2014
DOI: 10.1103/physreve.90.042145
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Geometric critical exponents in classical and quantum phase transitions

Abstract: We define geometric critical exponents for systems that undergo continuous second-order classical and quantum phase transitions. These relate scalar quantities on the information theoretic parameter manifolds of such systems, near criticality. We calculate these exponents by approximating the metric and thereby solving geodesic equations analytically, near curvature singularities of two-dimensional parameter manifolds. The critical exponents are seen to be the same for both classical and quantum systems that w… Show more

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Cited by 27 publications
(40 citation statements)
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“…This result agrees with that obtained in [18] for the van der Waals fluid. The third condition of the previous section is also satisfied.…”
Section: A Geometric Scaling Relation For Rn-ads Fluidssupporting
confidence: 92%
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“…This result agrees with that obtained in [18] for the van der Waals fluid. The third condition of the previous section is also satisfied.…”
Section: A Geometric Scaling Relation For Rn-ads Fluidssupporting
confidence: 92%
“…This result is strictly valid close to criticality, and is an example of a geometric scaling. In [18], it was argued from generic grounds that this relation should in general be true for two dimensional parameter manifolds, and we see that it is indeed the case here.…”
Section: A Geometric Scaling Relation For Rn-ads Fluidssupporting
confidence: 70%
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“…By computing JLC vector fields for the previous three and two dimensional Gaussian models in the Eqs. (113) and (115), we arrive at the following asymptotic relation…”
Section: B Complexitymentioning
confidence: 99%
“…To a somewhat lesser extent, same can be said about such connections found in thermodynamics of phase transitions ('Fisher-Ruppeiner metric') [110][111][112][113], quantum information and tensor network states [114][115][116][117][118][119][120], QHE hydrodynamics ('Fubini-Study metric') [121][122][123], Chern classes of the Bloch eigenstates of momentum [124][125][126], Berry phase of the adiabatic time evolution [127][128][129], etc. In all these different contexts, some underlying invariance under pertinent diffeomorphisms facilitates an elegant and insightful gravitational description.…”
Section: Emergent Geometry and 'Holography Light'mentioning
confidence: 99%