Chaos in chiral condensates in gauge theories
arXiv:1605.08124 · doi:10.1103/PhysRevLett.117.231602
Abstract
Assigning a chaos index for dynamics of generic quantum field theories is a challenging problem, because the notion of Lyapunov exponent, which is useful for singling out chaotic behaviors, works only in classical systems. We address the issue by using the AdS/CFT correspondence, as the large limit provides a classicalization (other than the standard ) while keeping nontrivial quantum condensation. We demonstrate the chaos in the dynamics of quantum gauge theories: Time evolution of homogeneous quark condensates and in an supersymmetric QCD with the gauge group at large and at large 't Hooft coupling exhibits a positive Lyapunov exponent. The chaos dominates the phase space for energy density where is the quark mass. We evaluate the largest Lyapunov exponent as a function of and find that the supersymmetric QCD is more chaotic for smaller .
9 pages, 5 figures. v2: Analysis of Lyapunov exponent of linear sigma model added, references and a footnote added. v3: Published version. An appendix added for explaining relation between classical chaos and out-of-time-ordered correlator. Title modified, abstract refined v4: Typos and grammatical errors corrected
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