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共振介质存在下的量子干涉。

Quantum interference in the presence of a resonant medium.

作者信息

Kalashnikov Dmitry A, Melik-Gaykazyan Elizaveta V, Kalachev Alexey A, Yu Ye Feng, Kuznetsov Arseniy I, Krivitsky Leonid A

机构信息

Data Storage Institute, Agency for Science, Technology and Research (A*STAR), 138634, Singapore, Singapore.

Faculty of Physics, M. V. Lomonosov Moscow State University, 119991, Moscow, Russia.

出版信息

Sci Rep. 2017 Sep 13;7(1):11444. doi: 10.1038/s41598-017-11694-z.

Abstract

Interaction of light with media often occurs with a femtosecond response time. Its measurement by conventional techniques requires the use of femtosecond lasers and sophisticated time-gated optical detection. Here we demonstrate that by exploiting quantum interference of entangled photons it is possible to measure the dephasing time of a resonant media on the femtosecond time scale (down to 100 fs) using accessible continuous wave laser and single-photon counting. We insert a sample in the Hong-Ou-Mandel interferometer and observe the modification of the two-photon interference pattern, which is driven by the coherent response of the medium, determined by the dephasing time. The dephasing time is then inferred from the observed pattern. This effect is distinctively different from the basic effect of spectral filtering, which was studied in earlier works. In addition to its ease of use, our technique does not require compensation of group velocity dispersion and does not induce photo-damage of the samples. Our technique will be useful for characterization of ultrafast phase relaxation processes in material science, chemistry, and biology.

摘要

光与介质的相互作用通常发生在飞秒响应时间内。用传统技术测量它需要使用飞秒激光器和复杂的时间选通光学检测。在此我们证明,通过利用纠缠光子的量子干涉,使用普通连续波激光器和单光子计数,就有可能在飞秒时间尺度(低至100飞秒)上测量共振介质的退相时间。我们在Hong-Ou-Mandel干涉仪中插入一个样品,并观察由介质的相干响应驱动的双光子干涉图样的变化,该相干响应由退相时间决定。然后从观察到的图样推断出退相时间。这种效应与早期工作中研究的光谱滤波的基本效应明显不同。除了使用方便之外,我们的技术不需要补偿群速度色散,也不会对样品造成光损伤。我们的技术将有助于表征材料科学、化学和生物学中的超快相位弛豫过程。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eea1/5597610/d2246703e37c/41598_2017_11694_Fig1_HTML.jpg

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