利用高压纳秒脉冲和光致发光光谱分析探测NV和SiV电荷态动力学

Artur Pambukhchyan, Sizhe Weng, Indu Aravind, S. Cronin, Susumu Takahashi
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摘要

金刚石中的氮空位(NV)和硅空位(SiV)色缺陷是在量子技术中有应用前景的系统。NV和SiV中心具有多种电荷态,它们的电荷态具有不同的电子、光学和自旋性质。对于NV中心,大多数量子传感应用的研究都是针对带负电荷的NV (NV$^{-}$), NV中心处于NV$^{-}$状态是很重要的。然而,已知在激光激发下,NV中心转变为中性带电态(NV$^{0}$)。NV和SiV中心的能量有利电荷态取决于它们的局部环境。理解和控制电荷态动力学对于它们的量子应用至关重要。本文讨论了高压纳秒脉冲放电下NV和SiV中心的电荷态动力学。NV中心和SiV中心在金刚石晶体中共存。高压脉冲能够有效地控制电荷状态。通过光致发光光谱分析探讨了这些电压引起的电荷态变化。实验分析结果表明,高压纳秒脉冲能引起化学势的位移,使NV和SiV中心的电荷态发生转换,转换速率为$\sim$ MHz。这一结果还表明,样品中SiV中心的主要种群是双负电荷态(SiV$^{2-}$),由于其非荧光和非磁性而经常被忽视。该演示为未来快速操纵NV和SiV电荷态的方法铺平了道路。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Probing NV and SiV charge state dynamics using high-voltage nanosecond pulse and photoluminescence spectral analysis
Nitrogen-vacancy (NV) and silicon-vacancy (SiV) color defects in diamond are promising systems for applications in quantum technology. The NV and SiV centers have multiple charge states, and their charge states have different electronic, optical and spin properties. For the NV centers, most investigations for quantum sensing applications are targeted on the negatively charged NV (NV$^{-}$), and it is important for the NV centers to be in the NV$^{-}$ state. However, it is known that the NV centers are converted to the neutrally charged state (NV$^{0}$) under laser excitation. An energetically favorable charge state for the NV and SiV centers depends on their local environments. It is essential to understand and control the charge state dynamics for their quantum applications. In this work, we discuss the charge state dynamics of NV and SiV centers under high-voltage nanosecond pulse discharges. The NV and SiV centers coexist in the diamond crystal. The high-voltage pulses enable manipulating the charge states efficiently. These voltage-induced changes in charge states are probed by their photoluminescence spectral analysis. The analysis result from the present experiment shows that the high-voltage nanosecond pulses cause shifts of the chemical potential and can convert the charge states of NV and SiV centers with the transition rates of $\sim$ MHz. This result also indicates that the major population of the SiV centers in the sample is the doubly negatively charged state (SiV$^{2-}$), which is often overlooked because of its non-fluorescent and non-magnetic nature. This demonstration paves a path for a method of rapid manipulation of the NV and SiV charge states in the future.
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