**World Journal of Condensed Matter Physics**

Vol.05 No.02(2015), Article ID:55287,4 pages

10.4236/wjcmp.2015.52008

Violating of the Essam-Fisher and Rushbrooke Relationships at Low Temperatures

Vladimir Udodov

Department of Theoretical Physics, Katanov Khakas State University, Abakan, Russia

Email: udododvv@hotmail.com

Copyright © 2015 by author and Scientific Research Publishing Inc.

This work is licensed under the Creative Commons Attribution International License (CC BY).

Received 4 January 2015; accepted 30 March 2015; published 1 April 2015

ABSTRACT

The Essam-Fisher and Rushbrooke relationships (1963) that connect the equilibrium critical exponents of susceptibility, specific heat and order parameter (and some other relations that follow from the scaling hypothesis) are shown to be valid only if the critical temperature T_{С} > 0 and T → T_{C}. For phase transitions (PT’s) with T_{C} = 0 K these relations are proved to be of different form. This fact has been actually observed experimentally, but the reasons were not quite clear. A general formula containing the classical results as a special case is proposed. This formula is applicable to all equilibrium PT’s of any space dimension for both T_{C} = 0 and T_{C} > 0. The predictions of the theory are consistent with the available experimental data and do not cast any doubts upon the scaling hypothesis.

**Keywords:**

Essam-Fisher and Rushbrooke Relationships, The Equilibrium Critical Exponents, The Scaling Hypothesis, Low Temperatures

1. Introduction

The critical exponents and scaling hypothesis (Patashinsky and Pokrovsky (1964); Widom (1965); Domb and Hunter (1965); Kadanoff (1966)) underlying the theory of critical phenomena [1] -[5] . Essam and Fisher equality [6] and Rushbrooke inequality [7] (as the most famous inequality between critical exponents) were discovered 52 years ago and everyone believed that the relations are performed. These relations are connected with the critical exponents of the specific heat (α, α'), susceptibility (γ, γ') and the order parameter β (determining of the critical exponents see below) [1] - [7] . In 1965-1966, it was shown that under the scaling hypothesis the Essam and Fisher equality are fulfilled and the Rushbrooke inequality reduces to equality [1]

.)

These results were obtained under the assumption that the critical temperature is finite T_{С} > 0 and T→T_{C}. However, recently quantum phase transitions (PT’s) have inspired a new interest in low-temperature thermodynamics and statistical physics [8] - [10] . For quantum PT’s the temperature of phase transition T_{C} is zero. In this paper we show that if T_{С} = 0 K, the classical Essam-Fisher equation and Rushbrooke inequality changes: the right-hand side equal to two, is replaced by one. Change as well, and some other equations for the critical exponents resulting from the scaling hypothesis. In this paper, we propose a general interpolation formula (generalized Essam-Fisher equality), the right side of which ranges from 2 to 1. This general formula is valid for both finite critical temperature and for the case of T_{С} = 0 K. In the experimental measurements of the critical exponents for the PT's at low temperatures (T → 0) we can expect that the right side of these relations will be less than 2 [1] . The proposed theory can be tested for any quantum phase transitions [8] -[11] .

Even now there is evidence that these relations are broken. For example, for the magnetic transition in nickel we have [12] (within the framework of the scaling hypothesis γ = γ')

.

For the critical point in CO_{2} [12] , for example,

.

Explanations of these violations were absent apart from possible measurement errors, but everyone believed that the formulas are correct, since derived from thermodynamics. The situation is complicated by the fact that a breach of these relationships speaks about the disturbance of the scaling hypothesis [1] - [5] . Though the apparent violations of the scaling hypothesis are discussed by Aharony and Ahlers [13] , they did not consider the case of zero critical temperature.

It turns out, if T_{С} = 0, the classic relationships [6] [7] have the different form and this may be explains the apparent violations and it can save the scaling hypothesis.

