Optical parametric amplification by monolayer transition metal dichalcogenides

Optical parametric amplification by monolayer transition metal dichalcogenides
复制标题

DOI:
10.1038/s41566-020-00728-0
复制
发表时间:
2020-12-21
期刊:
影响因子:
35
通讯作者:
Cerullo, Giulio
Cerullo, Giulio
中科院分区:
物理与天体物理1区
文献类型:
--
作者:
Trovatello, Chiara;Marini, Andrea;Cerullo, Giulio

文献摘要

被引文献

相似文献

光参量放大是一种二阶非线性过程,通过产生空闲场,光信号被泵浦放大。这种机制本质上与自发的参数下转换有关,它目前构成了纠缠光子对产生的基础(2),这是现代量子技术中利用的一个过程。在这里,我们演示了在极限厚度下的单程光学参量放大;使用半导体过渡金属二卤代化合物(3,4),我们证明了通过单原子层的超传播可以实现放大。这种二维极限的二阶非线性相互作用绕过了相位匹配要求(5),实现了超宽带放大带宽。与第一性原理计算一致,我们观察到放大过程与信号场和泵浦光场的面内极化无关。通过AA堆积多层膜的使用,我们为转换效率的扩展提供了一条清晰的途径。我们的结果为开发原子大小的可调谐辐射源铺平了道路,该辐射源在纳米光子学和量子信息技术中具有潜在的应用前景。
Optical parametric amplification is a second-order nonlinear process whereby an optical signal is amplified by a pump via the generation of an idler field'. This mechanism is inherently related to spontaneous parametric down-conversion, which currently constitutes the building block for entangled photon pair generations(2), a process that is exploited in modern quantum technologies. Here we demonstrate single-pass optical parametric amplification at the ultimate thickness limit; using semiconducting transition metal dichalcogenides(3,4), we show that amplification can be attained over propagation through a single atomic layer. Such a second-order nonlinear interaction at the two-dimensional limit bypasses phase-matching requirements(5) and achieves ultrabroad amplification bandwidths. In agreement with first-principle calculations, we observe that the amplification process is independent of the in-plane polarization of signal and pump fields. By the use of AA-stacked multilayers, we present a clear pathway towards the scaling of conversion efficiency. Our results pave the way for the development of atom-sized tunable sources of radiation with potential applications in nanophotonics and quantum information technology.