Low-noise quantum frequency down-conversion of indistinguishable photons (Conference Presentation)

Benjamin Kambs, J. Kettler, M. Bock, J. Becker, C. Arend, M. Jetter, P. Michler, C. Becher
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Abstract

Single-photon sources based on quantum dots have been shown to exhibit almost ideal properties such as high brightness and purity in terms of clear anti-bunching as well as high two-photon interference visibilities of the emitted photons, making them promising candidates for different quantum information applications such as quantum computing, quantum communication and quantum teleportation. However, as most single-photon sources also quantum dots typically emit light at wavelengths of electronic transitions within the visible or the near infrared range. In order to establish quantum networks with remote building blocks, low-loss single photons at telecom wavelengths are preferable, though. Despite recent progress on emitters of telecom-photons, the most efficient single-photon sources still work at shorter wavelengths. On that matter, quantum frequency down-conversion, being a nonlinear optical process, has been used in recent years to alter the wavelength of single photons to the telecom wavelength range while conserving their nonclassical properties. Characteristics such as lifetime, first-order coherence, anti-bunching and entanglement have been shown to be conserved or even improved due to background suppression during the conversion process, while the conservation of indistinguishability was yet to be shown. Here we present our experimental results on quantum frequency down-conversion of single photons emitted by an InAs/GaAs quantum dot at 903.6 nm following a pulsed excitation of a p-shell exciton at 884 nm. The emitted fluorescence photons are mixed with a strong pump-field at 2155 nm inside a periodically poled lithium niobate ridge waveguide and converted to 1557 nm. Common issues of a large background due to Raman-scattered pump-light photons spectrally overlapping with the converted single photons could largely be avoided, as the pump-wavelength was chosen to be fairly longer than the target wavelength. Additional narrowband spectral filtering at the telecom regime as a result of the small conversion bandwidth and using a high-performance fiber-Bragg-grating solely left the detector dark counts as the only noise source in our setup. Therefore, we could achieve conversion efficiencies of more than 20 %. In order to test the indistinguishability, sequentially emitted photons were fed into a Mach-Zehnder interferometer and spatially as well as temporally overlapped at the output beam splitter. Cross-correlation measurements between both output-ports of the beam splitter exhibit two-photon interference contrasts of more than 40 % prior to and after the down-conversion step. Accordingly, we demonstrate that the process of quantum frequency conversion preserves photon indistinguishability and can be used to establish a versatile source of indistinguishable single photons at the telecom C-Band. Furthermore our scheme allows for converting photons in a wavelength band from 900 nm to 910 nm to the same telecom target wavelength. This enables us to test indistinguishability of frequency-converted photons, originally stemming from different sources with dinstinguishable wavelengths.
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不可分辨光子的低噪声量子频率下变频(会议报告)
基于量子点的单光子源已经显示出几乎理想的特性,如高亮度和纯度,在清晰的反聚束方面以及发射光子的高双光子干涉可见性,使它们成为不同量子信息应用的有希望的候选者,如量子计算,量子通信和量子隐形传态。然而,正如大多数单光子源一样,量子点通常在可见光或近红外范围内发射电子跃迁波长的光。不过,为了用远程构建块建立量子网络,电信波长的低损耗单光子更可取。尽管最近在电信光子发射器上取得了进展,但最有效的单光子源仍然工作在更短的波长上。在这个问题上,量子频率下转换作为一种非线性光学过程,近年来被用来改变单光子的波长到电信波长范围,同时保持它们的非经典性质。在转换过程中,由于背景抑制,诸如寿命、一阶相干性、反聚束和纠缠等特性被证明是守恒的,甚至得到了改善,而不可区分性的守恒尚未得到证明。本文介绍了在884 nm处脉冲激发p壳激子后,InAs/GaAs量子点在903.6 nm处发射的单光子量子频率下转换的实验结果。在周期性极化的铌酸锂脊波导中,将发射的荧光光子与2155 nm的强泵浦场混合,并转换为1557 nm。由于拉曼散射泵浦光光子与转换后的单光子在光谱上重叠而导致的大背景的常见问题可以在很大程度上避免,因为泵浦波长被选择得比目标波长长得多。在我们的设置中,由于较小的转换带宽和使用高性能光纤布拉格光栅,在电信系统中进行了额外的窄带频谱滤波,仅将检测器暗计数作为唯一的噪声源。因此,我们可以实现超过20%的转换效率。为了测试不可区分性,将顺序发射的光子送入马赫-曾德尔干涉仪,并在输出分束器处空间和时间上重叠。在分束器的两个输出端口之间的相互关联测量显示,在下转换步骤之前和之后的双光子干涉对比度超过40%。因此,我们证明了量子频率转换过程保持了光子的不可区分性,并可用于在电信c波段建立不可区分的单光子的通用源。此外,我们的方案允许将900 nm至910 nm波长范围内的光子转换为相同的电信目标波长。这使我们能够测试频率转换光子的不可区分性,这些光子最初来自具有不可区分波长的不同光源。
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