Phase Transitions and Critical Phenomena

By M. Fisher. 2021

3,771 citations recorded by the source corpus.

Subfields: Computational Theory and Mathematics, Materials Chemistry, Statistical and Nonlinear Physics

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Citations in the corpus

Action Semantics Network: Considering the Effects of Actions in Multiagent Systems (2019, background): “Recently, Yang et al. (2018) proposed applying mean-ﬁeld theory (Stanley, 1971) to solve large-scale multiagent learning problems.”
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Spin Ice State in Frustrated Magnetic Pyrochlore Materials (2001, background): “These include “energetic” generalisations of the ice model that display a wealth of interesting thermodynamic phenomena in close resemblance with those observed in real ice ( [12,13]).”
Computational structure characterisation tools in application to ordered and disordered porous materials (2011, methodology): “A simple recursive algorithm is used to calculate the distribution of the clusters in the system given the xyz coordinates of the particles and the mean cluster size S using [16]:”
The interplay of surface segregation and atomic order in alloys (2000, background): “However, for a second-order transition at the Fe±27%Al alloy boundaries, a different behavior consistent with the theoretically expected power law [177] was observed [178].”
Imbalanced Feshbach-resonant Fermi gases (2009, background): “A more detailed check on the consistency of the interpretation can come from a comparison with the predictions for the cloud shape, heat capacity, and local polarization controlled by the mean-field tricritical point [117], which are predicted to follow distinct power laws [150, 151].”
Collective behavior of interacting self-propelled particles (2000, background): “(1) and (2) is a transport related, non-equilibrium analog of ferromagnetic models [17].”
Quantum spin-ice and dimer models with Rydberg atoms (2014, background): “So the classical phase gives way to a Coulomb gas [61, 62], an approximate realization of a classical Coulomb phase, with only a very small density of defects.”
The QCD phase diagram for small densities from imaginary chemical potential (2002, background): “However, in the presence of a complex chemical potential, a Z(N) transformation of the fermion fields is equivalent to a shift in µI , thus leading to a new symmetry: the partition function is periodic in µI with period 2πT/N [13], Z(µ̄R, µ̄I) = Z(µ̄R, µ̄I + 2π/N).”
LATTICE QCD AT FINITE TEMPERATURE (2003, background): “The “resonance” like enhancement of σV results in the enhancement of the dilepton rate over the perturbative tree level (Born) rate [103] for energies p0/T ∈ [4, 8].”
Quasilocal charges in integrable lattice systems (2016, background): “Besides defining and describing integrability in closed quantum many-body systems in 1D [7], it also covers 2D equilibrium classical statistical systems [8], nonequilibrium classical driven diffusive 1D systems [9], as well as classical Hamiltonian systems [10,11], and since more recently, also inte”