2009
DOI: 10.1016/j.optcom.2009.08.049
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Measurement of coherence dynamics based on coherent anti-Stokes Raman scattering

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Cited by 2 publications
(1 citation statement)
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“…Stimulated Raman adiabatic passage (STIRAP) and its variations are established techniques for efficient manipulation of population among states of atoms or molecules. STIRAP has been implemented with continuous wave (cw) [1] and pulsed [2] lasers for a variety of purposes such as: the preparation of molecules in specific rovibrational states for chemical reactions [3], preparation of molecules for dissociative attachment of electrons [4,5], excitation of targeted magnetic sub levels [6] and superpositions of levels [7,8], selective momentum transfer for isotopic separation [9], Rydberg state excitation [10,11], excitation between dipole-forbidden states through a continuum of states [12], the coherent preparation of atoms to optimize [13] or measure [14] coherent anti-Stokes Raman scattering (CARS), excitation of individual Ca 2+ ions and their potential for information storage [15], coherent optical transfer of Feshbach molecules to a lower vibrational state [16], photo association of bi-alkali [17,18], and other molecules [19], creating a population inversion in dopants of a solid [20] including tripod STIRAP in a doped Pr 3+ : Y 2 SiO 5 [21], storing information [22], and performing logic operations [23] in doped solids. * mtilley@uw.edu, Corresponding author…”
Section: Introductionmentioning
confidence: 99%
“…Stimulated Raman adiabatic passage (STIRAP) and its variations are established techniques for efficient manipulation of population among states of atoms or molecules. STIRAP has been implemented with continuous wave (cw) [1] and pulsed [2] lasers for a variety of purposes such as: the preparation of molecules in specific rovibrational states for chemical reactions [3], preparation of molecules for dissociative attachment of electrons [4,5], excitation of targeted magnetic sub levels [6] and superpositions of levels [7,8], selective momentum transfer for isotopic separation [9], Rydberg state excitation [10,11], excitation between dipole-forbidden states through a continuum of states [12], the coherent preparation of atoms to optimize [13] or measure [14] coherent anti-Stokes Raman scattering (CARS), excitation of individual Ca 2+ ions and their potential for information storage [15], coherent optical transfer of Feshbach molecules to a lower vibrational state [16], photo association of bi-alkali [17,18], and other molecules [19], creating a population inversion in dopants of a solid [20] including tripod STIRAP in a doped Pr 3+ : Y 2 SiO 5 [21], storing information [22], and performing logic operations [23] in doped solids. * mtilley@uw.edu, Corresponding author…”
Section: Introductionmentioning
confidence: 99%