1990
DOI: 10.1103/physrevlett.65.1340
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Effects of coherent polarization interactions on time-resolved degenerate four-wave mixing

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Cited by 279 publications
(122 citation statements)
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“…The first and most prominent was a signal for the ''wrong'' time delay in a two-pulse TFWM experiment. Theoretically, such signals could arise from several effects including local fields (3,4), biexcitons (5), excitation-induced dephasing (6, 7), or excitation-induced shift (8). Time resolving the signal also provided evidence for many-body contributions (9,10), although it did not resolve the ambiguity regarding the underlying phenomena.…”
mentioning
confidence: 99%
“…The first and most prominent was a signal for the ''wrong'' time delay in a two-pulse TFWM experiment. Theoretically, such signals could arise from several effects including local fields (3,4), biexcitons (5), excitation-induced dephasing (6, 7), or excitation-induced shift (8). Time resolving the signal also provided evidence for many-body contributions (9,10), although it did not resolve the ambiguity regarding the underlying phenomena.…”
mentioning
confidence: 99%
“…Phase-coherent nonlinear spectroscopic measurements such as four-wave-mixing are sensitive to the changes that occur when excitons interact through Coulomb forces [5] or local fields [6]. Early nonlinear 'self-diffraction' measurements revealed a signal at 'negative' delays due to many-body interactions (MBIs) [6][7][8], but since the exciton coherence frequencies could not be correlated with the emitted coherence frequencies, the contributions due to MBIs such as excitationinduced dephasing (EID) [9], excitation-induced energy shift (EIS) [10], and local field effects (LFEs) [6] could not be distinguished. EID and EIS result in density-dependent collisional broadening and renormalization of the exciton energy, respectively.…”
mentioning
confidence: 99%
“…In conclusion we have demonstrated that our theoretical approach is able to describe the microscopic dynamics of laser-excited semiconductors quantitatively for all excitation densities at the (3) level. This is achieved by accounting on the same footing for two important effects: ͑i͒ scattering with free carriers as the most effective dephasing process and ͑ii͒ screening of the Coulomb interaction that controls correlation effects.…”
Section: Discussionmentioning
confidence: 98%
“…Indeed it is now possible to perform experiments with time resolution shorter than the scattering time scales of the fundamental elementary excitations and with interferometric control of the excitation density and energy. 1,2 However, most of the work, experimental or theoretical, concentrates on either one of two completely different experimental situations, involving, respectively, coherently driven states [3][4][5][6][7] or incoherently relaxing distributions. [8][9][10][11][12][13][14] In real life this distinction is artificial since an initially coherently driven system naturally relaxes and eventually reaches thermodynamic equilibrium.…”
Section: Introductionmentioning
confidence: 99%
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