K*0 and φ meson production in proton–nucleus interactions at $\sqrt{s}=41.6\text{GeV}$

Abt, I.; Adams, M. R.; Agari, M.; Albrecht, H.; Aleksandrov, A.; Amaral, Vasco; Amorim, A.; Aplin, S.; Aushev, V.; Bagaturia, Y.; Balagura, V.; Bargiotti, M.; Barsukova, O.; Bastos, J.; Batista, J.; Bauer, C.; Bauer, Th.; Bel'kov, A.A.; Belotelov, I.; Bertin, A.; Bobchenko, B.; Böcker, M.; Bogatyrev, A.; Böhm, G.; Bräuer, M.; Bruinsma, M.; Bruschi, M.; Buchholz, P.; Buran, T.; Carvalho, J.; Conde, P.; Cruse, C.; Dam, M.; Danielsen, K.M.; Danilov, M.; Castro, S. De; Deppe, H.; Dong, X.; Dreis, H. B.; Egorytchev, V.; Ehret, K.; Eisele, F.; Emeliyanov, D.; Essenov, S.; Fabbri, L.; Faccioli, P.; Feuerstack-Raible, M.; Flammer, J.; Fominykh, B.; Funcke, M.; Garrido, L.; Gellrich, A.; Giacobbe, B.; Gläß, J.; Goloubkov, D.; Golubkov, D.; Golutvin, A.; Golutvin, I.; Gorbounov, I.; Gorišek, A.; Gouchtchine, O.; Goulart, D. C.; Gradl, S.; Gradl, W.; Grimaldi, F.; Groth-Jensen, J.; Guilitsky, Y.; Hansen, J. D.; Hernández, J. M.; Hofmann, W.; Hohlmann, M.; Hott, T.; Hulsbergen, W.; Husemann, U.; Igonkina, O.; Ispiryan, M.; Jagla, T.; Jiang, C. H.; Kapitza, H.; Karabekyan, S.; Karpenko, N.N.; Keller, S.; Keßler, J.; Khasanov, F.; Kiryushin, Yu.T.; Kisel, I.; Klinkby, E. B.; Knöpfle, K. T.; Kolanoski, H.; Korpar, S.; Krauss, C. B.; Kreuzer, P.; Križan, P.; Krücker, D.; Küpper, Sebastian; Kvaratskheliia, T.; Lanev, A.; Lau, K.; Lewendel, B.; Löhse, T.; Lomonosov, B.; Männer, Reinhard; Mankel, R.; Masciocchi, S.; Massa, I.; Matchikhilian, I.; Medin, G.; Medinnis, M.; Mevius, M.; Michetti, A.; Mikhailov, Yu.V.; Mizuk, R.; Mureşan, R.; Nedden, M. zur; Negodaev, M.; Nörenberg, M.; Nowak, S.; Vera, María Teresa Núñez Pardo de; Ouchrif, M.; Ould-Saada, F.; Aranda, C. Padilla; Peralta, D.; Pernack, R.; Pestotnik, R.; Petersen, B. A.; Piccinini, M.; Pleier, M. A.; Poli, M.; Popov, V.; Pose, D.; Prystupa, S.; Pugatch, V.; Pylypchenko, Y.; Pyrlik, J.; Reeves, K.; Reßing, D.; Rick, H.; Riu, I.; Robmann, P.; Rostovtseva, I.; Rybnikov, V.; Sanchez, F. J. Munoz; Sbrizzi, A.; Schmelling, M.; Schmidt, B.; Schreiner, A.; Schröder, H.; Schwanke, U.; Schwartz, A. J.; Schwarz, A. S.; Schwenninger, B.; Schwingenheuer, B.; Sciacca, F. G.; Semprini‐Cesari, N.; Shuvalov, S.; Silva, L.; Sözüer, L.; Solunin, S.; Somov, A.; Somov, S.; Spengler, J.; Spighi, R.; Спиридонов, А.; Stanovnik, A.; Starič, M.; Stegmann, C.; Subramania, Halasya Siva; Symalla, M.; Tikhomirov, I.; Titov, M.; Tsakov, I.; Uwer, U.; Eldik, C. van; Vassiliev, Y.; Villa, M.; Vitale, A.; Vukotić, I.; Wahlberg, H.; Walenta, A.H.; Walter, Michael; Wang, J.J.; Wegener, D.; Werthenbach, U.; Wolters, H.; Wurth, R.; Wurz, A.; Zaitsev, Yu.; Zavertyaev, M.; Zeuner, T.; Zhelezov, A.; Zheng, Z. P.; Zimmermann, R.; Živko, T.; Zoccoli, À.

