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How to probe a fractionally charged quasihole?
We report an anomalous dispersion of charged excitons in photoluminescence experiments on a two-dimensional electron gas subjected to a quantizing magnetic field around ν= 1 3 . We have found that the anomaly exists only at a very low temperature (0.1 K) and an intermediate electron density (0.9×10...
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Published in: | Physica. E, Low-dimensional systems & nanostructures Low-dimensional systems & nanostructures, 2004-04, Vol.22 (1), p.131-134, Article 131 |
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Main Authors: | , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We report an anomalous dispersion of charged excitons in photoluminescence experiments on a two-dimensional electron gas subjected to a quantizing magnetic field around
ν=
1
3
. We have found that the anomaly exists only at a very low temperature
(0.1
K)
and an intermediate electron density
(0.9×10
11
cm
−2)
. It is explained to occur due to the perturbation of the incompressible liquid at
ν=
1
3
. The perturbation is induced by the close proximity of a localized charged exciton which creates a fractionally charged quasihole in the liquid. The intriguing experimentally observed puzzle that the anomaly can be destroyed by applying a small thermal energy of
∼0.2
meV
is thereby resolved, as this energy is enough to close the quasihole energy gap. This work presents a probe of the quasihole gap in a quantum Hall system. |
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ISSN: | 1386-9477 1873-1759 |
DOI: | 10.1016/j.physe.2003.11.233 |