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The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data. / Ivanov, D. Yu; Murdaca, B.; Papa, A.

в: Journal of High Energy Physics, Том 2014, № 10, 58, 2014.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

Harvard

Ivanov, DY, Murdaca, B & Papa, A 2014, 'The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data', Journal of High Energy Physics, Том. 2014, № 10, 58. https://doi.org/10.1007/JHEP10(2014)058

APA

Ivanov, D. Y., Murdaca, B., & Papa, A. (2014). The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data. Journal of High Energy Physics, 2014(10), [58]. https://doi.org/10.1007/JHEP10(2014)058

Vancouver

Ivanov DY, Murdaca B, Papa A. The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data. Journal of High Energy Physics. 2014;2014(10):58. doi: 10.1007/JHEP10(2014)058

Author

Ivanov, D. Yu ; Murdaca, B. ; Papa, A. / The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data. в: Journal of High Energy Physics. 2014 ; Том 2014, № 10.

BibTeX

@article{868dc30a8b9b4a0ba9f7f0c2e96d8e09,
title = "The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data",
abstract = "We study the total cross section for the collision of two highly-virtual photons at large energies, taking into account the BFKL resummation of energy logarithms with full next-to-leading accuracy. A necessary ingredient of the calculation, the next-to-leading order impact factor for the photon to photon transition, has been calculated by Balitsky and Chirilli using an approach based on the operator expansion in Wilson lines. We extracted the result for the photon impact factor in the original BFKL calculation scheme comparing the expression for the photon-photon total cross section obtained in BFKL with the one recently derived by Chirilli and Kovchegov in the Wilson-line operator expansion scheme. We perform a detailed numerical analysis, combining different, but equivalent in nextto-leading accuracy, representations of the cross section with various optimization methods of the perturbative series. We compare our results with previous determinations in the literature and with the LEP2 experimental data. We find that the account of Balitsky and Chirilli expression for the photon impact factor reduces the BFKL contribution to the cross section to very small values, making it impossible to describe LEP2 data as the sum of BFKL and leading-order QED quark box contributions.",
keywords = "QCD, Resummation",
author = "Ivanov, {D. Yu} and B. Murdaca and A. Papa",
note = "Publisher Copyright: {\textcopyright} The Authors. Copyright: Copyright 2015 Elsevier B.V., All rights reserved.",
year = "2014",
doi = "10.1007/JHEP10(2014)058",
language = "English",
volume = "2014",
journal = "Journal of High Energy Physics",
issn = "1029-8479",
publisher = "Springer US",
number = "10",

}

RIS

TY - JOUR

T1 - The γ*γ* Total cross section in next-to-leading order BFKL and LEP2 data

AU - Ivanov, D. Yu

AU - Murdaca, B.

AU - Papa, A.

N1 - Publisher Copyright: © The Authors. Copyright: Copyright 2015 Elsevier B.V., All rights reserved.

PY - 2014

Y1 - 2014

N2 - We study the total cross section for the collision of two highly-virtual photons at large energies, taking into account the BFKL resummation of energy logarithms with full next-to-leading accuracy. A necessary ingredient of the calculation, the next-to-leading order impact factor for the photon to photon transition, has been calculated by Balitsky and Chirilli using an approach based on the operator expansion in Wilson lines. We extracted the result for the photon impact factor in the original BFKL calculation scheme comparing the expression for the photon-photon total cross section obtained in BFKL with the one recently derived by Chirilli and Kovchegov in the Wilson-line operator expansion scheme. We perform a detailed numerical analysis, combining different, but equivalent in nextto-leading accuracy, representations of the cross section with various optimization methods of the perturbative series. We compare our results with previous determinations in the literature and with the LEP2 experimental data. We find that the account of Balitsky and Chirilli expression for the photon impact factor reduces the BFKL contribution to the cross section to very small values, making it impossible to describe LEP2 data as the sum of BFKL and leading-order QED quark box contributions.

AB - We study the total cross section for the collision of two highly-virtual photons at large energies, taking into account the BFKL resummation of energy logarithms with full next-to-leading accuracy. A necessary ingredient of the calculation, the next-to-leading order impact factor for the photon to photon transition, has been calculated by Balitsky and Chirilli using an approach based on the operator expansion in Wilson lines. We extracted the result for the photon impact factor in the original BFKL calculation scheme comparing the expression for the photon-photon total cross section obtained in BFKL with the one recently derived by Chirilli and Kovchegov in the Wilson-line operator expansion scheme. We perform a detailed numerical analysis, combining different, but equivalent in nextto-leading accuracy, representations of the cross section with various optimization methods of the perturbative series. We compare our results with previous determinations in the literature and with the LEP2 experimental data. We find that the account of Balitsky and Chirilli expression for the photon impact factor reduces the BFKL contribution to the cross section to very small values, making it impossible to describe LEP2 data as the sum of BFKL and leading-order QED quark box contributions.

KW - QCD

KW - Resummation

UR - http://www.scopus.com/inward/record.url?scp=84928572670&partnerID=8YFLogxK

U2 - 10.1007/JHEP10(2014)058

DO - 10.1007/JHEP10(2014)058

M3 - Article

AN - SCOPUS:84928572670

VL - 2014

JO - Journal of High Energy Physics

JF - Journal of High Energy Physics

SN - 1029-8479

IS - 10

M1 - 58

ER -

ID: 27431628