Transverse momentum spectra of charged particles in proton–proton collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si1.gif" overflow="scroll"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>900</mml:mn><mml:mtext> GeV</mml:mtext></mml:math> with ALICE at the LHC

Aamodt, K.; Abel, N.; Abeysekara, U.; Quintana, A. Abrahantes; Abramyan, A.; Adamová, D.; Aggarwal, M. M.; Rinella, G. Aglieri; Agocs, A. G.; Salazar, S. Aguilar; Ahammed, Z.; Ahmad, Arshad; Ahmad, N.; Ahn, S. U.; Akimoto, R.; Akindinov, A.; Aleksandrov, Dmitry; Alessandro, B.; Molina, R. Alfaro; Alici, A.; Aviña, E. Almaráz; Alme, J.; Alt, T.; Altini, V.; Altinpinar, S.; Andrei, C.; Andronic, A.; Anelli, G.; Angelov, V.; Anson, C.; Antičić, T.; Antinori, F.; Antinori, S.; Antipin, K.; Antończyk, D.; Antonioli, P.; Anzo, A.; Aphecetche, L.; Appelshäuser, H.; Arcelli, S.; Arceo, R.; Arend, A.; Armesto, N.; Arnaldi, R.; Aronsson, T.; Arsene, I. C.; Asryan, A.; Augustinus, A.; Averbeck, R.; Awes, T. C.; Äystö, J.; Azmi, M. D.; Bablok, S.; Bach, M.; Badalà, A.; Baek, Yongwook; Bagnasco, S.; Bailhache, R.; Bala, R.; Baldisseri, A.; Baldit, A.; Bán, J.; Barbera, R.; Barnaföldi, G. G.; Barnby, L. 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doi:10.1016/j.physletb.2010.08.026

Cited by 185 publications

(112 citation statements)

References 45 publications

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“…In right panel of figure 5 we observe the slight decrease of the p t -n correlation function at extremely large multiplicities. One can find the signature of this effect in figure 7 in paper [27] for the correlation between transverse momentum and multiplicity of charged particles produced in the same window (in the acceptance of ALICE TPC |η| < 0.8) in 900 GeV pp collisions.…”

Section: Correlation Between Transverse Momentum and Multiplicitymentioning

confidence: 89%

“…Note the nonlinear dependence of the correlation function on µ F . If we will use as in the previous subsection 4.1 and in paper [17] the modified poissonian distribution P (N) for the total number of strings, then omitting common constant factor, we can use as Φ(F) (27) for the calculation of B F in (25). By (26) we can get explicit expression:…”

Section: The Correlation Function N B N Fmentioning

confidence: 99%

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Nonlinearity of the forward-backward correlation function in the model with string fusion

Vechernin

2017

EPJ Web Conf.

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Abstract. The behavior of the forward-backward correlation functions and the corresponding correlation coefficients between multiplicities and transverse momenta of particles produced in high energy hadronic interactions is analyzed by analytical and MC calculations in the models with and without string fusion. The string fusion is taking into account in simplified form by introducing the lattice in the transverse plane. The results obtained with two alternative definitions of the forward-backward correlation coefficient are compared. It is shown that the nonlinearity of correlation functions increases with the width of observation windows, leading at small string density to a strong dependence of correlation coefficient value on the definition. The results of the modeling enable qualitatively to explain the experimentally observed features in the behavior of the correlation functions between multiplicities and mean transverse momenta at small and large multiplicities.

show abstract

Section: Correlation Between Transverse Momentum and Multiplicitymentioning

confidence: 89%

Section: The Correlation Function N B N Fmentioning

confidence: 99%

Nonlinearity of the forward-backward correlation function in the model with string fusion

Vechernin

2017

EPJ Web Conf.

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“…The Collaborations CMS [1], ATLAS [2] and ALICE [3] have published inclusive charged particle transverse momentum distributions in pp interaction at center-of-mass energy √ s = 900 GeV 1 . The ATLAS and ALICE compared their measurements to inclusive cross sections of pp interaction obtained by the UA1 Collaboration [6] at the same energy √ s = 900 GeV.…”

Section: Introductionmentioning

confidence: 99%

“…Figure 1: The ratios of invariant inclusive cross sections of the UA1 [6] to ATLAS [2] (a), ALICE [3] (b) and CMC [1] (c) at √ s = 900 GeV. The shaded areas indicate the errors of the ratios.…”

Section: Introductionmentioning

confidence: 99%

Comparison of the data on proton-proton and proton-antiproton interactions at high energies on basis of the Low Constituents Number Model

Abramovsky¹

2013

Proceedings of XXI International Baldin Seminar on High Energy Physics Problems — PoS(Baldin ISHEPP XXI)

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We argue that hadrons production is different in pp and pp interactions at high energies. There is process of hadrons production from three quark strings in pp which is absent in pp. This process grows as (ln √ s) 2 and becomes significant when energy of collision increases. Inclusive cross sections of pp interaction exceed inclusive cross sections of pp. The UA1 data on pp transverse momentum distribution are about 1.2 -1.3 times higher than the CMS, ATLAS and ALICE data on pp at energy √ s = 900 GeV. Question regarding existence of the Pomranchuk theorem demands further investigation on evidence of difference of multiple processes in pp and pp interactions.

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“…The global tracking and momentum reconstruction are based on the TPC and ITS subdetectors (see [9] for details). 3.…”

mentioning

confidence: 99%

Probing QCD with the ALICE detector at the LHC

Andronic¹

2010

AIP Conference Proceedings

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Transverse momentum spectra of charged particles in proton–proton collisions at s=900 GeV with ALICE at the LHC

Cited by 185 publications

References 45 publications

Nonlinearity of the forward-backward correlation function in the model with string fusion

Nonlinearity of the forward-backward correlation function in the model with string fusion

Comparison of the data on proton-proton and proton-antiproton interactions at high energies on basis of the Low Constituents Number Model

Probing QCD with the ALICE detector at the LHC

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