Integrability of the evolution equations for heavy–light baryon distribution amplitudes

We consider evolution equations describing the scale dependence of the wave function of a baryon containing an infinitely heavy quark and a pair of light quarks at small transverse separations, which is the QCD analogue of the helium atom. The evolution equations depend on the relative helicity of t...

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Main Authors: V.M. Braun, S.E. Derkachov, A.N. Manashov
Format: Article
Language:English
Published: Elsevier 2014-11-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269314007205
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spelling doaj-c4be8312ded04dd1ab596bed21a5840c2020-11-24T21:15:19ZengElsevierPhysics Letters B0370-26932014-11-01738334340Integrability of the evolution equations for heavy–light baryon distribution amplitudesV.M. Braun0S.E. Derkachov1A.N. Manashov2Institut für Theoretische Physik, Universität Regensburg, D-93040 Regensburg, Germany; Corresponding author.St. Petersburg Department of Steklov Mathematical Institute, 191023 St. Petersburg, Russia; St. Petersburg State Polytechnic University, 195251 St. Petersburg, RussiaInstitut für Theoretische Physik, Universität Regensburg, D-93040 Regensburg, Germany; Department of Theoretical Physics, St. Petersburg University, 199034 St. Petersburg, RussiaWe consider evolution equations describing the scale dependence of the wave function of a baryon containing an infinitely heavy quark and a pair of light quarks at small transverse separations, which is the QCD analogue of the helium atom. The evolution equations depend on the relative helicity of the light quarks. For the aligned helicities, we find that the equation is completely integrable, that is, it has a nontrivial integral of motion, and obtain exact analytic expressions for the eigenfunctions and the anomalous dimensions. The evolution equation for anti-aligned helicities contains an extra term that breaks integrability and creates a “bound state” with the anomalous dimension separated from the rest of the spectrum by a finite gap. The corresponding eigenfunction is found using numerical methods. It describes the momentum fraction distribution of the light quarks in, e.g., Λb-baryon at large scales.http://www.sciencedirect.com/science/article/pii/S0370269314007205
collection DOAJ
language English
format Article
sources DOAJ
author V.M. Braun
S.E. Derkachov
A.N. Manashov
spellingShingle V.M. Braun
S.E. Derkachov
A.N. Manashov
Integrability of the evolution equations for heavy–light baryon distribution amplitudes
Physics Letters B
author_facet V.M. Braun
S.E. Derkachov
A.N. Manashov
author_sort V.M. Braun
title Integrability of the evolution equations for heavy–light baryon distribution amplitudes
title_short Integrability of the evolution equations for heavy–light baryon distribution amplitudes
title_full Integrability of the evolution equations for heavy–light baryon distribution amplitudes
title_fullStr Integrability of the evolution equations for heavy–light baryon distribution amplitudes
title_full_unstemmed Integrability of the evolution equations for heavy–light baryon distribution amplitudes
title_sort integrability of the evolution equations for heavy–light baryon distribution amplitudes
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2014-11-01
description We consider evolution equations describing the scale dependence of the wave function of a baryon containing an infinitely heavy quark and a pair of light quarks at small transverse separations, which is the QCD analogue of the helium atom. The evolution equations depend on the relative helicity of the light quarks. For the aligned helicities, we find that the equation is completely integrable, that is, it has a nontrivial integral of motion, and obtain exact analytic expressions for the eigenfunctions and the anomalous dimensions. The evolution equation for anti-aligned helicities contains an extra term that breaks integrability and creates a “bound state” with the anomalous dimension separated from the rest of the spectrum by a finite gap. The corresponding eigenfunction is found using numerical methods. It describes the momentum fraction distribution of the light quarks in, e.g., Λb-baryon at large scales.
url http://www.sciencedirect.com/science/article/pii/S0370269314007205
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AT sederkachov integrabilityoftheevolutionequationsforheavylightbaryondistributionamplitudes
AT anmanashov integrabilityoftheevolutionequationsforheavylightbaryondistributionamplitudes
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