Pulsed all-fiber gas Raman laser oscillator based on hollow-core photonic crystal fibers

2021 ◽  
Author(s):  
Hao Li ◽  
Wenxi Pei ◽  
Wei Huang ◽  
Zefeng Wang
2020 ◽  
Vol 132 ◽  
pp. 106474
Author(s):  
Hao Li ◽  
Wei Huang ◽  
Yulong Cui ◽  
Zhiyue Zhou ◽  
Zefeng Wang

Photonics ◽  
2021 ◽  
Vol 8 (9) ◽  
pp. 382
Author(s):  
Wenxi Pei ◽  
Hao Li ◽  
Wei Huang ◽  
Meng Wang ◽  
Zefeng Wang

We report here an all-fiber structure tunable gas Raman laser based on deuterium-filled hollow-core photonic crystal fibers (HC-PCFs). An all-fiber gas cavity is fabricated by fusion splicing a 49 m high-pressure deuterium-filled HC-PCF with two solid-core single-mode fibers at both ends. When pumped with a pulsed fiber amplifier seeded by a tunable laser diode at 1.5 μm, Raman lasers ranging from 1643 nm to 1656 nm are generated. The maximum output power is ~1.2 W with a Raman conversion efficiency of ~45.6% inside the cavity. This work offers an alternative choice for all-fiber lasers operating at 1.6–1.7 μm band.


Sensors ◽  
2021 ◽  
Vol 21 (1) ◽  
pp. 284
Author(s):  
Bowei Wan ◽  
Lianqing Zhu ◽  
Xin Ma ◽  
Tianshu Li ◽  
Jian Zhang

Due to their flexible structure and excellent optical characteristics hollow-core photonic crystal fibers (HC-PCFs) are used in many fields, such as active optical devices, communications, and optical fiber sensing. In this paper, to analyze the characteristics of HC-PCFs, we carried out finite element analysis and analyzed the design for the band gap cladding structure of HC-PCFs. First, the characteristics of HC19-1550 and HC-1550-02 in the C-band were simulated. Subsequently, the structural optimization of the seven-cell HC-1550-02 and variations in characteristics of the optimized HC-1550-02 in the wavelength range 1250–1850 nm were investigated. The simulation results revealed that the optimal number of cladding layers is eight, the optimal core radius is 1.8 times the spacing of adjacent air holes, and the optimal-relative thickness of the core quartz-ring is 2.0. In addition, the low confinement loss bandwidth of the optimized structure is 225 nm. Under the transmission bandwidth of the optimized structure, the core optical power is above 98%, the confinement loss is below 9.0 × 10−3 dB/m, the variation range of the effective mode field area does not exceed 10 μm2, and the relative sensitivity is above 0.9570. The designed sensor exhibits an ultra-high relative sensitivity and almost zero confinement loss, making it highly suitable for high-sensitivity gas or liquid sensing.


2009 ◽  
Vol 17 (26) ◽  
pp. 23468 ◽  
Author(s):  
J. K. Lyngsø ◽  
B. J. Mangan ◽  
C. Jakobsen ◽  
P. J. Roberts

2015 ◽  
Vol 23 (9) ◽  
pp. 11227 ◽  
Author(s):  
Marco Triches ◽  
Mattia Michieletto ◽  
Jan Hald ◽  
Jens K. Lyngsø ◽  
Jesper Lægsgaard ◽  
...  

2021 ◽  
Vol 29 (9) ◽  
pp. 13787
Author(s):  
Jie Luan ◽  
Philip St.J. Russell ◽  
David Novoa

Sign in / Sign up

Export Citation Format

Share Document