Magnetic susceptibility (Ising model)

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SUMMARY

The discussion centers on proving the relationship between magnetic susceptibility (\chi) and magnetization (\langle M \rangle) in the context of the Ising model. The formula \(\chi=\frac{\partial \langle M \rangle}{\partial H}\) is equated to \(\chi=\frac{\langle M^2 \rangle - \langle M \rangle^2}{T}\). Participants express \(\langle M \rangle\) as \(\frac{\sum M_s e^{-E/k_B T}}{\sum e^{-E/k_B T}}\), where \(E=-J\sum S_i S_j - H\sum S_i\). The discussion highlights the use of partial derivatives and the importance of understanding the partition function (Z) in this context.

PREREQUISITES
  • Understanding of the Ising model and its applications in statistical mechanics.
  • Familiarity with concepts of magnetic susceptibility and magnetization.
  • Knowledge of statistical thermodynamics, particularly the partition function (Z).
  • Proficiency in calculus, specifically in differentiation and partial derivatives.
NEXT STEPS
  • Study the derivation of the partition function (Z) in the Ising model.
  • Learn about the implications of the fluctuation-dissipation theorem in statistical mechanics.
  • Explore advanced topics in magnetic susceptibility, including critical phenomena.
  • Investigate numerical methods for simulating the Ising model, such as Monte Carlo simulations.
USEFUL FOR

Physicists, particularly those specializing in statistical mechanics, researchers studying magnetic materials, and graduate students in condensed matter physics will benefit from this discussion.

garyman
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Hi,

I'm slightly confused about how to prove that:

[tex]\chi[/tex]=[tex]\vartheta[/tex]<M>/[tex]\vartheta[/tex]H

is equal to...

[tex]\chi[/tex]=(<M2>-<M>2 )/ T

I've expressed <M> as [tex]\sum[/tex]Msexp(-E/kBT) /
[tex]\sum[/tex]exp(-E/kBT)

and know that E=-J[tex]\sum[/tex]SiSj-H[tex]\sum[/tex]Si

But seem to get lost in the differentiation. I am going aobut this the correct way?
 
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garyman said:
Hi,

I'm slightly confused about how to prove that:

[tex]\chi[/tex]=[tex]\vartheta[/tex]<M>/[tex]\vartheta[/tex]H

is equal to...

[tex]\chi[/tex]=(<M2>-<M>2 )/ T

I've expressed <M> as [tex]\sum[/tex]Msexp(-E/kBT) /
[tex]\sum[/tex]exp(-E/kBT)

and know that E=-J[tex]\sum[/tex]SiSj-H[tex]\sum[/tex]Si

But seem to get lost in the differentiation. I am going aobut this the correct way?

what is "[itex]M_s[/itex]"?

Also, you can use "\partial", i.e., "[itex]\partial[/itex]" for partial derivatives.
 
Firstly [tex]M=\sum_i S_i \neq M_s[/tex]? I can't really envision what [itex]M_s[/itex] would be at all. Secondly I personally find it easiest to solve this problem by first noticing that [tex]\langle M \rangle= k_b T \frac{\partial \log Z}{\partial h}[/tex] then compute [tex]\frac{\partial \langle M \rangle}{\partial h}[/tex].
 

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