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where <math>k_B</math> is the [[Boltzmann constant]], <math>T</math> is [[temperature]] and  <math>E(q)</math> is [[energy]] of state  <math>q</math>. Furthermore, the probability of a given state, <math>q</math>, occurring is given by
 
where <math>k_B</math> is the [[Boltzmann constant]], <math>T</math> is [[temperature]] and  <math>E(q)</math> is [[energy]] of state  <math>q</math>. Furthermore, the probability of a given state, <math>q</math>, occurring is given by
   −
where <math>k_B</math> is the Boltzmann constant, <math>T</math> is temperature and  <math>E(q)</math> is energy of state  <math>q</math>. Furthermore, the probability of a given state, <math>q</math>, occurring is given by
      
其中<math>k_B</math>是玻尔兹曼常数,<math>T</math> 是温度,<math>E(q)</math> 是状态<math>q</math>的能量。此外,给定状态 <math>q</math>出现的概率是
 
其中<math>k_B</math>是玻尔兹曼常数,<math>T</math> 是温度,<math>E(q)</math> 是状态<math>q</math>的能量。此外,给定状态 <math>q</math>出现的概率是
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