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Optoelectronics Letters

Four-bit all-optical quantization based on Raman self-fre-quency shift and spectral compression

梁锐, 周晓军, 张旨遥, 李和平, 刘永智, 刘永

Published Jan 1, 2009• 0 citations
OpenAlex

Abstract

所有光的量子化基于在 photonic 水晶纤维(PCF ) 的拉曼自我频率移动(RSFS ) 并且光谱在增加分散的纤维(DIF ) 的压缩被分析,并且在纤维的 femtosecond 脉搏的进化被数字地解决概括非线性的 Schr 描述 ? 黑人方程(GNLSE ) 。有 300 fs 的宽度和 1550 nm 的中心波长的 Gaussian 脉搏被注入 15 m 长的 PCF 和 100 m 长的 DIF。模拟结果证明中心波长与从 110 W 改变到 165 W 的输入山峰力量线性地增加。65.3 nm 的 RSFS 并且最大光谱压缩比率 3.38 能被获得。量子化的决定被使用从 2.4 位改进到 4 位光谱在 DIF 的压缩。

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所有光的量子化基于在 photonic 水晶纤维(PCF ) 的拉曼自我频率移动(RSFS ) 并且光谱在增加分散的纤维(DIF ) 的压缩被分析,并且在纤维的 femtosecond 脉搏的进化被数字地解决概括非线性的 Schr 描述 ? 黑人方程(GNLSE ) 。有 300 fs 的宽度和 1550 nm 的中心波长的 Gaussian 脉搏被注入 15 m 长的 PCF 和 100 m 长的 DIF。模拟结果证明中心波长与从 110 W 改变到 165 W 的输入山峰力量线性地增加。65.3 nm 的 RSFS 并且最大光谱压缩比率 3.38 能被获得。量子化的决定被使用从 2.4 位改进到 4 位光谱在 DIF 的压缩。
The advancement of quantum technologies [1] heavily relies on the efficient generation and manipulation of the photon-pairs. Among the numerous methods available for photon-pairs generation, spontaneous four-wave mixing (SFWM) in photonic crystal fibers [2] has emerged as a promising technique due to its inherent advantages in scalability and integration within existing telecommunication infrastructures. Inhibited-coupling hollow-core photonic crystal fibers (IC-HCPCFs) filled with inert gases provide a unique platform for SFWM-based photon- pairs generation, offering several features including entanglement control [3], integrability into telecommunication networks and also Raman-free generation [4] which minimizes noise and enhances the purity of the generated photon-pairs resulting in record coincidence-to-accidental ratio (CAR) superior to 104[5]. Building upon these advantages, we have recently focused on enhancing the photon-pairs brightness. In our previous work, we demonstrated significant improvements in brightness through optimization of fiber parameters such length, effective area and dispersion [5]–[6] on one hand and the use of a GHz-repetition rate femtosecond laser [7] on another hand to get closer to the MHz-level. One of the remaining parameters to further improve the generation efficiency(η)(\eta)(η)of IC-HCPCF based photon-pair source, and thereby conclude our investigation, is the pump pulse duration(τp)(\tau_{\mathrm{p}})(τp​). Sinceη\etaηis inversely proportional to the pump pulse duration [8], shorter pulses are expected to yield larger brightness. In this work, we developed a homemade pulse compressor [9] based on a hybrid IC-HCPCF design [10], which was integrated as the first stage of our photon-pair generation set-up as shown in Fig. 1a. By engineering the fiber dispersion and by controlling the optical nonlinearities through the pressure of the filling gas (argon), we achieved a self-compression of input pulses from an ultrashort pulse laser (~280 fs pulse width,1030 nm wavelength, 2 MHz repetition rate) down to ~35 fs. Fig. 1b shows the pulse duration of the compressor output over an input energy range of0.01μJ0.01 \mu \mathrm{J}0.01μJto0.7μJ0.7 \mu \mathrm{J}0.7μJ. The energy transmission efficiency of the compressor was measured to exceed 80%. This compressor enables tunable pulse durations ranging from 280 fs down to 35 fs. As expected, the compression was accompanied by a spectral broadening from 8 nm to 41 nm (gaussian fit FWHM), primarly driven by self-phase modulation (see Fig. 1c). The compressed pulses were subsequently coupled into the photon-pair generation fiber (1 m of tubular lattice HCPCF with a 40 μm core, filled with xenon at 3.2 bar). As expected, when the pulse duration is reduced, the brightness increase scales as1/τp1 / \tau_{\mathrm{p}}1/τp​(see Fig. 1d). For the shortest input duration of 35 fs, the brightness was enhanced by a factor of 7.7, which is in agreement with the expected value. Additionally, we observed a slight improvement in the CAR attributed to the increase in the number of coincidences (see Fig. 1e). Finally, the structuring of the spectral pump has led to a change in the joint spectral intensity (JSI) pattern (see inset of Fig. 1d). The implication of this change on the photon-correlation is under investigation.