325 research outputs found
Frequency-dependent spontaneous emission rate from CdSe and CdTe nanocrystals: influence of dark states
We studied the rate of spontaneous emission from colloidal CdSe and CdTe
nanocrystals at room temperature. The decay rate, obtained from luminescence
decay curves, increases with the emission frequency in a supra-linear way. This
dependence is explained by the thermal occupation of dark exciton states at
room temperature, giving rise to a strong attenuation of the rate of emission.
The supra-linear dependence is in agreement with the results of tight-binding
calculations.Comment: 11 page
Electronic states and optical properties of PbSe nanorods and nanowires
A theory of the electronic structure and excitonic absorption spectra of PbS
and PbSe nanowires and nanorods in the framework of a four-band effective mass
model is presented. Calculations conducted for PbSe show that dielectric
contrast dramatically strengthens the exciton binding in narrow nanowires and
nanorods. However, the self-interaction energies of the electron and hole
nearly cancel the Coulomb binding, and as a result the optical absorption
spectra are practically unaffected by the strong dielectric contrast between
PbSe and the surrounding medium. Measurements of the size-dependent absorption
spectra of colloidal PbSe nanorods are also presented. Using room-temperature
energy-band parameters extracted from the optical spectra of spherical PbSe
nanocrystals, the theory provides good quantitative agreement with the measured
spectra.Comment: 35 pages, 12 figure
Efficient electron spin manipulation in a quantum well by an in-plane electric field
Electron spins in a semiconductor quantum well couple to an electric field
{\it via} spin-orbit interaction. We show that the standard spin-orbit coupling
mechanisms can provide extraordinary efficient electron spin manipulation by an
in-plane ac electric field
Comment on "Self-Purification in Semiconductor Nanocrystals"
In a recent Letter [PRL 96, 226802 (2006)], Dalpian and Chelikowsky claimed
that formation energies of Mn impurities in CdSe nanocrystals increase as the
size of the nanocrystal decreases, and argued that this size dependence leads
to "self-purification" of small nanocrystals. They presented
density-functional-theory (DFT) calculations showing a strong size dependence
for Mn impurity formation energies, and proposed a general explanation. In this
Comment we show that several different DFT codes, pseudopotentials, and
exchange-correlation functionals give a markedly different result: We find no
such size dependence. More generally, we argue that formation energies are not
relevant to substitutional doping in most colloidally grown nanocrystals.Comment: 1 page, 1 figur
Single-particle states in spherical Si/SiO quantum dots
We calculate ground and excited electron and hole levels in spherical Si
quantum dots inside SiO in a multiband effective mass approximation.
Luttinger Hamiltonian is used for holes and the strong anisotropy of the
conduction electron effective mass in Si is taken into account. As boundary
conditions for electron and hole wave functions we use continuity of the wave
functions and the velocity density at the boundary of the quantum dots.Comment: 8 pages, 5 figure
Electron spin synchronization induced by optical nuclear magnetic resonance feedback
We predict a new physical mechanism explaining the electron spin precession
frequency focusing effect observed recently in singly charged quantum dots
exposed to a periodic train of resonant circularly polarized short optical
pulses [A. Greilich et al, Science 317, 1896 (2007), Ref. 1]. We show that
electron spin precession in an external magnetic field and a field of nuclei
creates a Knight field oscillating at the frequency of nuclear spin resonance.
This field drives the projection of the nuclear spin onto magnetic field to the
value that makes the electron spin precession frequency a multiple of the train
cyclic repetition frequency, which is the condition at which the Knight field
vanishes.Comment: 4+ pages, 3 figure
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