2d ising cft
Analyzing the two dimensional Ising model with conformal eld
plication to the statistical mechanical Ising model of ferromagnetism is presented This approach allows to highlight the connections between phenomena at criticality and quantum eld theory in particular the model of a free fermion Starting from a classical picture the Ising model is quantized |
2D CFT and the Ising Model
2D CFT and the Ising Model Alex Atanasov December 27 2017 Abstract In this lecture we review the results of Appendix E from the seminal paper by Belavin Polyakov and Zamolodchikov on the critical scaling exponents of the 2D Ising model by studying the conformal eld theory of a free massless fermion system 1 Review of 2D CFT Basics |
Conformal Field Theory
Aim: to understand CFT’s in 2d Why? (A)Second order phase transitions in 2d systems (so-called critical phenomena) For example the 2d Ising model Take a 2d lattice of critical sites (in principal this is assumed to be in nite): a ˙spin1 2 These spins are equipped with a nearest neighbor interaction |
Which coset model describes a 2D CFT with ZK Symme-try?
k + 2 k + 2 which is equal to (5.94). Indeed, this coset model describes the 2d CFT with Zk symme-try [FZ85, ISZ88-No.14]. This model contains a current with fractional spin (conformal dimension), which does obey neither bose nor fermi statistics, and is rather subject to para-statistics. Therefore, it is called parafermion. Zk
Which 2D CFT is the most important?
Since the Ising model is the most important 2d CFT, let us investigate it more in detail. For the Ising model on a lattice of (N M) sites, the statistical partition function is where we define K = J/(kBT). One can use the identity At high temperature, tanh . K is small and one can take expansion.
What is an example of a 2D Ising model?
For example, the 2d Ising model. Take a 2d lattice of These spins are equipped with a nearest neighbor interaction. The 2. j #i). is the inverse temperature. j. ! ! 0. If ! and the system reaches criticality. Ising model at criticality. meaning. It concerns itself with the time evolution of 1d objects reparametrization invariant and Weyl invariant.
Can radial quantization be used in a 2D CFT?
However, in a 2d CFT, it is most convenient to work in the complex coordinate with the Euclidean signature. In fact, there is a natural choice in the context of string theory by using radial quantization. We may first define our theory on an infinite space-time cylinder, with time t going from to along the “flat” direc-
1 Introduction
Conformal field theories have been at the center of much attention during the last few decades since they have been relevant for at least three different areas of modern theoretical physics: quantum field theories at an infra-red fixed point, two-dimensional critical phenomena, string theory. 2d CFTs are moreover placed on mathematically rig-orous
1.1 Renormalization group flow and Wilson-Fisher fixed points
In quantum field theory, a partition function is conceptually defined by using Feyn-man path integral. The basic integration variables are the Fourier modes fk of a field f. With a cutoff L, we schematically write arxiv.org
CFT2
By naive dimensional analysis, the possible parameter space becomes finite-dimensional. Although one can consider infinitely many interaction terms arxiv.org
Sint = Z ddx å giOi(f) ,
the terms with d < i are suppressed at low energy, which are called irrelevant. D Oi Therefore, we just need to consider finitely many terms Oi with d i at low energy. D To understand the behavior of a theory for these terms, we need to consider the beta function b(g) which describes how the coupling parameter g changes in terms of energy scale : arxiv.org
3.4 Example: Free boson
Now we will study the free boson field as an example. We first review some basic concepts in field theory. arxiv.org
Radial quantization
In the previous discussion, we find that operator formalism distinguishes a time di-rection from a space direction. However, in a 2d CFT, it is most convenient to work in the complex coordinate with the Euclidean signature. In fact, there is a natural choice in the context of string theory by using radial quantization. We may first define our theor
Iw dz a(z)b(w) = dz a(z)b(w) dz b(w)a(z) = [A, b(w)] , (3.92)
where the operator A is the contour integral of a(z) at a fixed time arxiv.org
4 Free boson and free fermion
In this section, we are going to demonstrate more simple examples in CFT. arxiv.org
4.1 Free boson
In the previous sections, we have learned the calculation of some basic OPEs in the massless free boson theory. We will further study this theory. arxiv.org
2 z w
When w z, this result coincides with the previous one. So, the boundary condition does not affect the two-point function locally. However, globally when z or w is taken around the origin, there arises a minus sign due to the boundary condition. We find that different boundary conditions lead to different two-point functions on the plane. arxiv.org
Z Z2.
fore, it is sufficient to check whether a theory is modular invariant by studying its behav-ior under T and S transformations. arxiv.org
Torus partition function
Now we will define a torus partition function Z in terms of Virasoro generators. The story is analogous to the partition function in statistical mechanics arxiv.org
24 cAA(t) .
On the other hand, the modular S-transformation leads to arxiv.org
Kac Determinant
A representation of the Virasoro algebra is said to be unitary if it contains no negative-norm states. In the section of Verma module, we have mentioned that the negative of central charge and highest weight will make the states non-unitary. As we will see below, the unitarity imposes strong constraints on (c, h). In addition to unitarity, one has
3-state Potts model (p0, p) = (6, 5)
On a square lattice, the hamiltonian of the three-state Potts model is given by J arxiv.org
o , g(n)
i in this way. Then, ignoring an overall constant, we have the equivalence of the statistical partition functions å exp h arxiv.org
g = R (g )
Since the coarse-graining does not affect the theory, it is scale-invariant, implying that it is conformal. As briefly explained in the introduction, critical phenomena are described by these fixed points. arxiv.org
Affinization
Hence, one can straightforwardly generalize the current associated to a Lie algebra g as follows. First, the current taking its value on a Lie algebra g can be written arxiv.org
S G
where is generally a two-dimensional manifold, called a Riemann surface. Under the S variation of the action arxiv.org
(z w)2 i fabc . åc (z w)
Introducing the modes Ja n from the Laurent expansion arxiv.org
T(z) = åz n 2Ln . (7.42) n2Z
With the OPEs listed above, we can compute the complete affine Lie and Virasoro algebra c arxiv.org
z w
This can be generalized to define a WZNW primary field. Any WZNW primary field fl,m with l and m specified the representation in the holomorphic and antiholomorphic sector respectively should satisfy the following OPE arxiv.org
Tg/h := Tg Th . bgkg/bhkh
Then, we have Jb h(w) ¶w jb ̇ h(w) Tg(z)Jb h(w) = + + arxiv.org
Rational conformal field theories
The minimal models, the WZNW models and the coset models belong to a class of rational conformal field theories (RCFTs). A theory is endowed with a chiral algebra A that contains the Virasoro algebra as a subalgebra. The definition of an RCFT is (roughly) given as follows. It is unitary with a unique vacuum. There are finitely many primary fields f
Boundary
Figure 32: Holographic entanglement entropy As we will see at the end, when the region A is large enough, the minimal surface (submanifold) wraps the horizon of AdS black hole, and the RT formula can explain the Bekenstein-Hawking entropy as a special case. However, minimal surfaces (submani-folds) are more general so that the RT formula can be int
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The two dimensional Ising model
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Integrals of Motion in the 2 Dimensional Ising Model and Lattice
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