Homework Set 1: Difference between revisions

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For one-dimensional harmonic oscillator, the expectation value of the number operator at finite temperature <math> T </math> is given by  
For one-dimensional harmonic oscillator, the expectation value of the number operator at finite temperature <math> T </math> is given by  


\langle \hat{a}^\dagger \hat{a} \rangle = \frac{1}{e^{\beta \hbar \omega} - 1},
<math> \langle \hat{a}^\dagger \hat{a} \rangle = \frac{1}{e^{\beta \hbar \omega} - 1} </math>


where \beta=1/(k_B T).  
where \beta=1/(k_B T).  
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\frac{1}{2}\langle \{\hat{x}(t),\hat{x}(0) \} \rangle  
<math> \frac{1}{2}\langle \{\hat{x}(t),\hat{x}(0) \} \rangle </math>




and give physical interpretation of its first and second term.
and give physical interpretation of its first and second term. Here <math> \{\hat{A},\hat{B}\} </math> is antucommutator of two operators.


'''(b)''' What happens to the autocorrelation function in the high temperature limit?
'''(b)''' What happens to the autocorrelation function in the high temperature limit?

Revision as of 22:06, 9 September 2019

Problem 1: Three-dimensional isotropic harmonic oscillator

Problem 2: Autocorrelation function of harmonic oscillator at finite temperature

For one-dimensional harmonic oscillator, the expectation value of the number operator at finite temperature T is given by

a^a^=1eβω1

where \beta=1/(k_B T).

(a) Compute the autocorrelation function of the position operator


12{x^(t),x^(0)}


and give physical interpretation of its first and second term. Here {A^,B^} is antucommutator of two operators.

(b) What happens to the autocorrelation function in the high temperature limit?

Problem 3: Coordinate representation of coherent state

Problem 4: Phonons in one-dimensional chain with two different atoms per unit cell

Consider an infinite one-dimensional chain described by classical Hamiltonian:

H=j[pj22mj+k2(xjxj1)2]

whose even sites host atoms of mass m2j=m and odd sites host atoms of mass m2j+1=M.

(a) Find classical normal mode frequencies and sketch their dispersion curves ω(k).

(b) What is the gap in the excitation spectrum?

(c) Write the diagonalized Hamiltonian in second quantized form and discuss how you might arrive at your final answer. You will now need two types of creation operators.