2016
DOI: 10.1016/j.optmat.2016.05.052
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Phase control of six-wave mixing from circularly polarized light

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Cited by 2 publications
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“…In the following section, we will focus on the influence of the E 2 field at different angles on the OB of the PTS and SWM signals. Since the change in the E 2 field angle will cause a change in the signal phase difference, the first-order and fifthorder density matrix of the system should introduce a phase factor ∆φ [16]. The specific expression is as follows: Finally, we will fix the E 2 field intensity to 30 mW, which produces an obvious spectral intensity asymmetry, adjusting the incident angle of the E 2 to 0.3 • to generate EIA dips for PTS and add a QWP in front of the E 2 field to observe the OB of the PTS and SWM signals as the QWP changes.…”
Section: Resultsmentioning
confidence: 99%
“…In the following section, we will focus on the influence of the E 2 field at different angles on the OB of the PTS and SWM signals. Since the change in the E 2 field angle will cause a change in the signal phase difference, the first-order and fifthorder density matrix of the system should introduce a phase factor ∆φ [16]. The specific expression is as follows: Finally, we will fix the E 2 field intensity to 30 mW, which produces an obvious spectral intensity asymmetry, adjusting the incident angle of the E 2 to 0.3 • to generate EIA dips for PTS and add a QWP in front of the E 2 field to observe the OB of the PTS and SWM signals as the QWP changes.…”
Section: Resultsmentioning
confidence: 99%