Abstract

A method of the Riemann–Hilbert problem is applied for Zhang’s conjecture 1 proposed in Philo. Mag. 87 (2007) 5309 for a ferromagnetic three-dimensional (3D) Ising model in the zero external field and the solution to the Zhang’s conjecture 1 is constructed by use of the monoidal transform. At first, the knot structure of the ferromagnetic 3D Ising model in the zero external field is determined and the non-local behavior of the ferromagnetic 3D Ising model can be described by the non-trivial knot structure. A representation from the knot space to the Clifford algebra of exponential type is constructed, and the partition function of the ferromagnetic 3D Ising model in the zero external field can be obtained by this representation (Theorem I). After a realization of the knots on a Riemann surface of hyperelliptic type, the monodromy representation is realized from the representation. The Riemann–Hilbert problem is formulated and the solution is obtained (Theorem II). Finally, the monoidal transformation is introduced for the solution and the trivialization of the representation is constructed (Theorem III). By this, we can obtain the desired solution to the Zhang’s conjecture 1 (Main Theorem). The present work not only proves the Zhang’s conjecture 1, but also shows that the 3D Ising model is a good platform for studying in deep the mathematical structure of a physical many-body interacting spin system and the connections between algebra, topology, and geometry.

Highlights

  • The study on the Ising model has attracted intensive interest since the 1920s [1], which applies to interpret phase transitions and critical phenomena in different fields, and provides fundamental understanding on interactions and dimensionality in nature.Onsager derived the exact solution of a two-dimensional (2D) Ising model in the zero external field, in which no non-trivial topological structures exist [2]

  • The ferromagnetic 3D Ising model we studied has the nearest neighboring interaction only, the nature of three dimensions results in two different behaviors for the interactions: (i) Cj or s0j s0j+1 represents the nearest interaction along the first or second dimension, and (ii) s0j s0j+n represents the nearest interaction along the third dimension, which consists of the non-local behavior, namely, a kind of long-range many-body entanglement

  • We introduce the K/C algebra which is an extension of Clifford algebra of the ferromagnetic 3D Ising model

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Summary

A Method of Riemann–Hilbert Problem for Zhang’s Conjecture

Method of Riemann–Hilbert Problem for Zhang’s Conjecture 1 in a Ferromagnetic 3D Ising Model: Trivialization of Topological Structure.

Introduction
Hamiltonian and Partition Function of 3D Ising Model
Zhang’s Conjecture 1
Clifford Algebra of the Ferromagnetic 3D Ising Model
Knot Structure of the Ferromagnetic 3D Ising Model
Knots with Clifford Algebra Data
Acalled knot called basicof form
Realization of Knots on a Riemann Surface
Realization
Realization on a Riemann
Method
Riemann-Hilbert Problem
Riemann–Hilbert Problem for the Ferromagnetic 3D Ising Model
Construction of Trivialization
Direction
Monoidal Transform
Complex Line Bundle of Monoidal Transformation given as follows
Construction of Monoidal
Basic Notations on Trivialization
18. Identification
Construction of Solution to the Zhang’s Conjecture 1
Conclusions
ProofThe of authors
Clifford

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