Inverse Electromagnetically Induced Transparency in Multimode Cavity Optomechanical Systems

Fig. 2. Variation of number of output probe photons with n value under different cavity field power conditions. (a) $n = 0$ ; (b) $n = 0.5$ ; (c) $n = 1$ ; (d) $n = 1.5$

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Fig. 3. Variation of number of probe photons and mechanical excitation $b_{2}$ with n value under different cavity field power conditions. (a)(b) $n = 0$ ; (c)(d) $n = 1$

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Fig. 4. Variation of number of probe photons and two mechanical excitations in the cavity under different conditions. (a)-(c) Variation of number of probe photons and mechanical excitation $b_{1}$ and $b_{2}$ in the cavity at $n = 0.5$ under different cavity field power conditions; (d) when $G_{2} = 2 κ$ , peak value of number of probe photons and mechanical excitation $b_{1}$ and $b_{2}$ varing with $n$

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Fig. 5. Variation of number of probe photons and two mechanical excitations in the cavity under different conditions. (a)-(c) Variation of number of probe photons and mechanical excitation $b_{1}$ and $b_{2}$ in the cavity at $n = 1.5$ under different cavity field power conditions; (d) when $G_{2} = 2 κ$ , variation of the width of number of probe photons and mechanical excitation $b_{1}$ and $b_{2}$ with $n$

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Yunhe Liu, Huajun Chen. Inverse Electromagnetically Induced Transparency in Multimode Cavity Optomechanical Systems[J]. Acta Optica Sinica, 2023, 43(22): 2226001

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Paper Information

Category: Physical Optics

Received: May. 17, 2023

Accepted: Jul. 12, 2023

Published Online: Nov. 8, 2023

The Author Email: Chen Huajun (chenphysics@126.com)

DOI:10.3788/AOS230998

Topics

laser devices and laser physics

Lasers and Laser Optics

Laser physics

laser manufacturing

Instrumentation, Measurement and Metrology