The specific heat per spin is calculated according to the
fluctuation-dissipation theorem:
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEjmXQ_OtoFktJLO6itiglCVa3NUb8THK6mAO1OkaIHr7Z-nrAcepXY5P6U4hWy0kxUlu8_5qJek_O0pvO86R_7avrqJy1afiBeh5W1IXzJwJJzDNyAzdb3fl-mLIl3zW9WzqMa4TfQJ_irp/s200/ex5.PNG) |
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:
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEhhoNx-mwky1o_EGuVeebHvwGoTC5SBDYQXPY0JhgGKhUDgJIcx57HwfFl5DzE9DFHY_PpiNwzKMPzOhmxeQQdRSRQCHs0f2hwSedErRmFdHKx_UCGBoSZEswvsl1jCLHW86pTlDLc3NOSC/s200/EQ5.PNG) |
Equation 2. total energy variance |
Where < E >^2 is the average energy level and < E^2 > is the average squared energy level:
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEg43k9DGxlQV08OAysGVKYnR0CfLTc5S085UXAsEvDQiqSZSQ5rM19T8q5S4Jl9K8Kmu8LKK7YX2a2WMQi97o_7n7Ol67rnXLBtevI1Bu47jHSQGuc4mYYKgqKhaFZk7vTRbR99TuldW-BM/s400/SPECHEAT.png) |
Figure 1. Specific heat simulated |
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEhF3zZnxU05i8ZNGfRxmhs0g_1325cKVkP-qkN7Xm0uUE6f8RgFBySBvIxXUgOMlZ5hEDjrfiy6m-nYe00TaB265sQmnYu0vEficzWpNkIlXzbDkeQmSW-TDD7CNJUvgBfxadWLAHzgDxAP/s400/SPECIFIC+HEAT.png) |
Figure 2. Specific heat computational physics by Giordano (Fig 8.10) [1] |
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