20,139 research outputs found

    Kinematic Basis of Emergent Energetics of Complex Dynamics

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    Stochastic kinematic description of a complex dynamics is shown to dictate an energetic and thermodynamic structure. An energy function Ο†(x)\varphi(x) emerges as the limit of the generalized, nonequilibrium free energy of a Markovian dynamics with vanishing fluctuations. In terms of the βˆ‡Ο†\nabla\varphi and its orthogonal field Ξ³(x)βŠ₯βˆ‡Ο†\gamma(x)\perp\nabla\varphi, a general vector field b(x)b(x) can be decomposed into βˆ’D(x)βˆ‡Ο†+Ξ³-D(x)\nabla\varphi+\gamma, where βˆ‡β‹…(Ο‰(x)Ξ³(x))=\nabla\cdot\big(\omega(x)\gamma(x)\big)= βˆ’βˆ‡Ο‰D(x)βˆ‡Ο†-\nabla\omega D(x)\nabla\varphi. The matrix D(x)D(x) and scalar Ο‰(x)\omega(x), two additional characteristics to the b(x)b(x) alone, represent the local geometry and density of states intrinsic to the statistical motion in the state space at xx. Ο†(x)\varphi(x) and Ο‰(x)\omega(x) are interpreted as the emergent energy and degeneracy of the motion, with an energy balance equation dΟ†(x(t))/dt=Ξ³Dβˆ’1Ξ³βˆ’bDβˆ’1bd\varphi(x(t))/dt=\gamma D^{-1}\gamma-bD^{-1}b, reflecting the geometrical βˆ₯Dβˆ‡Ο†βˆ₯2+βˆ₯Ξ³βˆ₯2=βˆ₯bβˆ₯2\|D\nabla\varphi\|^2+\|\gamma\|^2=\|b\|^2. The partition function employed in statistical mechanics and J. W. Gibbs' method of ensemble change naturally arise; a fluctuation-dissipation theorem is established via the two leading-order asymptotics of entropy production as Ο΅β†’0\epsilon\to 0. The present theory provides a mathematical basis for P. W. Anderson's emergent behavior in the hierarchical structure of complexity science.Comment: 7 page

    Criticality in Translation-Invariant Parafermion Chains

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    In this work we numerically study critical phases in translation-invariant ZN\mathbb{Z}_N parafermion chains with both nearest- and next-nearest-neighbor hopping terms. The model can be mapped to a ZN\mathbb{Z}_N spin model with nearest-neighbor couplings via a generalized Jordan-Wigner transformation and translation invariance ensures that the spin model is always self-dual. We first study the low-energy spectrum of chains with only nearest-neighbor coupling, which are mapped onto standard self-dual ZN\mathbb{Z}_N clock models. For 3≀N≀63\leq N\leq 6 we match the numerical results to the known conformal field theory(CFT) identification. We then analyze in detail the phase diagram of a N=3N=3 chain with both nearest and next-nearest neighbor hopping and six critical phases with central charges being 4/54/5, 1 or 2 are found. We find continuous phase transitions between c=1c=1 and c=2c=2 phases, while the phase transition between c=4/5c=4/5 and c=1c=1 is conjectured to be of Kosterlitz-Thouless type.Comment: published versio
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