Physics:Lee–Yang theorem

In statistical mechanics, the Lee–Yang theorem states that if partition functions of certain models in statistical field theory with ferromagnetic interactions are considered as functions of an external field, then all zeros are purely imaginary (or on the unit circle after a change of variable). The first version was proved for the Ising model by T. D. Lee and C. N. Yang (1952) (Lee Yang). Their result was later extended to more general models by several people. Asano in 1970 extended the Lee–Yang theorem to the Heisenberg model and provided a simpler proof using Asano contractions. (Simon Griffiths) extended the Lee–Yang theorem to certain continuous probability distributions by approximating them by a superposition of Ising models. (Newman 1974) gave a general theorem stating roughly that the Lee–Yang theorem holds for a ferromagnetic interaction provided it holds for zero interaction. (Lieb Sokal) generalized Newman's result from measures on R to measures on higher-dimensional Euclidean space.

There has been some speculation about a relationship between the Lee–Yang theorem and the Riemann hypothesis about the Riemann zeta function; see (Knauf 1999).

Statement

Preliminaries

Along the formalization in (Newman 1974) the Hamiltonian is given by

[math]\displaystyle{ H = -\sum J_{jk} S_j S_k - \sum z_j S_j }[/math]

where S_j's are spin variables, z_j external field. The system is said to be ferromagnetic if all the coefficients in the interaction term J_jk are non-negative reals.

The partition function is given by

[math]\displaystyle{ Z = \int e^{- H} d\mu_1(S_1)\cdots d\mu_N(S_N) }[/math]

where each dμ_j is an even measure on the reals R decreasing at infinity so fast that all Gaussian functions are integrable, i.e.

[math]\displaystyle{ \int e^{b S^2} d|\mu_j(S)| \lt \infty , \, \forall b \in \mathbb{R}. }[/math]

A rapidly decreasing measure on the reals is said to have the Lee-Yang property if all zeros of its Fourier transform are real as the following.

[math]\displaystyle{ \int e^{h S} d\mu_j(S) \neq 0 , \, \forall h \in \mathbb{H}_{+} := \{ z \in \mathbb{C} \mid \Re(z)\gt 0 \} }[/math]

Theorem

The Lee–Yang theorem states that if the Hamiltonian is ferromagnetic and all the measures dμ_j have the Lee-Yang property, and all the numbers z_j have positive real part, then the partition function is non-zero.

[math]\displaystyle{ Z(\{ z_j \}) \neq 0 , \, \forall z_j \in \mathbb{H}_{+} }[/math]

In particular if all the numbers z_j are equal to some number z, then all zeros of the partition function (considered as a function of z) are imaginary.

In the original Ising model case considered by Lee and Yang, the measures all have support on the 2 point set −1, 1, so the partition function can be considered a function of the variable ρ = e^πz. With this change of variable the Lee–Yang theorem says that all zeros ρ lie on the unit circle.

Examples

Some examples of measure with the Lee–Yang property are:

• The measure of the Ising model, which has support consisting of two points (usually 1 and −1) each with weight 1/2. This is the original case considered by Lee and Yang.
• The distribution of spin n/2, whose support has n+1 equally spaced points, each of weight 1/(n + 1). This is a generalization of the Ising model case.
• The density of measure uniformly distributed between −1 and 1.
• The density [math]\displaystyle{ \exp(-\lambda\cosh(S))\,dS }[/math]
• The density [math]\displaystyle{ \exp(-\lambda S^4-bS^2)\,dS }[/math] for positive λ and real b. This corresponds to the (φ⁴)₂ Euclidean quantum field theory.
• The density [math]\displaystyle{ \exp(-\lambda S^6- aS^4-bS^2)\,dS }[/math] for positive λ does not always have the Lee-Yang property.
• If dμ has the Lee-Yang property, so does exp(bS²) dμ for any positive b.
• If dμ has the Lee-Yang property, so does Q(S) dμ for any even polynomial Q all of whose zeros are imaginary.
• The convolution of two measures with the Lee-Yang property also has the Lee-Yang property.

See also

• Lee–Yang theory

References

• Itzykson, Claude; Drouffe, Jean-Michel (1989), Statistical field theory. Vol. 1, Cambridge Monographs on Mathematical Physics, Cambridge University Press, ISBN 978-0-521-34058-8 
• Knauf, Andreas (1999), "Number theory, dynamical systems and statistical mechanics", Reviews in Mathematical Physics 11 (8): 1027–1060, doi:10.1142/S0129055X99000325, ISSN 0129-055X, Bibcode: 1999RvMaP..11.1027K 
• Lee, T. D.; Yang, C. N. (1952), "Statistical Theory of Equations of State and Phase Transitions. II. Lattice Gas and Ising Model", Physical Review 87 (3): 410–419, doi:10.1103/PhysRev.87.410, ISSN 0031-9007, Bibcode: 1952PhRv...87..410L 
• Lieb, Elliott H.; Sokal, Alan D. (1981), "A general Lee-Yang theorem for one-component and multicomponent ferromagnets", Communications in Mathematical Physics 80 (2): 153–179, doi:10.1007/BF01213009, ISSN 0010-3616, Bibcode: 1981CMaPh..80..153L, http://projecteuclid.org/euclid.cmp/1103919874 
• Newman, Charles M. (1974), "Zeros of the partition function for generalized Ising systems", Communications on Pure and Applied Mathematics 27 (2): 143–159, doi:10.1002/cpa.3160270203, ISSN 0010-3640 
• Simon, Barry; Griffiths, Robert B. (1973), "The (φ⁴)₂ field theory as a classical Ising model", Communications in Mathematical Physics 33 (2): 145–164, doi:10.1007/BF01645626, ISSN 0010-3616, Bibcode: 1973CMaPh..33..145S, http://projecteuclid.org/euclid.cmp/1103859251 
• Yang, C. N.; Lee, T. D. (1952), "Statistical Theory of Equations of State and Phase Transitions. I. Theory of Condensation", Physical Review 87 (3): 404–409, doi:10.1103/PhysRev.87.404, ISSN 0031-9007, Bibcode: 1952PhRv...87..404Y