2014
DOI: 10.1088/1054-660x/24/8/085406
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Controllable azimuthons of four-wave mixing and their applications

J L2,
et al.

Abstract: We report controllable azimuthons of four-wave mixing (FWM), which can be modulated by several parameters in experiment. The spot number, splitting depth, rotation angular velocity and direction of such azimuthons can be controlled by the frequency and intensity of the FWM signal or the dressing field through the cross-phase modulation due to atomic coherence. The intensity gain of the azimuthons can be modulated by frequency detuning through quantum parametric amplification. The quantum correlated FWM vortex … Show more

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Cited by 3 publications
(1 citation statement)
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“…We take lobes A, B, and C marked in Figure 2a as an instance to explain the formation of vortex. If the strength of complex amplitude vector of compounded field which results from the interference between the light fields of lobes A, B, and C at a point (T x , T y ) on the observa-tion plane is zero, the complex amplitude vector of compounded field at any point with the polar angle πœ‘ around the point (T x , T y ) can be obtained as in polar coordinates [21] E c = A x cos(πœ‘ + 𝛿 1 ) + iA y cos(πœ‘ + 𝛿 2 )…”
Section: Experimental Setup and Theorymentioning
confidence: 99%
“…We take lobes A, B, and C marked in Figure 2a as an instance to explain the formation of vortex. If the strength of complex amplitude vector of compounded field which results from the interference between the light fields of lobes A, B, and C at a point (T x , T y ) on the observa-tion plane is zero, the complex amplitude vector of compounded field at any point with the polar angle πœ‘ around the point (T x , T y ) can be obtained as in polar coordinates [21] E c = A x cos(πœ‘ + 𝛿 1 ) + iA y cos(πœ‘ + 𝛿 2 )…”
Section: Experimental Setup and Theorymentioning
confidence: 99%