2017
DOI: 10.1039/c7nr01512g
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Ultrafast transient optical loss dynamics in exciton–plasmon nano-assemblies

Abstract: We study the exciton-plasmon dynamics that lead to optical loss mitigation via ultrafast transient absorption spectroscopy (UTAS) on hybrid aggregates of core-shell quantum dots (QDs) and Au nanoparticles (NPs). We highlight that generating hot electrons in plasmonic NPs contributes to the transient differential absorption spectrum under optical excitation. The results suggest modifying the method of analyzing the transient absorption spectra of loss mitigated systems. Additionally, we investigate the effect o… Show more

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Cited by 18 publications
(16 citation statements)
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“…The dependence of − ∆ 0 on pump power is consistent with the semiconductor to quasimetal transition to which Ge is subject under optical excitation, which gives rise to an increase in photoconductive free carriers. The relative change in the transmission exhibits a characteristic exponential decay: mono-exponential decay profile convolved with the instrument response function is fitted to the experimentally measured data points inFigure 3, using the following equation:49…”
mentioning
confidence: 99%
“…The dependence of − ∆ 0 on pump power is consistent with the semiconductor to quasimetal transition to which Ge is subject under optical excitation, which gives rise to an increase in photoconductive free carriers. The relative change in the transmission exhibits a characteristic exponential decay: mono-exponential decay profile convolved with the instrument response function is fitted to the experimentally measured data points inFigure 3, using the following equation:49…”
mentioning
confidence: 99%
“…The differential transmissions (−∆ E / E 0 ) of the terahertz pulse at various pump fluences are experimentally extracted and theoretically fitted. When the amorphous Ge is pumped by a laser beam at 800 nm, we can derive the lifetime of relaxation according to exponential decay function, which is expressed as follows [ 89 ] ΔE/E0=normale()tt0IRF/2ln22×A0+Aanormalett0τ1…”
Section: Resultsmentioning
confidence: 99%
“…The qualitative effect of weak versus strong coupling exists regardless of whether or not the pump affects other material properties of the system. For instance, an ultrashort optical pump can significantly affect the conductivity of the metallic parts, leading to additional pump-dependent changes, 26 whereas in an electrically pumped system (or in an optically pumped system with less intense but longer duration pump pulses), this effect would be absent. In any case, and regardless of the coupling level, the differential transmittance depends on the population difference Δ N (and therefore on the pump–probe delay δτ pp ), and since after excitation, the populations return to their ground state, Δ N tends to zero and similarly does Δ Τ / Τ , as shown in Figure 1.…”
Section: Pump–probe Experimentsmentioning
confidence: 99%
“…One obvious way of compensating for loss is to introduce gain materials into the metamaterial structure. [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26] This constitutes a promising solution, provided that we can achieve a sufficiently strong coupling between the gain material and the meta-atoms of the metamaterial, so that the resonance becomes loss compensated, that is, undamped.…”
Section: Introductionmentioning
confidence: 99%