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Suppose the density matrix $\rho$ with eigenvalues $k_{i}$.

Now consider the density matrix $\rho$ in a thermal equilibrium with temperature $T$. Let's show the density matrix with $\rho(T)$ in this case.

What are the eigenvalues of $\rho(T)$?

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Thermal equilibrium Gibbs state is usually defined as $$\rho = \frac{1}{Z} e^{-\beta H} = \frac{1}{Z} \text{diag}(e^{-\beta E_0}, e^{-\beta E_1} \cdots)\,, $$ where $\beta$ is the inverse temperature defined as $$ \beta = \frac{1}{K_B T}\,,$$

And $Z$ is the partition function $$ Z = \sum_i e^{-\beta E_i} \,.$$

So, the eigenvalues $\{ \lambda_i \}$ are $$ \lambda_i = \frac{e^{-\beta E_i}}{Z}\,. $$

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  • $\begingroup$ How does this recover: $\rho=\mathrm{diag}(E_i)$ for $T\to 0$? Or it should not? $\endgroup$
    – Mauricio
    Commented Feb 1 at 20:42

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