论文标题

波长可启动开放双微腔,以增强两个紧密间隔的光学转变

Wavelength-tunable open double-microcavity to enhance two closely spaced optical transitions

论文作者

Seyfferle, Simon, Herzog, Thomas, Sittig, Robert, Jetter, Michael, Portalupi, Simone Luca, Michler, Peter

论文摘要

长期以来,由于其有用性增强光萃取和轻度 - 物质相互作用,因此长期以来一直认为量子光子研究中的必不可少元素。常规的高Q腔结构通常只允许单个光学转换以特定模式调节到共振中。但是,向更先进的双腔结构的过渡引入了新的有趣的可能性,例如同时使用两种不同的空腔模式同时增强了两个频谱接近光学的转变。在这里,我们研究了一个由两个半导体分布的布拉格反射器(DBR)和沉积在纤维尖端上的顶部介电镜之间的整体平面腔组成的空腔结构。虽然底部腔是由两个DBR形成的,但纤维尖端上的镜子和半导体芯片的顶部DBR会产生第二个可调腔。这些耦合的腔体在调节共振时表现出模式杂交,并且可以调整它们的分裂,以通过合适的样品设计与紧密间隔的光学跃迁的光谱分离匹配。此外,我们报告了半导体量子点的激子和Biexciton跃迁的同时共振调节,每个量子均以开放纤维的双腔的单独模式。同时共振的衰减时间测量表明,p_p^x $ = 1.9 $ \ pm $ 0.4 $ f_p^x $ 0.4。

Microcavities have long been recognized as indispensable elements in quantum photonic research due to their usefulness for enhanced light extraction and light-matter interaction. A conventional high-Q cavity structure typically allows only a single optical transition to be tuned into resonance with a specific mode. The transition to a more advanced double-cavity structure, however, introduces new and interesting possibilities such as enhancing two spectrally close optical transitions at the same time with two distinct cavity modes. Here, we investigate a cavity structure composed of a monolithic planar cavity enclosed between two semiconductor distributed Bragg reflectors (DBR) and a top dielectric mirror deposited on a fiber tip. While the bottom cavity is formed by the two DBRs, the mirror on the fiber tip and the top DBR of the semiconductor chip create a second tunable cavity. These coupled cavities exhibit mode hybridization when tuned into resonance and their splitting can be adjusted to match with the spectral separation of closely spaced optical transitions by a suitable sample design. Furthermore, we report on the simultaneous resonance tuning of the exciton and biexciton transition of a semiconductor quantum dot, each to a separate mode of the open fiber-based double cavity. Decay time measurements at simultaneous resonance showed a Purcell-factor of $F_P^X$=1.9$\pm$0.4 for the exciton transition.

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