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4
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0003493230
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For a review, see, edited by C. Domb and J. Lebowitz (Academic Press, New York
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For a review, see J. F. Nagle, C. S. O. Yokio, and S. M. Bhattacharjee, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. Lebowitz (Academic Press, New York, 1980), Vol. 13.
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(1980)
Phase Transitions and Critical Phenomena
, vol.13
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Nagle, J.F.1
Yokio, C.S.O.2
Bhattacharjee, S.M.3
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9
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0000219340
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The precise connection between classical and quantum correlations requires additional assumptions about the ergodicity of the quantum dimer Hamiltonian in the space of dimer configurations (Refs. 7 and 9). This problem was addressed for a finite triangular lattice with open boundary conditions in
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The precise connection between classical and quantum correlations requires additional assumptions about the ergodicity of the quantum dimer Hamiltonian in the space of dimer configurations (Refs. 7 and 9). This problem was addressed for a finite triangular lattice with open boundary conditions in C. Kenyon and E. Remila, Discrete Math. 152, 191 (1996).
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(1996)
Discrete Math.
, vol.152
, pp. 191
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Kenyon, C.1
Remila, E.2
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11
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0000816199
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F. Y. Wu, Phys. Rev. 168, 539 (1967).
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(1967)
Phys. Rev.
, vol.168
, pp. 539
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Wu, F.Y.1
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21
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85038269506
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An actual magnetic model will exhibit a finite density of spinons as a finite temperature. Our diagnostic is the equivalent of the “Polyakov loop” for gauge theories without dynamical matter, at finite temperatures. The latter measures the free energy of two static quarks at varying separations
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An actual magnetic model will exhibit a finite density of spinons as a finite temperature. Our diagnostic is the equivalent of the “Polyakov loop” for gauge theories without dynamical matter, at finite temperatures. The latter measures the free energy of two static quarks at varying separations.
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22
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85038329812
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This problem was concurrently studied numerically (by Monte Carlo simulations and by exact enumeration) by, unpublished
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This problem was concurrently studied numerically (by Monte Carlo simulations and by exact enumeration) by W. Krauth and R. Moessner, (unpublished).
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Krauth, W.1
Moessner, R.2
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25
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85038286280
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The corresponding expression for g in Ref. 9 contains an error in the sign of the argument of the first exponential, which is corrected here
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The corresponding expression for g in Ref. 9 contains an error in the sign of the argument of the first exponential, which is corrected here.
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32
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85038285175
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private communication
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K. Shtengel (private communication).
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Shtengel, K.1
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38
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85038339454
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We thank Michael Fowler for providing this proof
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We thank Michael Fowler for providing this proof.
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