A Parity-Time-Symmetric Optoelectronic Oscillator Based on Non-Reciprocal Electro-Optic Modulation

被引:14
作者
Fan, Jinying [1 ]
Li, Lingzhi [1 ]
Zhang, Jiejun [1 ]
Feng, Xinhuan [1 ]
Guan, Bai-Ou [1 ]
Yao, Jianping [1 ,2 ]
机构
[1] Jinan Univ, Inst Photon Technol, Guangdong Prov Key Lab Opt Fiber Sensing & Commun, Guangzhou 511443, Peoples R China
[2] Univ Ottawa, Sch Elect Engn & Comp Sci, Microwave Photon Res Lab, Ottawa, ON K1N 6N5, Canada
基金
中国国家自然科学基金;
关键词
Optical fibers; Optical polarization; Phase modulation; Gain; Microwave filters; Microwave oscillators; Optical variables control; Optoelectronic oscillator; parity-time symmetry; photonic signal generation; traveling-wave modulation; LASER;
D O I
10.1109/JLT.2020.3047697
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
In this paper, we propose and experimentally demonstrate a parity-time- (PT-) symmetric optoelectronic oscillator (OEO) based on non-reciprocal electro-optic modulation for the generation of a microwave signal with a low phase noise. In the proposed OEO, two mutually coupled optoelectronic loops with one having a gain and the other a loss are implemented based on the copropagating and counterpropagating modulation in a traveling-wave electro-optic Mach-Zehnder modulator (MZM), to achieve PT symmetry. Due to the non-reciprocity of the travelling-wave MZM, the modulation indices are different for the copropagating and counterpropagating light waves in relative to the applied microwave signal, which is then interpreted as different microwave round-trip gains for the mutually coupled optoelectronic loops. Once the gain/loss coefficient is greater than the coupling coefficient, the PT symmetry is broken, and single-mode oscillation is achieved. The proposed OEO is experimentally demonstrated. A 10-GHz microwave signal with a phase noise of -110 dBc/Hz at an offset frequency of 10 kHz and a sidemode suppression ratio of 42 dB is generated. The work provides a new solution to overcome the mode selection problem in a long-cavity OEO. Since a single physical loop is employed, the proposed PT-symmetric OEO has the simplest architecture as compared to any existing PT-symmetric OEOs.
引用
收藏
页码:2305 / 2310
页数:6
相关论文
共 27 条
[1]   VELOCITY-MATCHING TECHNIQUES FOR INTEGRATED OPTIC TRAVELING WAVE SWITCH MODULATORS [J].
ALFERNESS, RC ;
KOROTKY, SK ;
MARCATILI, EAJ .
IEEE JOURNAL OF QUANTUM ELECTRONICS, 1984, 20 (03) :301-309
[2]   Introduction to PT-symmetric quantum theory [J].
Bender, CM .
CONTEMPORARY PHYSICS, 2005, 46 (04) :277-292
[3]   Complex extension of quantum mechanics [J].
Bender, CM ;
Brody, DC ;
Jones, HF .
PHYSICAL REVIEW LETTERS, 2002, 89 (27)
[4]   Real spectra in non-Hermitian Hamiltonians having PT symmetry [J].
Bender, CM ;
Boettcher, S .
PHYSICAL REVIEW LETTERS, 1998, 80 (24) :5243-5246
[5]   Reversing the pump dependence of a laser at an exceptional point [J].
Brandstetter, M. ;
Liertzer, M. ;
Deutsch, C. ;
Klang, P. ;
Schoeberl, J. ;
Tuereci, H. E. ;
Strasser, G. ;
Unterrainer, K. ;
Rotter, S. .
NATURE COMMUNICATIONS, 2014, 5
[6]  
Fan Z., 2019, 2019 INT TOPICAL M M, P1
[7]   Single-mode laser by parity-time symmetry breaking [J].
Feng, Liang ;
Wong, Zi Jing ;
Ma, Ren-Min ;
Wang, Yuan ;
Zhang, Xiang .
SCIENCE, 2014, 346 (6212) :972-975
[8]   Nonlinear modal interactions in parity-time (PT) symmetric lasers [J].
Ge, Li ;
El-Ganainy, Ramy .
SCIENTIFIC REPORTS, 2016, 6
[9]   PERFORMANCE AND MODELING OF BROAD-BAND LIBNBO3 TRAVELING-WAVE OPTICAL-INTENSITY MODULATORS [J].
KGOPALAKRISHNAN, GK ;
BURNS, WK ;
MCELHANON, RW ;
BULMER, CH ;
GREENBLATT, AS .
JOURNAL OF LIGHTWAVE TECHNOLOGY, 1994, 12 (10) :1807-1819
[10]   Observation of PT-Symmetry Breaking in Complex Optical Potentials [J].
Guo, A. ;
Salamo, G. J. ;
Duchesne, D. ;
Morandotti, R. ;
Volatier-Ravat, M. ;
Aimez, V. ;
Siviloglou, G. A. ;
Christodoulides, D. N. .
PHYSICAL REVIEW LETTERS, 2009, 103 (09)