1-dimensional Ising model: Difference between revisions

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m (New page: Model: Consider a system with <math> N </math> spins in a row. The energy of the system will be given by <math> U = -K \sum_{i=1}^{N-1} S_{i} S_{i+1} </math>, where each variable <mat...)
 
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The energy of the system will be given by
The energy of the system will be given by


<math> U = -K \sum_{i=1}^{N-1} S_{i} S_{i+1} </math>,  
<math> U = -J \sum_{i=1}^{N-1} S_{i} S_{i+1} </math>,  


where each variable <math> S_j </math> can be either -1 or +1.
where each variable <math> S_j </math> can be either -1 or +1.
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The partition function of the system will be:
The partition function of the system will be:


<math> Q_N = \sum_{\Omega^N }  \exp \left[ - K \sum_{i=1}^{N-1} S_i S_{i+1}  \right]</math>,  
<math> Q_N = \sum_{\Omega^N }  \exp \left[ K \sum_{i=1}^{N-1} S_i S_{i+1}  \right]</math>,  


where <math> \Omega^N </math> represents the possible configuration of the N ''spins'' of the system.
 
where <math> \Omega^N </math> represents the possible configuration of the N ''spins'' of the system,
and <math> K = J/k_B T </math>


to be continued ...
to be continued ...

Revision as of 12:22, 23 February 2007

Model: Consider a system with spins in a row.

The energy of the system will be given by

,

where each variable can be either -1 or +1.

The partition function of the system will be:

,


where represents the possible configuration of the N spins of the system, and

to be continued ...