doi:10.1140/epjc/s10052-007-0237-3

Cited by 28 publications

(33 citation statements)

References 72 publications

(38 reference statements)

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“…In refs. [38], [39][40][41][42][43], and [44], the three revisions of the Hagedorn function (inverse power law) are given respectively, though specific nomenclatures on the revised Hagedorn functions are not mentioned in some cases. We shall not discuss the Hagedorn function and its revisions due to the fact that the hard scattering process has no contribution to the kinetic freeze-out temperature and transverse flow velocity.…”

Section: Formalism and Methodsmentioning

confidence: 99%

Energy dependent kinetic freeze-out temperature and transverse flow velocity in high energy collisions

Liu

2018

Eur. Phys. J. A

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Transverse momentum spectra of negative and positive pions produced at mid-(pseudo)rapidity in inelastic or non-single-diffractive proton-proton collisions and in central nucleus-nucleus collisions over an energy range from a few GeV to above 10 TeV are analyzed by a (two-component) blast-wave model with Boltzmann-Gibbs statistics and with Tsallis statistics respectively. The model results are in similarly well agreement with the experimental data measured by a few productive collaborations who work at the Heavy Ion Synchrotron (SIS), Super Proton Synchrotron (SPS), Relativistic Heavy Ion Collider (RHIC), and Large Hadron Collider (LHC), respectively. The energy dependent kinetic freeze-out temperature and transverse flow velocity are obtained and analyzed. Both the quantities have quick increase from the SIS to SPS, and slight increase or approximate invariability from the top RHIC to LHC. Around the energy bridge from the SPS to RHIC, the considered quantities in proton-proton collisions obtained by the blast-wave model with Boltzmann-Gibbs statistics show more complex energy dependent behavior comparing with the results in other three cases.Keywords: energy dependent kinetic freeze-out temperature, energy dependent transverse flow velocity, inelastic or non-single-diffractive proton-proton collisions, central nucleus-nucleus collisions

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Section: Formalism and Methodsmentioning

confidence: 99%

Energy dependent kinetic freeze-out temperature and transverse flow velocity in high energy collisions

Liu

2018

Eur. Phys. J. A

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“…On the other hand, the theoretical results for σ vis consistently coincide with the experimental measurements. andK * 0 meson production in pA collisions at √ s = 41.6 Gev with the corresponding experimental data by the HERAb Collaboration [39]. The curve representing the QGSM prediction forK * 0 -meson production practically coincides with the solid curve for K * 0 , and so it is not shown.…”

Section: K * -Meson Production On Nuclear Targets At Not Very High Enmentioning

confidence: 85%

Hadroproduction of neutral K*-mesons up to LHC energies

2019

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“…We analyze experimental data by the HERA-B Collaboration on φ-meson production in collisions of protons with C, T i, and W nuclei. These data were integrated over the whole range of the transverse momentum p T at √ s = 41.6 GeV [43].…”

Section: The φ-Meson Production In Hadron Collisions With Nuclear Tarmentioning

confidence: 99%

Description of ϕ-meson production in hadronic and nuclear collisions at very high energies

Arakelyan

Merino

Shabelski

2018

Int. J. Mod. Phys. A

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We expose the current experimental and theoretical situation of the interesting case of the production of φ mesons in up to very high energy collisions of hadrons on both nucleon and nuclear targets, and we present a quantitavely good theoretical description of the corresponding experimental data, based on the formalism of the well established Quark-Gluon String Model, that has proved to be valid for a wide energy range. All the available experimental data for φ-meson production in hadron-nucleon collisions on the spectra of secondary φ, and on the ratios of φ/π − and φ/K − production cross sections, as well the corresponding ones for φ-meson production on nuclear targets, are considered. In particular, it is seen that the production of φ-mesons on nuclear targets presents unusually small shadow corrections for the inclusive density in the central rapidity region.

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K*0 and φ meson production in proton–nucleus interactions at $\sqrt{s}=41.6\text{GeV}$

Cited by 28 publications

References 72 publications

Energy dependent kinetic freeze-out temperature and transverse flow velocity in high energy collisions

Energy dependent kinetic freeze-out temperature and transverse flow velocity in high energy collisions

Hadroproduction of neutral K*-mesons up to LHC energies

Description of ϕ-meson production in hadronic and nuclear collisions at very high energies

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