1.Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, Guangzhou 511442, China
2.Microwave Photonics Research Laboratory, School of Electrical Engineering and Computer Science, University of Ottawa, Ottawa, ON K1N 6N5, Canada
Jiejun Zhang (zhangjiejun@jnu.edu.cn)
Jianping Yao (jpyao@uottawa.ca)
纸质出版日期:2020,
网络出版日期:2020-09-27,
收稿日期:2020-07-30,
修回日期:2020-09-09,
录用日期:2020-09-10
Scan QR Code
Polarimetric parity-time symmetry in a photonic system[J]. LSA, 2020,9(5):1630-1637.
Li, L. Z. et al. Polarimetric parity-time symmetry in a photonic system. Light: Science & Applications, 9, 1630-1637 (2020).
Polarimetric parity-time symmetry in a photonic system[J]. LSA, 2020,9(5):1630-1637. DOI: 10.1038/s41377-020-00407-3.
Li, L. Z. et al. Polarimetric parity-time symmetry in a photonic system. Light: Science & Applications, 9, 1630-1637 (2020). DOI: 10.1038/s41377-020-00407-3.
Parity-time (PT) symmetry has attracted intensive research interest in recent years. PT symmetry is conventionally implemented between two spatially distributed subspaces with identical localized eigenfrequencies and complementary gain and loss coefficients. The implementation is complicated. In this paper
we propose and demonstrate that PT symmetry can be implemented between two subspaces in a single spatial unit based on optical polarimetric diversity. By controlling the polarization states of light in the single spatial unit
the localized eigenfrequencies
gain
loss
and coupling coefficients of two polarimetric loops can be tuned
leading to PT symmetry breaking. As a demonstration
a fiber ring laser based on this concept supporting stable and single-mode lasing without using an ultranarrow bandpass filter is implemented.
Regensburger, A. et al. Parity–time synthetic photonic lattices.Nature488, 167–171 (2012)..
Peng, B. et al. Parity–time-symmetric whispering-gallery microcavities.Nat. Phys.10, 394–398 (2014)..
Hodaei, H. et al. Enhanced sensitivity at higher-order exceptional points.Nature548, 187–191 (2017)..
Perez-Leija, A. et al. Coherent quantum transport in photonic lattices.Phys. Rev. A87, 012309 (2013)..
Hodaei, H. et al. Parity-time–symmetric microring lasers.Science346, 975–978 (2014)..
Feng, L. et al. Single-mode laser by parity-time symmetry breaking.Science346, 972–975 (2014)..
Wong, Z. J. et al. Lasing and anti-lasing in a single cavity.Nat. Photon.10, 796–801 (2016)..
Wan, W. J. et al. Time-reversed lasing and interferometric control of absorption.Science331, 889–892 (2011)..
Zhu, X. F. et al. One-way invisible cloak using parity-time symmetric transformation optics.Opt. Lett.38, 2821–2824 (2013)..
Sounas, D. L., Fleury, R.&Alù, A. Unidirectional cloaking based on metasurfaces with balanced loss and gain.Phys. Rev. Appl.4, 014005 (2015)..
El-Ganainy, R. et al. Non-Hermitian physics and PT symmetry.Nat. Phys.14, 11–19 (2018)..
Özdemir, Ş. K. et al. Parity–time symmetry and exceptional points in photonics.Nat. Mater.18, 783–798 (2019)..
Feng, L., El-Ganainy, R.&Ge, L. Non-Hermitian photonics based on parity–time symmetry.Nat. Photon.11, 752–762 (2017)..
Zhang, J. J.&Yao, J. P. Parity-time–symmetric optoelectronic oscillator.Sci. Adv.4, eaar6782 (2018)..
Liu, Y. Z. et al. Observation of parity-time symmetry in microwave photonics.Light Sci. Appl.7, 38 (2018)..
Schawlow, A. L.&Townes, C. H. Infrared and optical masers.Phys. Rev.112, 1940–1949 (1958)..
Beier, F. et al. Narrow linewidth, single mode 3 kW average power from a directly diode pumped ytterbium-doped low NA fiber amplifier.Opt. Express24, 6011–6020 (2016)..
Ma, R. L. et al. Tunable sub-kHz single-mode fiber laser based on a hybrid microbottle resonator.Opt. Letters43, 5315–5318 (2018)..
Mehravar, S. et al. Real-time dual-comb spectroscopy with a free-running bidirectionally mode-locked fiber laser.Appl. Phys. Lett.108, 231104 (2016)..
Quintino, L. et al. Welding with high power fiber lasers–A preliminary study.Mater. Des.28, 1231–1237 (2007)..
Richardson, D. J., Nilsson, J.&Clarkson, W. A. High power fiber lasers: current status and future perspectives [Invited].J. Opt. Soc. Am. B27, B63–B92 (2010)..
Chen, M. et al. Ultra-narrow-linewidth brillouin/erbium fiber laser. CLEO: QELS_Fundamental Science (OSA, San Jose, California, 2017).
Zhou, K. J. et al. kHz-order linewidth controllable 1550 nm single-frequency fiber laser for coherent optical communication.Opt. Express25, 19752–19759 (2017)..
Zhang, J. J. et al. Microfiber Fabry–Perot interferometer fabricated by taper-drawing technique and its application as a radio frequency interrogated refractive index sensor.Opt. Lett.37, 2925–2927 (2012)..
Meng, Z., Stewart, G.&Whitenett, G. Stable single-mode operation of a narrow-linewidth, linearly polarized, erbium-fiber ring laser using a saturable absorber.J. Lightwave Technol.24, 2179–2183 (2006)..
Chen, X. F. et al. Single-longitudinal-mode fiber ring laser employing an equivalent phase-shifted fiber Bragg grating.IEEE Photon. Technol. Lett.17, 1390–1392 (2005)..
Zhang, J. J. et al. Parity-time symmetry in wavelength space within a single spatial resonator.Nat. Commun.11, 3217 (2020)..
Liu, W. L., Wang, M. G.&Yao, J. P. Tunable microwave and sub-terahertz generation based on frequency quadrupling using a single polarization modulator.J. Lightwave Technol.31, 1636–1644 (2013)..
Ulrich, R., Rashleigh, S. C.&Eickhoff, W. Bending-induced birefringence in single-mode fibers.Opt. Lett.5, 273–275 (1980)..
Hui, R. Q.&O'Sullivan, M. Fiber Optic Measurement Techniques (Academic Press, San Diego, 2009).
Viciani, S. et al. Lineshape of a vertical cavity surface emitting laser.Opt. Commun.206, 89–97 (2002)..
Li,Y. H. et al. Photonic generation of W-band arbitrary waveforms with high time-bandwidth products enabling 3.9 mm range resolution.Optica1, 446–454 (2014)..
0
浏览量
0
Downloads
0
CSCD
关联资源
相关文章
相关作者
相关机构
京公网安备11010802024621