Golter D A, Lai C W
US Army Research Laboratory, 2800 Powder Mill Rd, Adelphi, MD, 20783, USA.
Sci Rep. 2017 Oct 17;7(1):13406. doi: 10.1038/s41598-017-13813-2.
We demonstrate optically induced switching between bright and dark charged divacancy defects in 4H-SiC. Photoluminescence excitation and time-resolved photoluminescence measurements reveal the excitation conditions for such charge conversion. For an energy below 1.3 eV (above 950 nm), the PL is suppressed by more than two orders of magnitude. The PL is recovered in the presence of a higher energy repump laser with a time-averaged intensity less than 0.1% that of the excitation field. Under a repump of 2.33 eV (532 nm), the PL increases rapidly, with a time constant 30 μs. By contrast, when the repump is switched off, the PL decreases first within 100-200 μs, followed by a much slower decay of a few seconds. We attribute these effect to the conversion between two different charge states. Under an excitation at energy levels below 1.3 eV, VV are converted into a dark charge state. A repump laser with an energy above 1.3 eV can excite this charged state and recover the bright neutral state. This optically induced charge switching can lead to charge-state fluctuations but can be exploited for long-term data storage or nuclear-spin-based quantum memory.
我们展示了在4H-SiC中明亮和暗带电双空位缺陷之间的光诱导切换。光致发光激发和时间分辨光致发光测量揭示了这种电荷转换的激发条件。对于低于1.3 eV(高于950 nm)的能量,光致发光被抑制了两个多数量级。在存在时间平均强度小于激发场强度0.1%的更高能量再泵浦激光时,光致发光得以恢复。在2.33 eV(532 nm)的再泵浦下,光致发光迅速增加,时间常数为30 μs。相比之下,当再泵浦关闭时,光致发光首先在100 - 200 μs内下降,随后是几秒钟的慢得多的衰减。我们将这些效应归因于两种不同电荷状态之间的转换。在低于1.3 eV能级的激发下,VV被转换为暗电荷状态。能量高于1.3 eV的再泵浦激光可以激发这种带电状态并恢复明亮的中性状态。这种光诱导电荷切换会导致电荷态波动,但可用于长期数据存储或基于核自旋的量子存储器。