2019
DOI: 10.1103/physrevd.100.046009
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Chaos of QCD string from holography

Abstract: It is challenging to quantify chaos of QCD, because non-perturbative QCD accompanies non-local observables. By using holography, we find that QCD strings at large Nc and strong coupling limit exhibit chaos, and measure their Lyapunov exponent at zero temperature. A pair of a quark and an antiquark separated by Lq in the large Nc QCD is dual to a Nambu-Goto string hanging from the spatial boundary of the D4-soliton geometry. We numerically solve the motion of the string after putting a pulse force on its bounda… Show more

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Cited by 17 publications
(9 citation statements)
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References 59 publications
(80 reference statements)
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“…There exist many more publications worth mentioning in this context. A very recent example dealing with QCD is, e.g., [38], while in Ref. [39] it is argued that, at least for entanglement entropy, bosons, and a quadratic Hamiltonian, a linear growth of entropy with the Kolmogorov-Sinaï entropy can be derived also for quantum systems.…”
Section: Entropy Production In Classical and Quantum Gauge Theoriesmentioning
confidence: 99%
“…There exist many more publications worth mentioning in this context. A very recent example dealing with QCD is, e.g., [38], while in Ref. [39] it is argued that, at least for entanglement entropy, bosons, and a quadratic Hamiltonian, a linear growth of entropy with the Kolmogorov-Sinaï entropy can be derived also for quantum systems.…”
Section: Entropy Production In Classical and Quantum Gauge Theoriesmentioning
confidence: 99%
“…In terms of supergravity, we choose a string embedding that produces the kind of differential equations of motion that can be examined under Kovacic's theorem, [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26]. Since an integrable theory has all of its dynamical sectors integrable, then every possible string configuration must echo integrable dynamics.…”
Section: Introductionmentioning
confidence: 99%
“…(1) using the AdS/CFT correspondence [11][12][13], adopting a dual geometry with a black hole and identifying T with the Hawking temperature, for example, in [14,15]. In particular, the heavy quark-antiquark pair, described holographically by a string hanging in the bulk with end points on the boundary [16][17][18][19], has been studied in this context [20][21][22]. For this system λ is the Lyapunov exponent characterizing the chaotic behavior of time-dependent fluctuations around the static configuration.…”
Section: Introductionmentioning
confidence: 99%