2011
DOI: 10.1016/j.cplett.2011.10.013
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Perturbed free induction decay in ultrafast mid-IR pump–probe spectroscopy

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Cited by 26 publications
(26 citation statements)
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“…Figure 6a shows examples of the oscillatory signals we observe. The oscillations start at negative time delays when the probe pulse arrives at the sample before the excitation pulse, suggesting that the probe pulse generates a coherence that the excitation pulse interacts with, as observed in perturbed free-induction decays45565758. However, the periods of the oscillations we observe are insensitive to probe frequency or pump pulse intensity, which is in stark contrast to the highly probe-frequency dependent perturbed free-induction decays or uncoupled Rabi oscillations (‘flopping')59.…”
Section: Resultsmentioning
confidence: 98%
“…Figure 6a shows examples of the oscillatory signals we observe. The oscillations start at negative time delays when the probe pulse arrives at the sample before the excitation pulse, suggesting that the probe pulse generates a coherence that the excitation pulse interacts with, as observed in perturbed free-induction decays45565758. However, the periods of the oscillations we observe are insensitive to probe frequency or pump pulse intensity, which is in stark contrast to the highly probe-frequency dependent perturbed free-induction decays or uncoupled Rabi oscillations (‘flopping')59.…”
Section: Resultsmentioning
confidence: 98%
“…S13). To minimize these oscillations, these data were filtered using an established method 72,73 for removing time-and frequency-dependent oscillations due to perturbed free-induction decay (PFID); 74,75 the resulting filtered transients are shown in Figs. 2 and 3.…”
Section: Results and Analysismentioning
confidence: 99%
“…The transient behavior of RDX is qualitatively similar for both pump frequencies and, except where noted, the following descriptions will apply to all transient results. To avoid the interpretation of coherent artifacts, [74][75][76] we will limit our analysis to signal occurring for Δt ≥ 0.3 ps. By 0.3 ps, the transient spectra show a negative change in absorbance due to stimulated emission or loss of ground state absorption (henceforth referred to as "bleach") from all vibrational modes across the probed spectral range.…”
Section: Frequencymentioning
confidence: 99%
“…Under this framework, harmonic waves cease to be solutions of Maxwell's equations, and effects such as frequency conversion, [36][37][38] photon acceleration, 35 nonreciprocal light reflection, beam steering or focusing [39][40][41] that are impossible in stationary systems rise, similar to original works in rapidly generated plasmas. 42,43 The frequency conversion that has recently been demonstrated for metasurfaces also has origins similar to that of the coherent artifact in ultrafast time-resolved infrared (IR) spectroscopy of vibrational transitions in chemical systems 44,45 and for semiconductors, 46,47 which manifest at negative time delays, when the probe pulse precedes the pump pulse. Even though many systems have demonstrated linear frequency conversion due to abrupt time modulation, ultrafast studies of nonlinear responses, [48][49][50][51] which are prominent in resonant metasurfaces, are yet to unveil the control of light frequency for nonlinearly generated waves.…”
Section: Introductionmentioning
confidence: 93%