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1.
Opt Express ; 27(8): 11510-11515, 2019 Apr 15.
Artigo em Inglês | MEDLINE | ID: mdl-31052994

RESUMO

In this paper, we proposed and numerically demonstrated a novel method to effectively minimize Fresnel reflection from a perpendicularly cleaved fiber using a uniform fiber Bragg grating (FBG) inscribed at the fiber end. By matching the reflectivity of an in-line FBG with the reflectivity caused by the glass-air boundary, the FBG acts as a virtual boundary, which provides destructive interference and suppresses Fresnel reflection. We achieved an anti-reflection FBG with a return loss of more than 80 dB by ensuring that the product of the index contrast and grating period number is almost constant, with a value of 0.2695.

2.
Opt Express ; 23(9): 11205-10, 2015 May 04.
Artigo em Inglês | MEDLINE | ID: mdl-25969216

RESUMO

We propose and demonstrate a passively Q-switched 1900-nm thulium all-fiber laser using the mode-field-area mismatch method. A thulium fiber laser was core-pumped at 1590 nm and saturable-absorber Q-switched at 1900 nm through the use of a thulium saturable absorber fiber that had a relatively smaller mode field area than the gain medium. Sequential pulsing with a pulse energy of 12 µJ and a pulse duration of 160 ns was obtained. The pulse repetition rate was increased linearly with the applied pump power. With a pump power of 4.5 W, an average output power of 0.61 W and a pulse repetition rate of 50.7 kHz were achieved.

3.
Opt Express ; 20(12): 12787-92, 2012 Jun 04.
Artigo em Inglês | MEDLINE | ID: mdl-22714307

RESUMO

We propose and numerically demonstrate a cascade pulsing mechanism in a CW-pumped Er³âº:ZBLAN all-fiber laser system. In the design, the laser was pumped at 980 nm and passively Q-switched at 1.6 µm. The Q-switched resonance reduced the population on 4/13/2 of the erbium gain fiber, thereby creating a population inversion between the levels of 4/11/2 and 4/13/2, and instantly inducing an intense gain-switched pulse at 2.7 µm. Sequential 2.7-µm single-mode pulsing with a pulse energy of 170 µJ and a peak power of 6 kW was achieved with an absorbed pump power of 0.65 W.

4.
Opt Lett ; 37(13): 2610-2, 2012 Jul 01.
Artigo em Inglês | MEDLINE | ID: mdl-22743471

RESUMO

Intense lensless intracavity focusing in a saturable absorber Q-switched all-fiber laser resonator by use of loss arrangement and mode-field-area mismatch between the fibers is investigated for the first time. The intracavity power distribution was related to the locations and values of the cavity losses as the saturable absorption loss, the reflection loss of the output coupler, and the splicing loss between the gain fiber and the absorber fiber. With a mode-field-area mismatch and a reduced splicing loss with the gain fiber, a power density in the absorber fiber was achieved that was 11.9 times higher than that in the gain fiber.

5.
Opt Express ; 18(23): 23523-8, 2010 Nov 08.
Artigo em Inglês | MEDLINE | ID: mdl-21164695

RESUMO

We demonstrate a novel passively pulsed all-Yb3+ all-fiber laser pumped by a continuous-wave 915-nm pump laser diode. The laser was saturable absorber Q-switched at 976 nm and gain-switched at 1064 nm, using the method of mode-field-area mismatch. With a pump power of 105 mW, the laser iteratively produced a 976-nm pulse with an energy of 2.8 µJ and a duration of 280 ns, followed by a 1064-nm pulse with 1.1 µJ and a 430-ns duration at a repetition rate of 9 kHz. A set of rate equations was established to simulate the self-balancing mechanism and the correlation between the Q- and gain-switched photon numbers and the populations of the gain and absorber fibers.

6.
Opt Lett ; 34(19): 2891-3, 2009 Oct 01.
Artigo em Inglês | MEDLINE | ID: mdl-19794758

RESUMO

We propose and demonstrate an all-fiber self-Q-switched erbium laser system that is saturable-absorber Q switched by the mismatch of the mode-field areas in the resonator and stabilized with a saturable-amplifier pump switch. Sequential pulses with a pulse energy of 8-6 microJ and a pulse duration of 80-320 ns, corresponding to a pulse repetition rate of 0.25-1 kHz, were obtained using a cw 980 nm laser-diode pump. A peak pulse power of near 100 W was achieved.

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