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Chemical Physics Letters

Interference between femtosecond pulses observed via time-resolved spontaneous fluorescence

Aleksander K. Rebane, Christophe Sigel, Mikhail A. Drobizhev

Published May 1, 2000• 9 citations
Publisher
DOI
10.1016/s0009-2614(00)00427-9

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We show how two identical laser pulses (with a controlled delay time) can be used to create a coherent superposition of two vibrational wave packets in a bound electronic state, which exhibit the following features as a function of the delay time between the laser pulses: high frequency oscillation (at the Bohr frequency) modulated by a slow envelope corresponding to the vibrational recurrences. We present a theoretical treatment of this effect and experimental results obtained in Cs2, with 160 fs, 768 nm laser pulses, in which the high frequency modulation is resolved, with a beat period of 2.6 fs1. Finally, we show how the detection scheme can affect the observability of these interferences when only two laser pulses are used: at 758 nm the interference fringes cannot be observed.

AIP conference proceedings•Jan 1, 1996•0 citations
We show that the coherence time and the pulse envelope of ultrashort fluorescence can be measured with two-photon interference. We have performed these measurements in a solution of Nile Blue in N,N-dimethylaniline in the femtosecond regime. The coherence time and the envelope contribute two components to a dip in the coincidence count rate. We have verified that these components can be measured separately at will. This technique provides the means to measure the pulse envelope of ultrashort pulses over a wide range of wavelengths and intensities.
Spontaneous fluorescence has been used to measure the coherent femtosecond response of the organic, binary crystal pentacene/p-terphenyl. By using two-pulse excitation with phase-randomized pulses in an interferometric setup and analyzing the variance of the fluctuating intensity of correlated fluorescence photons, femtosecond beatings have been observed. The pattern of these terahertz oscillations is strongly dependent on the detuning frequency range of the exciting pulses, but is rather invariant with regard to the spectral position of the fluorescence probe window. In the interferometric regime of freely propagating pulses novel, ultrafast fluorescence carrier-wave oscillations superimposed to the beat structure have been obtained. The oscillatory signals evolve from a coherent superposition of optical free induction decays, caused by the different electronic transition energies of the pentacene absorber sites O1, O2, O3, and O4, respectively, are monitored as intrinsic, heterodyne beats by the fluorescence square detector. The major part of oscillations is thus considered to result from typical polarization interferences, but vibrational quantum beats are also extractable from the interferogram in the ultimate frequency regime of the pentacene S0→S1ν=1, S0→S1ν=2 resonances. The early picosecond-decay of the fluorescence beats reveals the mechanism of the loss of coherence to be mainly controlled by inhomogeneous dephasing at low phonon temperatures. A model of uncoupled two-level systems that includes Gaussian inhomogeneous broadening of the individual absorber sites and a Gaussian frequency distribution for the excitation pulses can account for the experimental data, quite adequately.
We show how two identical laser pulses (with a controlled delay time) can be used to create a coherent superposition of two vibrational wave packets in a bound electronic state, which exhibit the following features as a function of the delay time between the laser pulses: high frequency oscillation (at the Bohr frequency) modulated by a slow envelope corresponding to the vibrational recurrences. We present a theoretical treatment of this effect and experimental results obtained in Cs2, with 160 fs, 768 nm laser pulses, in which the high frequency modulation is resolved, with a beat period of 2.6 fs1. Finally, we show how the detection scheme can affect the observability of these interferences when only two laser pulses are used: at 758 nm the interference fringes cannot be observed.