Antony Kuruvilla
Raja Ramanna Centre for Advanced Technology
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Featured researches published by Antony Kuruvilla.
Applied Optics | 2010
B.N. Upadhyaya; Antony Kuruvilla; U. Chakravarty; M. R. Shenoy; K. Thyagarajan; S. M. Oak
We report an experimental study of the effect of fiber length and laser linewidth on self-pulsing dynamics and output stabilization of a single-mode Yb-doped double-clad CW fiber laser. It is found that initiation of self-pulsing under low-level pumping conditions is due to relaxation oscillations and saturable absorption in the weakly pumped region of the doped fiber, irrespective of the fiber length and the laser linewidth. However, with an increase in pump power, depending on fiber length and laser linewidth, the pulses initiated due to relaxation oscillation get amplified, and result in short-duration giant pulses due to either stimulated Brillouin scattering (SBS) or stimulated Raman scattering (SRS). In the case of fiber lasers that employ a broadband mirror and wherein the fiber length is sufficient to reach the SRS threshold, the giant self-pulses are generated by SRS, whereas in the case of fiber lasers using a fiber Bragg grating, characterized by narrowband reflection and with sufficient fiber length to reach the SBS threshold, the giant self-pulses are generated by SBS. Output stabilization and, hence, elimination of self-pulsations can be achieved either by suppressing the relaxation oscillations with the addition of an appropriate length of a passive fiber to sufficiently increase the cavity photon lifetime, or by increasing the pump power to achieve gain uniformity along the doped fiber such that relaxation oscillations and reabsorption effects are suppressed.
Optics Express | 2007
B.N. Upadhyaya; U. Chakravarty; Antony Kuruvilla; K. Thyagarajan; M. R. Shenoy; S. M. Oak
The output pulse characteristics of Q-switched Yb-doped fiber lasers have been investigated experimentally. It has been observed that for any typical modulation frequency, the pump power and the modulator OFF-time govern the shape of the output Q-switched pulse. At a fixed modulation frequency, with a fine adjustment of acousto-optic modulation window ON-time, pump power and cavity mirror position, it was possible to obtain modulation free single-peak pulse, multi-peak pulse, mode-locked resembling pulse and multi-pulse structured pulse shapes in a Q-switched fiber laser output. These observations have been analyzed and explained. Our investigations show that multi-peak pulse output is due to onset of nonlinear phenomena like SBS and SRS. Similarly, we have found that the mode-locked resembling periodically modulated output pulse shape is due to mode beating between the zeroeth order and the first order diffracted beams of the intra-cavity acousto-optic Q-switch.
Applied Optics | 2017
U. Chakravarty; P. K. Mukhopadhyay; Antony Kuruvilla; B.N. Upadhyaya; K. S. Bindra
A narrow-linewidth broadly tunable Yb-doped Q-switched fiber laser using an acousto-optic modulator and multimode interference filter (MMIF) in the linear bulk cavity resonator and an all-fiber ring cavity resonator has been demonstrated. Insertion of an MMIF in the linear cavity resonator using bulk components decreased the spectral bandwidth of the Q-switched signal by two orders of magnitude from 11 to less than 0.1 nm. Spectral tunability of more than 16 nm in the range from 1057 to 1073 nm has also been achieved by the combination of MMIF and a standard polarization controller (SPC). A decrease in the pulse duration with a decrease in the spectral bandwidth of the output signal has also been recorded. The pulse duration of the Q-switched signal was reduced from ∼305 to ∼240 ns by the introduction of the MMIF in the resonator at the same value of the input pump power. In the case of the all-fiber Q-switched ring cavity resonator, the spectral bandwidth of the Q-switched signal was reduced by two orders of magnitude from ∼17 to less than 0.1 nm due to the introduction of the MMIF in the resonator. The spectral tunability of more than 12 nm in the range from 1038 to 1050 nm was achieved by an MMIF and an SPC.
Applied Optics | 2016
U. Chakravarty; Antony Kuruvilla; R. P. Singh; B.N. Upadhyaya; K. S. Bindra; S. M. Oak
We report on the generation of 41.6 W of average output power from a passively Q-switched ytterbium-doped fiber laser using Cr4+:YAG crystal as a saturable absorber (SA). This is the highest average power from passively Q-switched fiber lasers reported so far in the literature, to our knowledge, and it has been achieved by using a specially designed T-type double-end pumping configuration. Variation in average output power, pulse energy, pulse duration, pulse frequency, and pulse-to-pulse stability has also been studied using SAs of different linear transmissions. The effect of an intracavity SA on self-pulsing dynamics was also investigated and it was observed that, at lower input pump power near threshold, the presence of an SA enhances the peak power of relaxation oscillations to trigger the generation of stimulated Raman scattering in the gain fiber. With an increase in pump power, when the passive Q-switching threshold is reached, high peak power random self-pulses regenerate into low amplitude regular Q-switched pulses. The effect of the length of the gain medium on dual-wavelength generation at very low input pump power and broadband generation at sufficiently higher pump power has also been explored.
Optics Communications | 2010
B.N. Upadhyaya; U. Chakravarty; Antony Kuruvilla; S. M. Oak; M. R. Shenoy; K. Thyagarajan
Optics Communications | 2008
B.N. Upadhyaya; U. Chakravarty; Antony Kuruvilla; A. K. Nath; M. R. Shenoy; K. Thyagarajan
Optics and Laser Technology | 2013
U. Chakravarty; Antony Kuruvilla; H. Harikrishnan; B.N. Upadhyaya; K. S. Bindra; S. M. Oak
Laser Physics | 2017
Srikanth Gurram; Antony Kuruvilla; Rajpal Singh; K. S. Bindra
Pramana | 2014
U. Chakravarty; Antony Kuruvilla; Rajpal Singh; B N Upadhyay; K. S. Bindra; S. M. Oak
Optics and Laser Technology | 2019
U. Chakravarty; Srikanth Gurram; Antony Kuruvilla; B.N. Upadhyaya; K. S. Bindra