Bulk two-dimensional electron systems in a strong perpendicular
magnetic field exhibit the fascinating phenomenon of fractional
quantum Hall effect. Composite fermion theory was developed in the
process of understanding the fractional quantum Hall effect and was
proven to work successfully for the FQHE and even beyond. In this
dissertation, we explore the effect of the strong correlation
between electrons in several cases. All of them belong to the
category of 2DES in strong perpendicular magnetic field and they are
listed below:
(i)A fractional quantum Hall island surrounded by a bulk fractional
quantum Hall state with a different filling factor. Specifically, we
study the resonant tunneling composite fermions through their
quasibound states around the island. A rich set of possible
transitions are found and the possible relevance to an interesting
experiment is discussed. Also, we discuss the subtlety of separating
the effect of fractional braiding statistics from other factors.
(ii) Correlated states of a quantum dot, at high magnetic fields,
assuming four electrons with two components. Such a dot can be
realized by reducing the two lateral dimensions of a 2DES
tremendously. Both the liquid states and crystallites (the latter
occurring at large angular momenta) of four electrons in terms of
composite fermions are considered. Residual interaction between
composite fermions is shown to leads to complex spin correlations.
(iii) Bilayer quantum Hall effect at total filling $
u_T=5$.
This can accommodate an excitonic superfluid state at small layer
separations just like at $
u_T=1$. At large layer separations, however, $
u_T=5$ state evolves into
uncorrelated $
u=5/2$ fractional quantum Hall states in both
layers, in contrast to uncorrelated composite Fermi sea in $
u_T=1$ case. We focus on finding the critical layer separation at
which the correlation between electrons on different layers are
destroyed. Effects due to the finite width of the layers are also
considered.