2019
DOI: 10.1364/oe.27.018883
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Pulse operation of linearly polarized diode-pumped cesium-vapor laser based on acousto-optical modulation

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“…Conventionally, the polarization state manipulations of the light are static, which are controlled by the anisotropic response of the two orthogonal electric field components of the light, such as the dichromatic organic films and birefringent crystals. Then the electro‐optical (Pockels cells), [ 11–13 ] acousto‐optical (Raman–Nath diffractometers), [14 ] and magneto‐optical (Faraday rotators) [ 15,16 ] effects are leveraged to achieve the active polarization elements with high switching speed. However, they suffer from the macroscopic size, inappropriate for integration into optical and optoelectronic systems.…”
Section: Introductionmentioning
confidence: 99%
“…Conventionally, the polarization state manipulations of the light are static, which are controlled by the anisotropic response of the two orthogonal electric field components of the light, such as the dichromatic organic films and birefringent crystals. Then the electro‐optical (Pockels cells), [ 11–13 ] acousto‐optical (Raman–Nath diffractometers), [14 ] and magneto‐optical (Faraday rotators) [ 15,16 ] effects are leveraged to achieve the active polarization elements with high switching speed. However, they suffer from the macroscopic size, inappropriate for integration into optical and optoelectronic systems.…”
Section: Introductionmentioning
confidence: 99%