Understanding Markov Chains in Metropolis Monte Carlo Ising Simulation

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Discussion Overview

The discussion revolves around the role of Markov chains in the context of Metropolis Monte Carlo simulations applied to the Ising model. Participants explore the relationship between lattice site transitions, spin flips, and the probabilistic nature of these processes.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant expresses confusion about the presence of Markov chains in the Monte Carlo Ising simulation, questioning how the random movement between lattice sites relates to this concept.
  • Another participant suggests that the next lattice site after a spin flip is determined by a probability distribution centered around the current site.
  • A follow-up question seeks clarification on what is meant by "probability distribution around the previous lattice site."
  • It is noted that the choice of the next lattice site is random but defined by a displacement from the current site.
  • A participant attempts to summarize their understanding, stating that the probability of remaining at the current position after a spin flip depends solely on the current configuration of spins, independent of prior moves.
  • This understanding is affirmed by another participant, indicating agreement with the summary provided.

Areas of Agreement / Disagreement

Participants generally agree on the concept that the probability of transitioning to a new lattice site depends only on the current state and not on the history of previous states. However, the initial confusion about the role of Markov chains suggests that some aspects of the discussion remain unresolved.

Contextual Notes

There may be limitations in the understanding of how Markov chains specifically apply to the simulation process, as well as potential ambiguities in the definitions of terms used in the discussion.

LagrangeEuler
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I do not understand where are Markov chains in Monte Carlo Ising simulation. Going randomly from lattice site to lattice site one flip one spin calculates energy and goes ahaid. But where are Markov chain there? Could you please explain me this. Thanks a lot.
 
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The lattice site after a flip has a probability distribution around the previous lattice site.
 
mathman said:
The lattice site after a flip has a probability distribution around the previous lattice site.
What do you mean by "probability distribution around the previous lattice site"?
 
The choice of the next lattice site is random. However it is defined in terms of a displacement from the current lattice site.
 
Thanks. Let me see if I understood you well. So you are now at site ##i## and you fliping spin at that moment. Probablility that after fliping spin will stay in that position depends only of that current position of all spins at the lattice and not of the path that we did before it. Lattice does not remember which spins are moved earlier.
 
LagrangeEuler said:
Thanks. Let me see if I understood you well. So you are now at site ##i## and you fliping spin at that moment. Probablility that after fliping spin will stay in that position depends only of that current position of all spins at the lattice and not of the path that we did before it. Lattice does not remember which spins are moved earlier.
Correct!
 

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