The specific heat per spin is calculated according to the
fluctuation-dissipation theorem:
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Equation 1. fluctuation-dissipation theorem |
Where T is the temperature at a given point, Kb is the Boltzmann’s constant and (ΔE)^2 is the total energy variance and can be
calculated as follows:
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Equation 2. total energy variance |
Where < E >^2 is the average energy level and < E^2 > is the average squared energy level:
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Figure 1. Specific heat simulated |
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Figure 2. Specific heat computational physics by Giordano (Fig 8.10) [1] |
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