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arXiv 2602.06140cond-mat.mes-hallquant-ph
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在1550 nm处通过共振两光子激发增强的量子点产生高度不可区分的单光子

Highly-Indistinguishable Single-Photons at 1550 nm from a Two-photon Resonantly Excited Purcell-enhanced Quantum Dot

University of Würzburg(维尔茨堡大学)
Robert Behrends, Martin v. Helversen, Pratim K. Saha, Lucas Rickert, Koray Kaymazlar, Mareike Lach, Nils D. Kewitz, Jochen Kaupp, Yorick Reum, Tobias Huber-Loyo… 展开作者

Robert Behrends, Martin v. Helversen, Pratim K. Saha, Lucas Rickert, Koray Kaymazlar, Mareike Lach, Nils D. Kewitz, Jochen Kaupp, Yorick Reum, Tobias Huber-Loyola, Sven Höfling, Andreas Pfenning, Tobias Heindel

AI总结:

通过共振两光子激发增强的量子点在1550 nm处产生高度不可区分的单光子,实现了高可见度的两光子干涉。

摘要:

在本工作中,我们展示了一个增强腔体的InAs/In0.53Al0.23Ga0.24As量子点(QD)单光子源,处于电信C波段,其双激发子发射衰减时间达到记录低的67.4(2) ps,通过共振两光子激发(TPE)。我们观察到强的多光子抑制,关联到X激发子(X)和双激发子(XX)发射的g(2)X(0)=0.006(1)和g(2)XX(0)=0.007(1)。由于XX-X级联的非对称 Purcell 增强,XX光子在π脉冲激发下的两光子干涉(TPI)可见度达到理论极限,明显超过标准XX-X级联无光子工程时预期的约60%。此外,添加一个与XX发射能级重合的第二定时激光脉冲,我们展示了在电信C波段的受激发射TPE。结果是X光子的TPI可见度提高了,相比TPE的V_TPI=0.61(4),V_TPI=0.69(3),但两者都由于现有的相位失效应低于理论值。本工作中的进展对于实现基于确定性量子光源的高级量子通信方案具有重要意义。

英文摘要:

In this work we present a cavity-enhanced InAs/$\mathrm{In_{0.53}Al_{0.23}Ga_{0.24}As}$ quantum dot (QD) single-photon source in the telecom C-band with a record-low biexciton emitter decay time of \SI{67.4(2)}{ps} under resonant two-photon excitation (TPE). We observe strong multiphoton suppression associated with $g^{(2)}_\mathrm{X}(0) = 0.006(1)$ and $g^{(2)}_\mathrm{XX}(0) = 0.007(1)$ for the exciton (X) and biexciton (XX) emission, respectively. Due to a asymmetric Purcell enhancement of the XX-X cascade, the two-photon interference (TPI) visibility of XX photons under $π$-pulse excitation of $V_{\rm{TPI}} = 90(3)\%$ reaches the theoretical limit and clearly exceeds the $\sim60\%$ expected for standard XX-X cascades without photonic engineering. Furthermore, adding a second timed laser pulse coinciding with XX emission energy, we demonstrate stimulated TPE in the telecom C-Band. The result is an improved TPI visibility of the X photons of $V_{\rm{TPI}}=0.69(3)$ compared to TPE with $V_{\rm{TPI}}=0.61(4)$, with both being reduced compared to the theoretical values due to present dephasing effects. The advances presented in this work hold important promises for the implementation of advanced schemes of quantum communication using deterministic quantum light sources.

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