1981
DOI: 10.1007/978-3-662-08257-7_4
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Spectroscopic Instrumentation

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Cited by 50 publications
(71 citation statements)
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“…In contrast to previous state-resolved studies, 5 we per- formed the laser excitation of the molecular beam in close proximity to target surface in order to minimize the loss of alignment by nuclear hyperfine depolarization. 19 The focal length and position of the cylindrical lens were chosen to create an IR radiation field with suitably curved wavefronts to achieve Doppler tuning through a rovibrational transition for the methane molecules as they move through the focused laser beam. This Doppler tuning in combination with a suitably strong excitation field leads to excitation via rapid adiabatic passage (RAP), 20 which allows for complete population inversion of the rovibrational transition used for excitation.…”
Section: Methodsmentioning
confidence: 99%
“…In contrast to previous state-resolved studies, 5 we per- formed the laser excitation of the molecular beam in close proximity to target surface in order to minimize the loss of alignment by nuclear hyperfine depolarization. 19 The focal length and position of the cylindrical lens were chosen to create an IR radiation field with suitably curved wavefronts to achieve Doppler tuning through a rovibrational transition for the methane molecules as they move through the focused laser beam. This Doppler tuning in combination with a suitably strong excitation field leads to excitation via rapid adiabatic passage (RAP), 20 which allows for complete population inversion of the rovibrational transition used for excitation.…”
Section: Methodsmentioning
confidence: 99%
“…The heart of experimentally testing and controlling classical and quantum systems often lies in the introduction of an external periodic driving force [1,2,3]. The driving probes system specific properties, the knowledge of which allows one, in turn, to understand and to optimally control the system at hand.…”
Section: Introductionmentioning
confidence: 99%
“…Noteworthy, the differential scheme is expected to perform the same in reflection, which will be simpler to implement experimentally as only one objective needs then to be aligned. The sample is modeled in space as an ensemble of voxels containing each a collection of independent oscillators and, for each sample voxel, the change in intensity due to stimulated absorption/emission [49], along the coordinate z defined as the axis of propagation of the light pulses, normal to the sample surface, is inferred from…”
Section: Modelmentioning
confidence: 99%