G25.2651: Statistical Mechanics
Final Exam
Instructions: This is a take-home exam, hence lecture notes are permitted, however, books, journal articles, etc. are not! Partial credit will be given, so be sure to show ALL your work. The exam is due Monday, May 8.
where c is the speed of light and
is called the vector potential.
is related to the
magnetic field
by
One possible choice for
is
Hint: Show that the Schrödinger equation
is separable and derive the single-particle wave equation. Try a solution
to the single-particle equation of the form
and show that
satisfies a harmonic oscillator equation
with frequency
and equilibrium position
.
Assume L is much larger than the range of
.
where
is the average induced magnetization per unit volume
along the direction of the magnetic field and is given by
Calculate
and
for this system. Curie's Law for the
magnetic susceptibility states that
. Is your
result in accordance with Curie's Law? If not, explain why it should not be.
Hint: Consider using the canonical ensemble in this case.
write down the perturbation Hamiltonian
.
Hint: Consider using a convergence factor,
,
and let
to go 0 at the end of the calculation.
Consider a RG transformation, called the pair cell transformation,
in which
is re-expressed as
The transfer matrix is redefined by
. Find
the RG equation corresponding to this transformation and show that it leads
to the expected stable fixed point.
Hint: Try redefining the coupling constant by
and show that
can be put in the same form as
, i.e.,
and that c can be defined
implicitly in terms of u'.
Suppose that M;SPMgt;;SPMgt;m so that the motion of the y particle is very slow compared to x and that the temperature is high enough that spin statistics can be neglected. Under such conditions, it is reasonable to apply the ideas underlying the usual Born-Oppenheimer approximation to derive a path integral expression for the canonical partition function of the system. Such a situation arises in molecular systems with heavy nuclei and light electrons.
where S[x,y] is the Euclidean action functional, show that the partition function can be expressed exactly in the form
where
is the free Euclidean action integral for the y-particle:
and where
is the partition function of the x-particle computed along
a given path
of the y-particle. Provide a path integral
expression for
.
at a fixed value of y.
For use in the path integral, the eigenvalues
need to
be computed along a given path,
of the y-particle, which means
that the eigenvalues become functionals,
, of this path.
Use the idea of the Born-Oppenheimer approximation to explain why
these functionals can be approximately expressed as simple imaginary time averages
of
and provide, therefore, expressions for
and
within this approximation.
for all possible values of y. Write down an approximate expression for
in this case and give a physical interpretation of your expression.