Physics 573: Problem set 6
-
What are the orbital, spin, and total angular momentum values for
3dV? What is the Landé g factor? What is the
magnetic dipole moment?
-
A certain monatomic material has spin-split levels separated by
Δ. Calculate the partiction function, Z and the
internal energy E at
temperature T. Now calculate the heat
capacity C =
(∂E/∂T).
Plot this function to see how behaves near where Δ =
kBT. The name for these bumps in response functions
is Schottky anomaly. If Δ is induced by an external
magnetic field H discuss the changes in C(H).
If the splitting is small and arises from an ionic or crystal field
(such as hyperfine interactions) how does C depend on
temperature?
- An even richer version of the above problem obtains when the values
of Δ are distributed randomly throughout the crystal as
happens in glasses. A tractable version of this problem might have a
flat distribution of Δ between 0 and
Δmax. Start with states at energies
+Δ and -Δ, and recalculate E and
C. Now show that C(T) ∝ T for very low
temperature T <<
Δmax/kB
- A simple model for an antiferromagnet is a long row of spins where
next nearest neighbors are aligned parallel and neighbors are
antiparallel. That is there are two interleaved ferromagnetic
sublattices. The field on sublattice a is
Ba = Bext -
μ1Ma -
μ2Mb
and the effective field on sublattice b is
Bb = Bext -
μ1Mb -
μ2Ma.
Show that the Néel temperature is
[(μ2 - μ1)/
(μ1 + μ2)]θ,
where θ is the effective temperature offset for the
Curie-Weiss "law."
- A superconducting plate is aligned perpendicular to the z
axis. There is a constant magnetic field in the space near the plate
that lies parallel to the plate (e.g. along the x
axis). Obtain B(z) near the surface inside the
superconductor. Obtain the magnetization.
Describe the magnetization if the plate's thickness d is small
compared to the penetration depth. This is slightly less annoying if
you set the middle of the plate at z = 0.
The magnetization in the plate contribute extra free energy even at
T = 0. Average the magnetization across the thickness of
the plate and estimate the critical field. You should find that the
critical field for a very thin plate can be very different from the
bulk value.
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