therefore be used to further improve the theoretical description of [Formula: see text] and [Formula: see text] meson production.
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