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全光二极管和全光三极管是实现全光逻辑器件的基础. 我们之前已经研究了基于腔量子电动力学的全光二极管的量子统计性质 [
1 ], 讨论了在相干光和压缩光入射的情况下, 通过二极管后输出光的压缩性质. 这里将研究拓展到全光三极管, 以基于腔光机械系统的全光三极管作为研究对象. 这种全光三极管通过改变经典抽运光的强度可以对探测光的输出进行有效调控, 并可实现光放大. 本文具体讨论以压缩光以及相干光作为探测光, 通过全光三极管后其输出光的压缩特性. 研究结果表明, 当探测光为相干光时, 不论是否工作在光放大区域, 输出光依然为相干光, 没有被压缩. 而当输入探测光为压缩光时, 在全光三极管的光放大区域, 输出光依然是压缩光, 但压缩特性受到输入光压缩特性以及系统参数的调制. 当输入探测压缩光的压缩角为0时, 输出光的压缩参量 S 1的最小值随输入探测光压缩系数 r的增大而减小, 最小值接近压缩极限–0.25. 但当输入探测压缩光的压缩角改变时, 其对输出光的压缩参量 S 1,2影响很大, 压缩性会消失. 只有当压缩角 θ为π的整数倍时, 输出光的压缩性最好. 这一结果在量子测量、弱信号检测等领域有着潜在的应用价值.All-optical diodes and all-optical transistors are the basis of all-optical logic devices. We study the quantum statistical properties of all-optical diodes based on cavity quantum electrodynamics (QED) [1 ], and discuss the squeezed properties of the output light after passing through the diode when coherent light and squeezed light are incident. Here we extend our research to all-optical transistor, and take all-optical transistor based on cavity optomechanical system as the research object. By changing the intensity of classical pump light, the all-optical transistor can effectively control the output of the probe light and realize optical amplification. We discuss the squeezed properties of the output light of the all-optical transistor with squeezed light and coherent light as the probe light. Our results show that when the probe light is coherent, the output light remains coherent no matter whether it works in the amplified region, and is not squeezed. When the input probe light is amplitude squeezed light, the output light is still squeezed light in the light amplification region of all-optical transistor, but the squeezed properties are modulated by the input light squeezed properties and system parameters. When the squeezed angle of the input probe squeezed light is 0°, the minimum squeezed parameter S 1of the output squeezed light decreases with the increase of the squeezed coefficient r of the input probe light, and the minimum value approaches to the squeezed limit of –0.25. But the change of squeezed angle of the input probe squeezed light changes has a great influence on the squeezed parameter S 1,2of the output light, and the squeezed properties will disappear. Only when the squeezed angle is an integer multiple of π, will the squeezed properties of the output light be best. This result has a potential application value in quantum measurement, weak signal detection, and other fields.[1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] -
[1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30]
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