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G25.2651: Statistical Mechanics

Problem set #6

Due April 14, 2003

1.
Consider two distinguishable particles in one dimension with respective coordinates x and y and conjugate momenta tex2html_wrap_inline65 and tex2html_wrap_inline67 with a Hamiltonian

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a.
Show that the density matrix tex2html_wrap_inline69 can be written in the form

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where T[x;y,y'] is known as the influence functional. What is the functional integral expression for T[x;y,y'], and of what function is T[x;y,y'] a functional?

b.
Give a closed form expression for tex2html_wrap_inline77 by evaluating the functional integral.

: Use the method of expansion about the classical path, and treat tex2html_wrap_inline79 as an arbitrary function of time, i.e. as a forcing function in the equation of motion for tex2html_wrap_inline81 .

2.
a.
Show that the path integral expression for the density matrix can be written as:

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b.
Consider a double well potential of the form

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Show that, for a particle of unit mass, the dominant path for the density matrix tex2html_wrap_inline83 is given by

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in the low temperature limit with negligible error in the endpoint conditions. This path is called an instanton or kink solution. Discuss the behavior of this trajectory in imaginary time tex2html_wrap_inline85 .

c.
Calculate the classical imaginary-time action for the kink solution.





Mark Tuckerman
Mon Apr 28 14:32:36 EDT 2003