How Does Mean Field Theory Explain Spontaneous Symmetry Breaking?

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SUMMARY

Mean Field Theory (MFT) effectively explains spontaneous symmetry breaking by demonstrating that a system can acquire finite magnetization at low temperatures when the Free Energy decreases upon breaking symmetry. The critical temperature is determined by solving a self-consistent equation, which aligns with the point where the Free Energy begins to decrease. Additionally, the divergence of correlation functions in the normal state serves as a simpler method for calculating this critical temperature, reinforcing the relationship between Free Energy and symmetry breaking.

PREREQUISITES
  • Understanding of Mean Field Theory (MFT)
  • Knowledge of Free Energy concepts in statistical mechanics
  • Familiarity with critical temperature calculations
  • Basic grasp of correlation functions in phase transitions
NEXT STEPS
  • Study the derivation of critical temperatures in Mean Field Theory
  • Explore the relationship between Free Energy and phase transitions
  • Learn about correlation functions and their role in symmetry breaking
  • Investigate applications of Mean Field Theory in various physical systems
USEFUL FOR

Physicists, particularly those specializing in statistical mechanics and condensed matter physics, as well as students seeking to understand the implications of Mean Field Theory in spontaneous symmetry breaking.

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I am bit confused by how to approach this concept with mean field theory. As I understand a symmetry break (like a acquiring a finite magnetization) can happen if at low enough temperatures the Free energy decreases when breaking the symmetry.
Normally this temperature is found by calculating a thermal average and solving a self-consistent equation for the critical temperature. But is it obvious, that this is the same as finding the critical temperature at which the free energy begins to decrease when breaking the symmetry?
 
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As far as I remember, it is usually simpler to calculate the critical temperature as that temperature where some correlation functions calculated for the normal state diverge.
 

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