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Relevant bibliographies by topics / Free energy perturbation theory

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Journal articles

Academic literature on the topic 'Free energy perturbation theory'

Author: Grafiati

Published: 4 June 2021

Last updated: 6 February 2022

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Journal articles on the topic "Free energy perturbation theory"

1

Mon, K. K. "Lower free energy bound for hard-sphere perturbation theory." Journal of Chemical Physics 116, no. 21 (2002): 9392–94. http://dx.doi.org/10.1063/1.1472507.

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2

Kalikmanov, V. I., R. Hagmeijer, and C. H. Venner. "Statistical Mechanical Perturbation Theory of Solid–Vapor Interfacial Free Energy." Journal of Physical Chemistry C 121, no. 12 (2017): 6868–73. http://dx.doi.org/10.1021/acs.jpcc.7b01331.

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3

Vilseck, Jonah Z., Julian Tirado-Rives, and William L. Jorgensen. "Determination of partial molar volumes from free energy perturbation theory." Physical Chemistry Chemical Physics 17, no. 13 (2015): 8407–15. http://dx.doi.org/10.1039/c4cp05304d.

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Free Energy Perturbation calculations are employed to determine free energies of solvation (ΔG<sub>solv</sub>) for benzene and benzene-derivatives at elevated pressures. Absolute and relative partial molar volumes are determined as the pressure derivative of ΔG<sub>solv</sub>.

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4

Topor, Nadia. "Perturbation Method for Boundary S-Matrix in 2D Quantum Field Theory." Modern Physics Letters A 12, no. 38 (1997): 2951–62. http://dx.doi.org/10.1142/s0217732397003071.

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We develop a perturbation theory for evaluating the boundary S-matrix in 2D quantum field theory. We apply this approach to calculate the one-loop boundary S-matrix for the elementary particle of the sine–Gordon model with a boundary interaction. Our perturbative result agrees with the exact expression of the S-matrix conjectured by Goshal; it also allows us to derive the perturbative relation between the parameter ϑ in the S-matrix and the free parameter M in the boundary action, in the particular case in which its other free parameter φ0 is zero.

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5

PERIWAL, VIPUL. "FREE ENERGY DECREASES ALONG WILSON RENORMALIZATION GROUP TRAJECTORIES." Modern Physics Letters A 10, no. 21 (1995): 1543–48. http://dx.doi.org/10.1142/s0217732395001666.

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The free energy is shown to decrease along Wilson renormalization group trajectories, in a dimension-independent fashion, for d>2. The argument assumes the monotonicity of the cutoff function, and positivity of a spectral representation of the two-point function. The argument is valid for all orders in perturbation theory.

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6

Tobias, Douglas J., and Charles L. Brooks. "Calculation of free energy surfaces using the methods of thermodynamic perturbation theory." Chemical Physics Letters 142, no. 6 (1987): 472–76. http://dx.doi.org/10.1016/0009-2614(87)80646-2.

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7

Nieto, Agustin. "Perturbative QCD at High Temperature." International Journal of Modern Physics A 12, no. 08 (1997): 1431–64. http://dx.doi.org/10.1142/s0217751x97001043.

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Recent developments of perturbation theory at finite temperature based on effective field theory methods are reviewed. These methods allow the contributions from the different scales to be separated and the perturbative series to be reorganized. The construction of the effective field theory is shown in detail for ϕ4 theory and QCD. It is applied to the evaluation of the free energy of QCD at order g5 and the calculation of the g6 term is outlined. Implications for the application of perturbative QCD to the quark–gluon plasma are also discussed.

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8

ABE, MITSUO, and NOBORU NAKANISHI. "NONRENORMALIZABILITY MAY BE SUPERFICIAL IN THE COVARIANT FORMALISM OF QUANTUM GRAVITY." Modern Physics Letters A 10, no. 21 (1995): 1501–6. http://dx.doi.org/10.1142/s0217732395001629.

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It is pointed out that the nonrenormalizability of quantum Einstein gravity may be caused by the inadequacy of the conventional perturbative approach. It is more reasonable to reconsider the problem in the light of a newly proposed perturbative scheme, which is free of the ad hoc assumption on which the conventional perturbation theory is based. It is explicitly shown that there is a gravity-theory example which is nonrenormalizable in the usual sense but completely finite if the new perturbative scheme is applied.

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9

MA, BO-QIANG, and JI SUN. "NEW SCALING VARIABLE FROM LIGHT-CONE PERTURBATION THEORY." International Journal of Modern Physics A 06, no. 03 (1991): 345–63. http://dx.doi.org/10.1142/s0217751x91000216.

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We argue from both the quark language and the free field light-cone expansion in light-cone perturbation theory that the constraint of overall “energy” conservation in deep inelastic lepton-nucleon scattering yields a similar new scaling variable xp, which reduces to the Weizmann variable, the Bloom-Gilman variable and the Bjorken variable at some approximations. The xp rescaling is expected to be a good scaling variable, and hence gives strong power-law type corrections to the deviations of Bjorken scaling. An understanding of this xp rescaling from both the free field operator product expans

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10

Greeff, C. W. "Tests of Monte Carlo perturbation theory for the free energy of liquid copper." Journal of Chemical Physics 128, no. 18 (2008): 184104. http://dx.doi.org/10.1063/1.2917355.

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