Automodelity in strong interactions

Matveev, V.; Muradyan, R.M.; Тавхелидзе, А.Н.

doi:10.1007/bf02777988

Cited by 98 publications

(55 citation statements)

References 3 publications

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“…In some sense the duality claims a kind of auto-model behaviour of strong correlator systems. There is an similarity with the auto-model behaviour of the parton model [6].…”

Section: Holographic Approach To Static Qgpmentioning

confidence: 54%

“…This metric is a solution [30,35] to a 5d model governed by the action where m 0 and Λ are constant and the 3-form H (3) and the 2-form B (2) are related by H (3) = dB (2) . There is a problem with action (6) since up to now we do not know the blacking version of the metric (5) as a solution to the model (6). However there is a possibility to support the metric (5) by another action and to find the corresponding blacking solution [32].…”

Section: Anisotropic Holographic Backgroundsmentioning

confidence: 99%

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Multiplicity and theremalization time in heavy-ions collisions

Aref’eva

2016

EPJ Web Conf.

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Abstract. We present a concise review of quark-gluon plasma formation in heavy-ions collisions within the holographic approach. In particular, we discuss how to get the total multiplicity in heavy ions collision to fit the recent experimental data. We also discuss theoretical estimations of time formation of QGP in heavy ions collision and show that different observables can give the different times of QGP formation.

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“…In some sense the duality claims a kind of auto-model behaviour of strong correlator systems. There is an similarity with the auto-model behaviour of the parton model [6].…”

Section: Holographic Approach To Static Qgpmentioning

confidence: 54%

Section: Anisotropic Holographic Backgroundsmentioning

confidence: 99%

Multiplicity and theremalization time in heavy-ions collisions

Aref’eva

2016

EPJ Web Conf.

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“…It is important to note that this asymptotical behaviour, consistent with the quark counting rules [23,24], includes the one-loop coupling only and is to be modified whenever the one-loop approximation fails, but not by means of a simple replacing of α s with its more precise value. Involved QCD calculations have been performed to obtain corrections to Eq.…”

Section: Asymptotics Of the Pion Form Factor At High Momentum Transfersmentioning

confidence: 70%

Poincaré-invariant constituent quark model for light mesons: capabilities and constraints

2016

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Abstract. We present a brief survey of some results on electroweak properties of composite systems that are obtained in the frameworks of our version of the instant form of relativistic quantum mechanics (RQM). Our approach describes well the π-and the ρ-mesons in wide range of momentum transfers Q 2 . At large Q 2 the obtained pion form factor asymptotics coincides with that of QCD predictions. The method permits to perform analytic continuation of pion form factor to complex plane of momentum transfers that is in accordance with predictions of quantum field theory.

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“…The consequences of the limiting fragmentation hypothesis [2] and those of the parton model [3] and the principle of automodelity for strong interactions [4] have been formulated in this way.…”

mentioning

confidence: 99%

Towards the light front variables for high energy production processes

et al. 1999

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Scale invariant presentation of inclusive spectra in terms of light front variables is proposed. The variables introduced go over to the well-known scaling variables x F = 2p z / √ s and x T = 2p T / √ s in the high p z and high p T limits respectively.Some surface is found in the phase space of produced π ± -mesons in the inclusive reaction pp → π ± X at 22.4 GeV/c, which separates two groups of particles with significantly different characteristics. In one of these regions a naive statistical model seems to be in a good agreement with data, whereas it fails in the second region.Classification codes: PACS numbers: 13.85 Ni, 13.90+i

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Automodelity in strong interactions

Cited by 98 publications

References 3 publications

Multiplicity and theremalization time in heavy-ions collisions

Multiplicity and theremalization time in heavy-ions collisions

Poincaré-invariant constituent quark model for light mesons: capabilities and constraints

Towards the light front variables for high energy production processes

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