2. The Essam and Fisher Equality

First, we recall the usual derived Essam-Fisher equality. The order parameter in a weak field (or lack thereof) is proportional to [1] - [3]

(1)

where, β is order parameter critical exponent. On the other hand in a weak field h, the order parameter is [3]

(2)

where χ?susceptibility, the critical exponent is determined by the ratio (in a weak field) [1] - [3]

(3)

γ?the critical exponent of the susceptibility. In the field PT becomes fuzzy. If we substitute Equations (1) and (3) in Equation (2), we find blur for temperature interval of PT [3]

(4)

from which we obtain

(5)

The same interval of blur can be found from the requirement that a field term of potential G_{h} is equal to a heat term G_{T} [3] (G?the Gibbs potential [1] - [3] )

(6)

where С_{р}?heat capacity, for which the formula is valid in weak field [1] -[3]

(7)

α, α'?the heat capacity critical exponents, within the framework of the scaling hypothesis α = α' [1] . Substituting Equations (5) and (7) into Equation (6) this gives

(8)

or

(9)

it is Essam and Fisher equality [1] [3] [6] .

Longer arguments prove Rushbrooke inequality [1] [7] , which is true for the stable states

(10)

where the primed symbols correspond to the region below the PT point (at temperature), the order parameter critical exponent β is defined only in this area [1] -[3] . In rare cases, the asymmetric phase can be high-temperature phase [3] , then the exponent β is determined for.

3. The Case of Zero Critical Temperature

Note that the heat term has the form (6) only if T_{С} > 0. In fact, let

(11)

We show that the heat term G_{T} in the form shown in Equation (6) leads to incorrect results. From Equation (11) it follows that

(12)

The thermal term becomes in the form (within the framework of the scaling hypothesis)

(13)

We find the entropy

(14)

and heat capacity (using Equations (12) and (14))

(15)

which contradicts Equation (7).

Let us find the right formula. Let heat term has the form

(16)

We now find b. Heat capacity is

(17)

hence we have

and

(18)

Essam and Fisher equality will take the form [14]

(19)

which differs from the standard formula (9) [1] -[3] [6] .

4. The General Case

In the general case may be offered the following interpolation formula (generalized Essam-Fisher equality)

(20)

where S-function is [14]

(21)

where positive constant n can be found either from the comparison with experiment, or from the microscopic theory. Indeed, if the T_{C} = 0 (T > 0), then we arrive at the formula (19). If T_{C}^{ }> 0 and T → T_{C}, we get a classical Essam and Fisher equality (9).

Turns out, if the number n is fraction, then S-function is a nonanalitic function at a point. For example, if, then the first derivative tends to infinity,. If n is an integer, then the function can be decomposed into a series of x. For, we get decomposition into a series accurate within quadratic term

(22)

Now consider the case. S-function is rewritten as

where

(23)

Now the S-function is analytic function at a point. The decomposition into a series is

(24)

where. Note that formulas (23) and (24) it is also true if Т_{С} → 0, however τ → 0, it follows from this Т → 0. Rushbrooke inequality in the general case is given by

(25)

that is, the right-hand side of equality (25) can be less than 2. We obtained a principal result: the right side of the classic relationships is not a constant, but rather a function that depends on the temperature and takes the values from 1 to 2.

Finally, two equalities which follow from the scaling hypothesis [1] [3]

(26)

(27)

alter their appearance (d?the space dimension, ν?critical exponent of the correlation length). ε?critical exponent for strong field [3]

(28)

Scaling relations now take the form

(29)

(30)

r?phase transition order in the sense of Baxter R. [2] , we believe that the scaling hypothesis is performed.

It should be noted that the S-function expresses the degree of “classical” behavior. Thus, for the non-classical behavior and T_{С} = 0 and corresponds to the known regime [6] [7] .

5. Conclusions

Thus showed that the classical Essam and Fisher equation and Rushbrooke inequality are only valid if the critical temperature T_{C} is finite and T → T_{C}. If the critical temperature is zero, the classic relationships change its form: on the right side instead of the deuce will be unit. Because at change of parameters critical temperature tends to zero for many quantum phase transitions, the right-hand side of these relations should be continuously varied from 2 to 1 [14] .

The real test of the results is possible for any quantum phase transitions [9] [10] as T → 0, for example for ferromagnetic Ce_{2.15}Pd_{1.95}In_{0.9} [11] , for heavy-fermions systems [15] or for superconductors [10] .

We note that the relations (19), (20), (25) are equilibrium, which implies that the right side equal to one, is unlikely to be achieved because the relaxation time (the transition to the equilibrium state) at T → T_{C} ~ 0 tends to infinity (critical slowing). In conclusion, it must be emphasized that the results can be observed at temperatures not very low (see [12] ).

Acknowledgements

I thank S. Prosandeev and A. Levanyuk for discussions and I am grateful for discussions and the support to I. Naumov.

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