1993
DOI: 10.1016/0009-2614(93)89002-y
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Phase-dependent absorption and stimulated emission in femtosecond pump-probe experiments

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Cited by 17 publications
(13 citation statements)
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“…Linear response theory of four-wave mixing typically represents the separate moments from cumulant expansions of the density operator, as shown by several authors in the past [46,[49][50][51][52]. A very useful picture of the interaction caused by the pump pulse, when separated from a probe, represents the 'Wigner' phase space [53][54][55] which allows a semi-classical description of the ultrafast material response.…”
Section: Vibrational Coherence Contributions With Femtosecond Opticalmentioning
confidence: 99%
“…Linear response theory of four-wave mixing typically represents the separate moments from cumulant expansions of the density operator, as shown by several authors in the past [46,[49][50][51][52]. A very useful picture of the interaction caused by the pump pulse, when separated from a probe, represents the 'Wigner' phase space [53][54][55] which allows a semi-classical description of the ultrafast material response.…”
Section: Vibrational Coherence Contributions With Femtosecond Opticalmentioning
confidence: 99%
“…[28][29][30] Another approach in the well-separated pulse limit is based on a description of the pump induced medium using nonstationary effective linear response functions. 10,25,[31][32][33] We have recently demonstrated the application of an effective linear response approach to pump-probe spectroscopy using a displaced thermal state representation of the pump induced ͑doorway͒ density matrix. 27 A key requirement for this representation is a knowledge of the moments of position (Q) and momentum ( P) in the doorway state.…”
Section: Introductionmentioning
confidence: 99%
“…The absorption spectrum at a frequency ⍀ is given by 34 are the Fourier transforms of the positive frequency components of the polarization P ϩ (t) and the field amplitude E(t), respectively. An optical polarization in the medium P(t) ϭ P ϩ (t)exp(Ϫit)ϩc.c.…”
Section: Calculation Of the Absorption Spectrummentioning
confidence: 99%
“…͑33͒ shows a phase dependent absorption. 34 In spite of the presence of a relatively large parameter in the denominator of this term, the last can be important when the imaginary part of the susceptibility Im ͓(t sp ),t sp ͔ϳ͐ Ϫϱ ϱ d␣͓F 1M ((t sp )Ϫ 21 ϩ␣) 1s (␣,t sp )ϪF 2M ((t sp )Ϫ 21 ϩ␣) 2s (␣,t sp )] is small. At the same time the real part of the susceptibility Re ((t),t) does not need to be small due to different frequency dependences of the imaginary and real parts of the susceptibility.…”
Section: ͑29͒mentioning
confidence: 99%
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