Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber

被引:1
|
作者
Haris, Hazlihan [1 ]
Jin, Tan Sin [2 ,3 ]
Batumalay, Malathy [4 ]
Muhammad, Ahmad Razif [5 ]
Sampe, Jahariah [5 ]
Markom, Arni Munira [6 ]
Zain, Huda Adnan [7 ]
Harun, Sulaiman Wadi [7 ]
Hasnan, Megat Muhammad Ikhsan Megat [1 ]
Saad, Ismail [1 ]
机构
[1] Univ Malaysia Sabah UMS, Fac Engn, Kota Kinabalu 88400, Sabah, Malaysia
[2] KDU Univ Coll, Sch Engn, UOW Malaysia, Shah Alam 40150, Selangor, Malaysia
[3] KDU Univ Coll, UOW Malaysia, George Town 10400, Pulau Pinang, Malaysia
[4] INTI Int Univ, Fac Data Sci & IT, Nilai 71800, Negeri Sembilan, Malaysia
[5] Univ Kebangsaan Malaysia, Inst Microengn & Nanoelect IMEN, Bangi 43600, Selangor, Malaysia
[6] Univ Teknol MARA, Coll Engn, Sch Elect Engn, Shah Alam 40450, Selangor, Malaysia
[7] Univ Malaya, Fac Engn, Dept Elect Engn, Kuala Lumpur 50603, Malaysia
关键词
soliton generation; fiber lasers; bismuth selenide; topological insulator; saturable absorber; WALLED CARBON NANOTUBES; DYNAMIC PATTERNS; PULSE GENERATION; SIDE-BAND; FEMTOSECOND; WAVELENGTH;
D O I
10.3390/nano13091538
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
In this work, we present the generation of two distinct types of soliton pulses using a Bismuth Selenide (Bi2Se3) saturable absorber (SA) synthesized in our laboratory. The soliton pulses were generated in two different laser cavity configurations, resulting in two types of solitons: a soliton pulse with Kelly sidebands and a bunched soliton pulse with peak-dip sidebands. Both solitons operated at the fundamental repetition rate-23.3 MHz (for the soliton with Kelly sidebands) and 13 MHz (for the bunched soliton with peak-dip sidebands). We observed that the accumulation of nonlinear phase shift from the added single mode fiber (SMF) split the single soliton pulse into 44 pulses in a bunched oscillation envelope. At the same time, peak-dip sidebands were imposed on the bunched soliton spectrum due to constructive and destructive interferences between soliton pulse and dispersive waves. The measured pulse width for both solitons were 0.63 ps (for the soliton with Kelly sidebands) and 1.52 ps (for the bunched soliton with peak-dip sidebands), respectively. Our results demonstrate the potential of Bi2Se3 SAs in generating different types of soliton pulses, which could have potential applications in various areas of optical communication and spectroscopy.
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页数:9
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