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[tex]\hat H = \frac{{{\hbar ^2}}}{{2m}}\frac{{{\partial ^2}}}{{\partial {x^2}}} + \frac{1}{2}m{\omega ^2}{x^2}[/tex]

with the trace given as

[tex]\int\limits_{ - \infty }^\infty {\left\langle x \right|\exp \left( { - \beta \hat H} \right)\left| x \right\rangle } = \frac{{\exp \left( { - 0.5\beta \hbar \omega } \right)}}{{1 - \exp \left( { - 0.5\beta \hbar \omega } \right)}}[/tex].

Beta is representing inverse temperature. From the mean energy in terms of the trace we get

[tex]\left\langle H \right\rangle = - \frac{\partial }{{\partial \beta }}\ln \sum\limits_x {\left\langle x \right|\exp \left( { - \beta \hat H} \right)\left| x \right\rangle } [/tex],

which finally amounts to

[tex]\left\langle H \right\rangle = \frac{1}{2}\hbar \omega \coth \left( {\frac{1}{2}\beta \hbar \omega } \right)[/tex].

My next step is to expand my program to 3 dimensions. I know that the energy of the classical harmonic oscillator in 3D is simply the result from 1D times the degrees of freedom (3 translational, 2 rotational and 1 vibrational), but does this also hold for the Quantum version of the harmonic oscillator?

I.e. is

[tex]\left\langle {{H_{3D}}} \right\rangle = 3\hbar \omega \coth \left( {\frac{1}{2}\beta \hbar \omega } \right)[/tex]

true?

Thanks in advance!