Polarized and Unpolarized Emission from a Single Emitter in a Bullseye Resonator

被引:1
|
作者
Peniakov, Giora [1 ]
Buchinger, Quirin [1 ]
Helal, Mohamed [1 ]
Betzold, Simon [1 ]
Reum, Yorick [1 ]
Rota, Michele B. [2 ]
Ronco, Giuseppe [2 ]
Beccaceci, Mattia [2 ]
Krieger, Tobias M. [3 ]
da Silva, Saimon F. Covre [3 ]
Rastelli, Armando [3 ]
Trotta, Rinaldo [2 ]
Pfenning, Andreas [1 ]
Hoefling, Sven [1 ]
Huber-Loyola, Tobias [1 ]
机构
[1] Julius Maximilians Univ Wurzburg, Phys Inst, Lehrstuhl Tech Phys, D-97074 Wurzburg, Germany
[2] Sapienza Univ Rome, Dept Phys, Piazzale Aldo Moro 5, I-00185 Rome, Italy
[3] Johannes Kepler Univ Linz, Inst Semicond & Solid State Phys, Altenberger Str 69, A-4040 Linz, Austria
基金
奥地利科学基金会;
关键词
bullseye microcavities; circular Bragg grating microcavities; polarization; semiconductor quantum dots; single-photon emitters; QUANTUM-DOT SPIN; PHOTON; ENTANGLEMENT; STATE;
D O I
10.1002/lpor.202300835
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Polarized |S| = 0.99 +/- 0.01, and unpolarized |S| = 0.03 +/- 0.01 emission from a single emitter embedded in a single, cylindrically symmetric device design is presented. The polarization stems from a position offset of the single emitter with respect to the cavity center, which breaks the cylindrical symmetry, and a position-dependent coupling to the frequency degenerate eigenmodes of the resonator structure is shown. The experimental results are interpreted by using numerical simulations and by experimental mapping of the polarization-resolved far-field emission patterns. The findings can be generalized to any nanophotonic structure where two orthogonal eigenmodes are not fully spatially overlapping.
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页数:7
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