APS March Meeting 2010
Volume 55, Number 2
Monday–Friday, March 15–19, 2010;
Portland, Oregon
Session Y2: Composite Fermions: Recent Advances in States and Excitations
8:00 AM–11:00 AM,
Friday, March 19, 2010
Room: Oregon Ballroom 202
Sponsoring
Units:
DCMP APS
Chair: Vito Scarola, Virginia Polytechnic Institute and State University
Abstract ID: BAPS.2010.MAR.Y2.2
Abstract: Y2.00002 : Collective Excitations of Composite Fermions Across Multiple $\Lambda$ Levels*
8:36 AM–9:12 AM
Preview Abstract
Abstract
Author:
Sudhansu Mandal
(Indian Association for the Cultivation of science, Kolkata 700032, India)
The collective behavior of electrons in the fractional quantum
Hall states results in the creation of so-called composite
fermions, quasi-particles formed by electrons attached to an even
number of quantized vortices, each having one unit of flux
quantum $hc/e$. This leads to formation of $\Lambda$
levels--effective kinetic energy levels resembling Landau levels
for such quasi-particles. The composite fermion (CF) theory
predicts collective excitations corresponding to an excitation of
CF from $\Lambda =0$ level to $\Lambda =1$ level at filling
factor $\nu =1/3$, with a roton minimum. A similar mode
of collective excitations is also predicted in a theory based on
single mode approximation (SMA) in which the excited state is the
density wave modulation over the ground state. This collective
mode is detected by Raman scattering and other
experiments. More recently, however, Hirjibehedin {\em et.
al.}\footnote{C.F.Hirjibehedin {\em et. al.}, Phys. Rev. Lett.
{\bf 95}, 066803 (2005).} have discovered that this mode is not a
single mode, as believed earlier, but splits into two as the
wavevector is increased. By definition, the SMA cannot
accommodate a doublet. We show that the observed new mode finds a
natural explanation within the CF theory. We
consider\footnote{D.Majumder, S.S.Mandal, and J.K.Jain, Nature
Physics {\bf 5}, 403 (2009).} excitations of CF from $\Lambda =0$
level to $\Lambda =2$ and 3 levels, apart from
$\Lambda =1$ level that had only been considered before for the
lowest mode. By extensive numerical calculation for 200
particles, we find that these three modes of excitations tend
to come closer at small wavevectors, the highest mode merges
first with the middle mode as we decrease wavevector and finally
the middle mode merges with the lowest mode at a very small
wavevector in the thermodynamic limit. We attribute this merging
at longwavelength to $100\%$ overlap between these three excited
states. The observed gap between the two modes is comparable with
the theoretical estimation. Further, the prediction of new roton
minima in higher modes of excitations are also confirmed
in a recent experiment.\footnote{T.David {\em et al.}, (in
preparation).} Similar study for $\nu=2/5$ state
will also be discussed and will be compared with the recent
experiment.\footnote{Ibid.}
*I sincerely thank my collaborators D. Majumder and J. K. Jain. I thank also to my Institution for financial support.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2010.MAR.Y2.2