1966
DOI: 10.1103/physrevlett.17.1281
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Observation of Degenerate Stimulated Four-Photon Interaction and Four-Wave Parametric Amplification

Abstract: mogeneously distributed stresses that would induce splitting of the J= 1 level. 7 T A in solid H 2 with high concentrations of ortho was first calculated by T. Moriya and K. Motizuki, Progr. •.Theoret. Phys. (Kyoto) 18_, 183 (1957). The calculation has been repeated recently by A. B. Harris and E. Hunt, Phys. Rev. Letters 16_, 845 (1966).

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Cited by 136 publications
(26 citation statements)
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“…Through this interaction, an intense be am can increase the index of refraction of the medium (solid, liquid, or gas) in which the be am is propagating. This causes self-focusing of the laser beam, because wherever the beam is most intense the refractive index increases, causing a locallenslike action that further increases the intensity of that portion of the be am [9]. The nonlinear response to the electrie field strength (a result of anharmonie electron motion) causes waves to be genera ted at harmonies of the frequency of the incoming beam [10].…”
Section: The 1960s At Stanford and Eisewherementioning
confidence: 96%
“…Through this interaction, an intense be am can increase the index of refraction of the medium (solid, liquid, or gas) in which the be am is propagating. This causes self-focusing of the laser beam, because wherever the beam is most intense the refractive index increases, causing a locallenslike action that further increases the intensity of that portion of the be am [9]. The nonlinear response to the electrie field strength (a result of anharmonie electron motion) causes waves to be genera ted at harmonies of the frequency of the incoming beam [10].…”
Section: The 1960s At Stanford and Eisewherementioning
confidence: 96%
“…Growth of small-scale low-level beam ripples occurs because the non linear interaction causes power to transfer from the main-beam mode to the smaller-scale ripple modes via a parametric interaction. 65 Figure 35 schematically demonstrates the effect. Figure 36 shows the results of an experiment showing this effect.…”
Section: 7smentioning
confidence: 99%
“…This process allows for the conversion or amplification of coherent signals and has been demonstrated in a wide number of waveguides including optical fibers, microstructured fibers and dispersion shifted fibers [2][3][4][5][6]. As the process exploits the Kerr effect in a medium, it is more easily achieved in a medium with relatively high nonlinearity [7].…”
Section: Introductionmentioning
confidence: 99%