Kumar Anand, Samaner Çağlar, Cholsuk Chanaprom, Matthes Tjorben, Paçal Serkan, Oyun Yağız, Zand Ashkan, Chapman Robert J, Saerens Grégoire, Grange Rachel, Suwanna Sujin, Ateş Serkan, Vogl Tobias
Department of Computer Engineering, School of Computation, Information and Technology, Technical University of Munich, 80333 Munich, Germany.
Abbe Center of Photonics, Institute of Applied Physics, Friedrich Schiller University Jena, 07745 Jena, Germany.
ACS Nano. 2024 Feb 9;18(7):5270-81. doi: 10.1021/acsnano.3c08940.
Quantum emitters in solid-state crystals have recently attracted a great deal of attention due to their simple applicability in optical quantum technologies. The polarization of single photons generated by quantum emitters is one of the key parameters that plays a crucial role in various applications, such as quantum computation, which uses the indistinguishability of photons. However, the degree of single-photon polarization is typically quantified using the time-averaged photoluminescence intensity of single emitters, which provides limited information about the dipole properties in solids. In this work, we use single defects in hexagonal boron nitride and nanodiamond as efficient room-temperature single-photon sources to reveal the origin and temporal evolution of the dipole orientation in solid-state quantum emitters. The angles of the excitation and emission dipoles relative to the crystal axes were determined experimentally and then calculated using density functional theory, which resulted in characteristic angles for every specific defect that can be used as an efficient tool for defect identification and understanding their atomic structure. Moreover, the temporal polarization dynamics revealed a strongly modified linear polarization visibility that depends on the excited-state decay time of the individual excitation. This effect can potentially be traced back to the excitation of excess charges in the local crystal environment. Understanding such hidden time-dependent mechanisms can further improve the performance of polarization-sensitive experiments, particularly that for quantum communication with single-photon emitters.
固态晶体中的量子发射体最近因其在光量子技术中的简单适用性而备受关注。量子发射体产生的单光子的偏振是在各种应用中起关键作用的关键参数之一,例如利用光子不可区分性的量子计算。然而,单光子偏振度通常使用单个发射体的时间平均光致发光强度来量化,这提供了关于固体中偶极子特性的有限信息。在这项工作中,我们使用六方氮化硼和纳米金刚石中的单个缺陷作为高效的室温单光子源,以揭示固态量子发射体中偶极子取向的起源和时间演化。通过实验确定了激发和发射偶极子相对于晶体轴的角度,然后使用密度泛函理论进行计算,得出了每个特定缺陷的特征角度,这些角度可作为缺陷识别和理解其原子结构的有效工具。此外,时间偏振动力学揭示了强烈改变的线性偏振可见度,这取决于单个激发的激发态衰变时间。这种效应可能追溯到局部晶体环境中多余电荷的激发。理解这种隐藏的时间相关机制可以进一步提高偏振敏感实验的性能,特别是与单光子发射体进行量子通信的实验性能。