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G25.2651: Statistical Mechanics

Problem set #5

Due: April 7, 2003

1.
The energy of a particle with magnetic moment tex2html_wrap_inline119 interacting with a magnetic field tex2html_wrap_inline121 is tex2html_wrap_inline123 . Consider an electron fixed in space interacting with a magnetic field in the z direction, so that tex2html_wrap_inline127 . The electron has a spin of 1/2, and its magnetic moment can be related to its spin tex2html_wrap_inline131 by tex2html_wrap_inline133 so that the Hamiltonian for the electron becomes

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The spin operator tex2html_wrap_inline135 where tex2html_wrap_inline137 is the spin gyromagnetic ration and tex2html_wrap_inline139 , tex2html_wrap_inline141 , and tex2html_wrap_inline143 are the Pauli matrices given by

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a.
Suppose an ensemble of such systems is prepared such that the density matrix initially is

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Calculate tex2html_wrap_inline145 .

b.
What are the expectation values of the operators tex2html_wrap_inline147 , tex2html_wrap_inline149 and tex2html_wrap_inline151 at any time t?
c.
Suppose now that the initial density matrix is

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For this case, calculate tex2html_wrap_inline145 .

d.
What are the expectation values of the operators tex2html_wrap_inline147 , tex2html_wrap_inline149 and tex2html_wrap_inline151 at time t for this case?
e.
What are the fluctuations in tex2html_wrap_inline147 ? Recall that

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f.
Suppose that the density matrix is given initially by a canonical density matrix:

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What is tex2html_wrap_inline145 ?

g.
What are the expectation values of tex2html_wrap_inline147 , tex2html_wrap_inline149 and tex2html_wrap_inline151 ?

2.
A simple two-state system with energies tex2html_wrap_inline175 and tex2html_wrap_inline177 is described by a Hamiltonian

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where tex2html_wrap_inline179 , tex2html_wrap_inline181 , and I is the identity operator. Suppose this system has an electric dipole moment tex2html_wrap_inline119 and is subject to a laser of frequency tex2html_wrap_inline187 with electric field component tex2html_wrap_inline189 such that the total Hamiltonian is

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Solve the Liouville equation for the density matrix of an ensemble of such systems and calculate the expectation value of tex2html_wrap_inline191 in this ensemble.

3.
Consider a one-dimensional free particle in a ``box'' of length L. The Hamiltonian for the system is

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a.
Write down a path integral expression for the canonical density matrix tex2html_wrap_inline195 as the limit tex2html_wrap_inline197 of a P-dimensional integral.

b.
By making the change of variables in the interal,

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which is defined recursively in terms of tex2html_wrap_inline201 , calculate the density matrix and the partition function tex2html_wrap_inline203 for a this system.

c.
Perform the Wick rotation and find an expression for the real-time quantum propagator U(x,x';t).

4.
The partition function for a 2-particle system in one dimension with boson exchange statistics is

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Derive a discrete (finite P) path integral expression for the exchange term tex2html_wrap_inline209 for the case that

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and give an intepretation of your result in terms of a classical mechanical model with points and springs.




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Mark Tuckerman
Sun Mar 30 22:46:20 EST 2003