Compute 1D Ising Correlation w/ Periodic, Anti-Periodic BDs

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Homework Help Overview

The discussion revolves around computing correlation functions for the 1D Ising model under various boundary conditions, specifically periodic and anti-periodic conditions, as well as fixed boundary conditions. The original poster seeks clarification on the computation process and the role of the transfer matrix technique in this context.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the use of the transfer matrix technique for calculating the partition function and correlation functions. The original poster expresses confusion about transitioning between steps in the provided reference and the uniqueness of the transfer matrix for periodic boundary conditions. Others question the correctness of specific calculations and clarify the implications of different boundary conditions on the results.

Discussion Status

The conversation is ongoing, with participants exploring the implications of boundary conditions on calculations. Some guidance has been offered regarding the transfer matrix technique, but there remains uncertainty about its application across different boundary conditions.

Contextual Notes

There is mention of missing understanding regarding the transfer matrix technique and its dependence on boundary conditions, which may affect the calculations being discussed. The original poster also notes a missed lecture, which could contribute to their confusion.

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Homework Statement


Compute correlation functions ##<\sigma_r \sigma_{r+l}>## for the 1D Ising model of length L with the follow BD conditions

(i) Periodic
(ii) Anti-Periodic
(iii) ##\sigma_1 = \sigma_{L+1}=1##
(iv) ##\sigma_1= -\sigma_{L+1}=1##

Homework Equations



##<\sigma_r \sigma_{r+l}> = \displaystyle\frac{1}{Z}\sum_{\sigma_l=\pm 1}^{L-1}e^{K(\sum_{k=1}^{L-1}\sigma_k \sigma_{k+1} +\sigma_1 \sigma_{L+1})} \sigma_r \sigma_{r+l}##

The Attempt at a Solution


[/B]
I know how to compute the partition function for the periodic case as its fairly common and I have a solution to computing the correlation function to http://www.colorado.edu/physics/phys7240/phys7240_fa14/notes/Week1.pdf although I don't understand how he goes from 1.11 to 1.12.But these solutions use the Trace of the transfer matrix which I am pretty sure is unique to the periodic BD conditions. Any help on how to compute these in general would be appreciated as I missed the lecture on it.
 
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Did you understood the transfer matrix technique? the first n-1 spin sum just becomes the normal trace of the transfer matrix. But then you have \sigma_m, but the possible value of \sigma_m are 1 and -1, with introduction of pauli matrix(+1 and -1 remember?), it just becomes a normal trace once again.
 
jitu16 said:
Did you understood the transfer matrix technique? the first n-1 spin sum just becomes the normal trace of the transfer matrix. But then you have \sigma_m, but the possible value of \sigma_m are 1 and -1, with introduction of pauli matrix(+1 and -1 remember?), it just becomes a normal trace once again.

Can you explain why this explicit calculation of the 1D model with 3 sites and periodic BDs is incorrect

##Z=\displaystyle\sum_{\sigma_1=\pm1}\sum_{\sigma_2=\pm1}\sum_{\sigma_3=\pm1}e^{K(\sum_{k=1}^2\sigma_k \sigma_{k+1} + \sigma_3 \sigma_1)}##

##=\displaystyle\sum_{\sigma_1=\pm1}\sum_{\sigma_2=\pm1}\sum_{\sigma_3=\pm1}e^{K(\sigma_1 \sigma_2 + \sigma_2 \sigma_3 + \sigma_3 \sigma_1)}##

##=\displaystyle\sum_{\sigma_1=\pm1}\sum_{\sigma_2=\pm1}e^{K(\sigma_1 \sigma_2 + \sigma_2 + \sigma_1)}+e^{K(\sigma_1 \sigma_2 + -\sigma_2 + -\sigma_1)}##

##=\displaystyle\sum_{\sigma_1=\pm1}e^{K(\sigma_1 + 1 + \sigma_1)}+e^{K(\sigma_1 -1 + -\sigma_1)}+e^{K(-\sigma_1 -1 + \sigma_1)}+e^{K(-\sigma_1+ 1 + -\sigma_1)}##

##=e^{K(1 + 1 + 1)}+e^{K(1 -1 + -1)}+e^{K(-1 -1 + 1)}+e^{K(-1+ 1 + -1)}+e^{K(-1 + 1 + -1)}+e^{K(-1 -1 + 1)}+e^{K(1 -1 -1)}+e^{K(1+ 1 + 1)}##

##=e^{K(3)}+e^{K(-1)}+e^{K(-1)}+e^{K(-1)}+e^{K(-1)}+e^{K(-1)}+e^{K(-1)}+e^{K(3)}##

##=2e^{3K}+6e^{-K}##

nvm It's correct, I guess I don't understand how the transfer matrix works, I thought it was dependent on periodic BDs to get the trace
 
Last edited:
Which boundary condition are you referring to?? If it's periodic then your calculation is right but if it's anti-periodic then your calculation is wrong.
 

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