1979
DOI: 10.1103/physrevb.20.2797
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Tricritical coexistence in three dimensions: The multicomponent limit

Abstract: The asymptotic tricritical equation of state, including the three=phase coexistence monohedron, is analyzed in detail for the exactly soluble multicomponent or spherical limit, n~, of the continuous-spin model with terms of order s, s, and s, in d =3 spatial dimensions. Various nonuniversal scaling functions and amplitude ratios, depending on the range parameter z~1/Ro, are evaluated explicitly and reveal the nature and magnitude of the deviations from the classical, phenomenological theory of tricriticality (… Show more

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Cited by 40 publications
(5 citation statements)
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“…( 22) and ( 24) we can form the universal ratio φ sd /φ c = 3, which, since λ ∼ T − Θ, measures the ratio of the slopes of the wing critical line and the phase separation boundary in the semi-dilute limit. The result φ sd /φ c = 3 coincides with Flory theory but differs from the result φ sd /φ c = 5/2 [25,26] that one finds from the Landau expansion by keeping h 2 constant instead of N in the calculation of the wing critical line. To our knowledge the only attempt to independently obtain this universal ratio was made in simulations by Frauenkron and Grassberger [27,28].…”
Section: Mean-field Descriptioncontrasting
confidence: 56%
“…( 22) and ( 24) we can form the universal ratio φ sd /φ c = 3, which, since λ ∼ T − Θ, measures the ratio of the slopes of the wing critical line and the phase separation boundary in the semi-dilute limit. The result φ sd /φ c = 3 coincides with Flory theory but differs from the result φ sd /φ c = 5/2 [25,26] that one finds from the Landau expansion by keeping h 2 constant instead of N in the calculation of the wing critical line. To our knowledge the only attempt to independently obtain this universal ratio was made in simulations by Frauenkron and Grassberger [27,28].…”
Section: Mean-field Descriptioncontrasting
confidence: 56%
“…Conversely, the parameter z exhibits a relatively smaller value for the fit range-C. The extracted z values for the smaller fit ranges in the present system reveal a well agreement with the reported values at the tricritical N-Sm-A phase transition for polar cyanobiphenyls [73], while they are found to be quite higher than the reported values of z = 0.12 for 3 He- 4 He mixtures and z = 0.21 for the metamagnet Dy 3 Al 5 O 12 [Dysprosium Aluminum Garnet (DAG)] [75,76]. Therefore, it can be concluded that the order character of the Sm-A-Sm-C transition for the mixtures x 7OCB = 0.1, 0.125, 0.15, 0.158, 0.167 and 0.174 are truly tricritical in nature.…”
Section: Tricritical Fitssupporting
confidence: 90%
“…Hence, in the present system the extracted values of the quotient / -+ A A are non-universal over the variation of fit ranges. According to Fisher and Sarbach [75,76], this type of amplitude ratio at the tricritical point can be well described by an exactly solvable spherical (n = ∞) model, where / -+ A A is a function of the single variable…”
Section: Tricritical Fitsmentioning
confidence: 99%
“…At the tricritical point K, the coefficient of A 3 in the bifurcation equation (26) vanishes. We can unfold this bifurcation by expanding the free energy up to O( 6 ) terms [32,33] and rescaling the bifurcation parameters. If we set…”
Section: B Bifurcation At the Tricritical Pointmentioning
confidence: 99%
“…Again, C eq is found by looking for the extrema of ∆F , and C eq = O( ). By introducing C eq = A, we have that A is the solution of the biquadratic equation (33). Let us denote by A 2 ± the two solutions of Eq.…”
Section: Appendix C: Effective Hamiltonian Landscapementioning
confidence: 99%