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The two-dimensional Coulomb plasma: quasi-free approximation and central limit theorem
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abstract
For the two-dimensional one-component Coulomb plasma, we derive an asymptotic expansion of the free energy up to order $N$, the number of particles of the gas, with an effective error bound $N^{1-\kappa}$ for some constant $\kappa > 0$. This expansion is based on approximating the Coulomb gas by a quasi-free Yukawa gas. Further, we prove that the fluctuations of the linear statistics are given by a Gaussian free field at any positive temperature. Our proof of this central limit theorem uses a loop equation for the Coulomb gas, the free energy asymptotics, and rigidity bounds on the local density fluctuations of the Coulomb gas, which we obtained in a previous paper.
Forward citations
Cited by 2 Pith papers
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Spectral rigidity of random Schr\"odinger operators via Feynman-Kac formulas
The spectrum of a large class of one-dimensional continuous random Schrödinger operators is number rigid under growth conditions on the deterministic potential, proved via Feynman-Kac variance estimates for exponentia...
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Partition function of 2D Coulomb gases with radially symmetric potentials and a hard wall
For radially symmetric potentials at beta = 2, the log N coefficient in the hard-wall partition function is -1/4 for an annulus and -1/3 for a disk when the wall lies strictly inside the droplet, instead of the usual -1/12.
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