Chen Shao-Yu, Lu Zhengguang, Goldstein Thomas, Tong Jiayue, Chaves Andrey, Kunstmann Jens, Cavalcante L S R, Woźniak Tomasz, Seifert Gotthard, Reichman D R, Taniguchi Takashi, Watanabe Kenji, Smirnov Dmitry, Yan Jun
Department of Physics , University of Massachusetts , Amherst , Massachusetts 01003 , United States.
National High Magnetic Field Laboratory , Tallahassee , Florida 32310 , United States.
Nano Lett. 2019 Apr 10;19(4):2464-2471. doi: 10.1021/acs.nanolett.9b00029. Epub 2019 Mar 25.
We report the experimental observation of radiative recombination from Rydberg excitons in a two-dimensional semiconductor, monolayer WSe, encapsulated in hexagonal boron nitride. Excitonic emission up to the 4 s excited state is directly observed in photoluminescence spectroscopy in an out-of-plane magnetic field up to 31 T. We confirm the progressively larger exciton size for higher energy excited states through diamagnetic shift measurements. This also enables us to estimate the 1 s exciton binding energy to be about 170 meV, which is significantly smaller than most previous reports. The Zeeman shift of the 1 s to 3 s states, from both luminescence and absorption measurements, exhibits a monotonic increase of the g-factor, reflecting nontrivial magnetic-dipole-moment differences between ground and excited exciton states. This systematic evolution of magnetic dipole moments is theoretically explained from the spreading of the Rydberg states in momentum space.
我们报告了在封装于六方氮化硼中的二维半导体单层WSe₂中里德堡激子辐射复合的实验观测结果。在高达31 T的面外磁场中,通过光致发光光谱法直接观测到了直至4s激发态的激子发射。我们通过抗磁位移测量证实了能量更高的激发态具有逐渐增大的激子尺寸。这也使我们能够估计1s激子结合能约为170 meV,这比之前的大多数报道都要小得多。从发光和吸收测量得到的1s到3s态的塞曼位移显示,g因子单调增加,这反映了基态和激发态激子之间非平凡的磁偶极矩差异。这种磁偶极矩的系统演化从里德堡态在动量空间中的扩展在理论上得到了解释。