Polarization shaping of Poincare beams by polariton oscillations

被引:46
作者
Colas, David [1 ]
Dominici, Lorenzo [2 ,3 ]
Donati, Stefano [2 ,3 ,4 ]
Pervishko, Anastasiia A. [5 ]
Liew, Timothy C. H. [5 ]
Shelykh, Ivan A. [5 ,6 ,7 ]
Ballarini, Dario [2 ]
de Giorgi, Milena [2 ]
Bramati, Alberto [8 ]
Gigli, Giuseppe [2 ,4 ]
del Valle, Elena [1 ]
Laussy, Fabrice P. [1 ,9 ]
Kavokin, Alexey V. [9 ,10 ]
Sanvitto, Daniele [2 ]
机构
[1] Univ Autonoma Madrid, Dept Fis Teor, Mat Condensada & Condensed Matter Phys Ctr IFIMAC, E-28049 Madrid, Spain
[2] CNR, Ist Nanotecnol, NANOTEC, I-73100 Lecce, Italy
[3] IIT Lecce, Ist Italiano Tecnol, I-73010 Lecce, Italy
[4] Univ Salento, I-73100 Lecce, Italy
[5] Nanyang Technol Univ, Div Phys & Appl Phys, Singapore 637371, Singapore
[6] Univ Iceland, Inst Sci, IS-107 Reykjavik, Iceland
[7] ITMO Univ, Lab Light Matter Coupling Nanostruct, St Petersburg 197101, Russia
[8] Univ Paris 06, Lab Kastler Brossel, F-75005 Paris, France
[9] Russian Quantum Ctr, Skolkovo 143025, Moscow Region, Russia
[10] CNR SPIN, I-00133 Rome, Italy
基金
欧洲研究理事会;
关键词
full Poincare beams; polaritons; polarization; pulse shaping; Rabi oscillations; RABI OSCILLATIONS; PULSE;
D O I
10.1038/lsa.2015.123
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We propose theoretically and demonstrate experimentally the generation of light pulses whose polarization varies temporally to cover selected areas of the Poincare sphere with both tunable swirling speed and total duration (1 ps and 10 ps, respectively, in our implementation). The effect relies on the Rabi oscillations of two polariton polarized fields excited by two counter-polarized and delayed pulses. The superposition of the oscillating fields result in the precession of the Stokes vector of the emitted light while polariton lifetime imbalance results in its drift from a circle of controllable radius on the Poincare sphere to a single point at long times. The positioning of the initial circle and final point allows to engineer the type of polarization spanning, including a full sweeping of the Poincare sphere. The universality and simplicity of the scheme should allow for the deployment of time-varying full-Poincare polarization fields in a variety of platforms, timescales, and regimes.
引用
收藏
页码:e350 / e350
页数:7
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