Abstract:Abstract:The results of the femtosecond four-wave mixing measurements performed on the CdS crystal at room temperature are reported. The dephasing time T d = 180 fs was obtained. The anti-Stokes shift of the primary photon echo spectrum with respect to the excitation spectrum was observed. The some peculiarities of the coherent responses decay curves indicate that this optical dephasing is due to the exciton-exciton interaction. The stimulated photon echo decay curves appear to have a fast decay component (the… Show more
A new method of two-photon excitation of femtosecond signals of "entangled" free induction decay (EFID) by two crossed 790-nm laser beams in a CdS crystal at room temperature has been realized for the first time. This "entangled" (through the wave vectors) coherent response appears only in the case when the photons involved to the process of twophoton excitation of the sample belong to the different laser beams. This technique allows one to separate the EFID signal from the exciting femtosecond pulses and to vary the response wavelength by varying the angle between their wave vectors. The most optimal case occurs when the angle between the wave vectors of exciting pulses as well as the angle between each of these wave vectors and that of the response is equal to 60 • .
A new method of two-photon excitation of femtosecond signals of "entangled" free induction decay (EFID) by two crossed 790-nm laser beams in a CdS crystal at room temperature has been realized for the first time. This "entangled" (through the wave vectors) coherent response appears only in the case when the photons involved to the process of twophoton excitation of the sample belong to the different laser beams. This technique allows one to separate the EFID signal from the exciting femtosecond pulses and to vary the response wavelength by varying the angle between their wave vectors. The most optimal case occurs when the angle between the wave vectors of exciting pulses as well as the angle between each of these wave vectors and that of the response is equal to 60 • .
“…Let us now consider the physics of FCPE signals formation in the CdS crystal. It is based on the two-photon character of absorption of the 793 nm femtosecond Ti:sapphire laser radiation that was experimentally shown earlier by other authors in [4,5] and also in our work [6]. The excitation is carried out simultaneously by two laser beams crossed (in the same region of CdS film) at an angle of 60° propagating in the directions of wave vectors k 1 and k 2 .…”
“…The experiment was performed using degenerate fourwave mixing (DFWM) technique in CdS crystal in a temperature range from 5 to 300 K [4]. We also carried out a similar experiment in 2009 [6]. A scheme of the femtosecond photon echo excitation and detection in this mode is shown in figure 2.…”
We consider the possibility of observing a femtosecond correlated photon echo (FCPE) under two-photon excitation of CdS crystal by two pairs of crossed laser beams. The peculiarities of FCPE signals and their possible applications are discussed.
“…Earlier, in [12], it was shown that the two-photon regime is necessary for the resonant excitation of the CdS crystal by 800 nm laser radiation of the Ti:sapphire laser. Then, following [7], we experimentally show that in the case of CdS nanopowder one needs the three-photon regime of excitation [13]. In the experiment study in [3] it was shown that the semiconductor nanoparticles CdSe-CdS, known as nanostructures of 'core-shell' type, can play the role of such a nanopowder.…”
Section: Peculiarities Of the Ensemble Of Cdse-cds Quantum Dotsmentioning
The possibility and conditions of the correlated signals of stimulated photon echo (SPE) generation under three-photon femtosecond excitation of a sample, which is an ensemble of N semiconductor nanoparticles, are investigated. Each of these nonoparticles consists of a CdSe core covered by a CdS shell. The phase matching conditions for correlated SPE signal formation in such a sample are obtained.
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