Abstract:We fabricate and study quantum dot structures incorporating quasi-one-dimensional excited states. The structures are realized by graded bandgap GaAs/AlGaAs quantum wires self-formed inside inverted tetrahedral pyramids. The ground state transitions exhibit typical characteristics of fully confined excitons, including single photon emission. Efficient carrier thermalization and relaxation, as well as correlated photon emission is observed also among the excited states, indicating the formation of quasi-one-dime… Show more
“…It is likely to have arisen because of the production of multiexciton per single photon upon excitation of PbSe in ZnSP1 at higher energies (2.755 eV) greater than the bandgap energy (0.278 eV) as shown below in eq . This aspect has earlier been demonstrated in IV– VI semiconductors by a number of workers. − Moreover, multiple exciton generation with higher charge carrier densities may create higher-energy states, which might transfer energy to the adsorbed dye, NB having higher standard redox potential (−0.12), before they could annihilate (eq ). The excited NB then emits at higher energy (670 nm; 1.85 eV) than that of PbSe (806 nm; 1.53 eV).Zn2+/(PbSe)n→hvZn2+/(PbSe)n(e−−h+)xZn2+/false(PbSefalse)italicnfalse(normale−−normalh+false)italicy+NB→Zn2+/false(PbSefalse)italicn+NB*where n is the agglomeration number, x > 1, and y > x .…”
Section: Discussionmentioning
confidence: 83%
“…This aspect has earlier been demonstrated in IV− VI semiconductors by a number of workers. 24−26 Moreover, multiple exciton generation with higher charge carrier densities may create higher-energy states, 27 which might transfer energy to the adsorbed dye, NB having higher standard redox potential (−0.12), 28 before they could annihilate (eq ii). The excited NB then emits at higher energy (670 nm; 1.85 eV) than that of PbSe (806 nm; 1.53 eV).…”
This paper reports the effect of the addition of varied concentrations of Zn 2+ on the photophysical properties of RNA-mediated PbSe nanostructures. An increasing addition of Zn 2+ results in diminishing of the excitonic feature in the optical spectrum associated with a decrease in red emission with a simultaneous increase in the near-infrared (NIR) region up to 10 × 10 −5 mol dm −3 . It causes the emission lifetime to decrease from 255 to 208 ns at 770 nm and increase from 10.4 to 17.6 ns at 1000 nm. The addition of Zn 2+ changes the nature of Q-PbSe from direct to indirect band gap semiconductor by creating different surface states within its band gap, inducing additional transitions. It is understood to facilitate the phonon-assisted relaxation populating the deeper traps responsible for enhanced NIR fluorescence. The adsorption capacity of aged Zn 2+/ PbSe is enhanced for Nile blue (NB) as compared to its fresh samples due to increased porosity. The excitation of PbSe with energy greater than the bandgap energy in NB-supported PbSe nanostructures results in an energy transfer from excited PbSe to NB involving multiple exciton generation per photon. The porosity, enhanced adsorption capacity with fairly high emission yield, and lifetime in the NIR region give Zn 2+/ PbSe significant potential as a synthesized nanosystem for tissue and bioimaging applications.
“…It is likely to have arisen because of the production of multiexciton per single photon upon excitation of PbSe in ZnSP1 at higher energies (2.755 eV) greater than the bandgap energy (0.278 eV) as shown below in eq . This aspect has earlier been demonstrated in IV– VI semiconductors by a number of workers. − Moreover, multiple exciton generation with higher charge carrier densities may create higher-energy states, which might transfer energy to the adsorbed dye, NB having higher standard redox potential (−0.12), before they could annihilate (eq ). The excited NB then emits at higher energy (670 nm; 1.85 eV) than that of PbSe (806 nm; 1.53 eV).Zn2+/(PbSe)n→hvZn2+/(PbSe)n(e−−h+)xZn2+/false(PbSefalse)italicnfalse(normale−−normalh+false)italicy+NB→Zn2+/false(PbSefalse)italicn+NB*where n is the agglomeration number, x > 1, and y > x .…”
Section: Discussionmentioning
confidence: 83%
“…This aspect has earlier been demonstrated in IV− VI semiconductors by a number of workers. 24−26 Moreover, multiple exciton generation with higher charge carrier densities may create higher-energy states, 27 which might transfer energy to the adsorbed dye, NB having higher standard redox potential (−0.12), 28 before they could annihilate (eq ii). The excited NB then emits at higher energy (670 nm; 1.85 eV) than that of PbSe (806 nm; 1.53 eV).…”
This paper reports the effect of the addition of varied concentrations of Zn 2+ on the photophysical properties of RNA-mediated PbSe nanostructures. An increasing addition of Zn 2+ results in diminishing of the excitonic feature in the optical spectrum associated with a decrease in red emission with a simultaneous increase in the near-infrared (NIR) region up to 10 × 10 −5 mol dm −3 . It causes the emission lifetime to decrease from 255 to 208 ns at 770 nm and increase from 10.4 to 17.6 ns at 1000 nm. The addition of Zn 2+ changes the nature of Q-PbSe from direct to indirect band gap semiconductor by creating different surface states within its band gap, inducing additional transitions. It is understood to facilitate the phonon-assisted relaxation populating the deeper traps responsible for enhanced NIR fluorescence. The adsorption capacity of aged Zn 2+/ PbSe is enhanced for Nile blue (NB) as compared to its fresh samples due to increased porosity. The excitation of PbSe with energy greater than the bandgap energy in NB-supported PbSe nanostructures results in an energy transfer from excited PbSe to NB involving multiple exciton generation per photon. The porosity, enhanced adsorption capacity with fairly high emission yield, and lifetime in the NIR region give Zn 2+/ PbSe significant potential as a synthesized nanosystem for tissue and bioimaging applications.
Quantum dots (QDs) are very attractive nanostructures from an application point of view due to their unique optical properties. Optical properties and valence band (VB) state character was numerically investigated with respect to the effects of nanostructure geometry and composition. Numerical simulation was carried out using the Luttinger–Kohn model adapted to the particular case of QDs in inverted pyramids. We present the source code of the 4-band Luttinger–Kohn model that can be used to model AlGaAs or InGaAs nanostructures. The work focuses on the optical properties of GaAs/AlGaAs [111] QDs and quantum dot molecules (QDMs). We examine the dependence of Ground State (GS) optical properties on the structural parameters and predict optimal parameters of the QD/QDM systems to achieve dynamic control of GS polarization by an applied electric field.
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