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Dive into the research topics where Antony Kuruvilla is active.

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Featured researches published by Antony Kuruvilla.


Applied Optics | 2010

Effect of laser linewidth and fiber length on self-pulsing dynamics and output stabilization of single-mode Yb-doped double-clad fiber laser

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

Mechanisms of generation of multi-peak and mode-locked resembling pulses in Q-switched Yb-doped fiber lasers.

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

Narrow-linewidth broadly tunable Yb-doped Q-switched fiber laser using multimode interference filter

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

Generation of more than 40 W of average output power from a passively Q-switched Yb-doped fiber laser.

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

Self-pulsing characteristics of a high-power single transverse mode Yb-doped CW fiber laser

B.N. Upadhyaya; U. Chakravarty; Antony Kuruvilla; S. M. Oak; M. R. Shenoy; K. Thyagarajan


Optics Communications | 2008

Effect of steady-state conditions on self-pulsing characteristics of Yb-doped cw fiber lasers

B.N. Upadhyaya; U. Chakravarty; Antony Kuruvilla; A. K. Nath; M. R. Shenoy; K. Thyagarajan


Optics and Laser Technology | 2013

Study on self-pulsing dynamics in Yb-doped photonic crystal fiber laser

U. Chakravarty; Antony Kuruvilla; H. Harikrishnan; B.N. Upadhyaya; K. S. Bindra; S. M. Oak


Laser Physics | 2017

Generation of 6.8 W of CW output power at 1550 nm using small mode field diameter Er:Yb co-doped double clad fiber in laser oscillator configuration

Srikanth Gurram; Antony Kuruvilla; Rajpal Singh; K. S. Bindra


Pramana | 2014

Linearly polarized intracavity passive Q-switched Yb-doped photonic crystal fibre laser

U. Chakravarty; Antony Kuruvilla; Rajpal Singh; B N Upadhyay; K. S. Bindra; S. M. Oak


Optics and Laser Technology | 2019

Short pulse generation in active Q-switched Yb-doped all fiber laser and its amplification

U. Chakravarty; Srikanth Gurram; Antony Kuruvilla; B.N. Upadhyaya; K. S. Bindra

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B.N. Upadhyaya

Raja Ramanna Centre for Advanced Technology

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S. M. Oak

Raja Ramanna Centre for Advanced Technology

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U. Chakravarty

Raja Ramanna Centre for Advanced Technology

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K. S. Bindra

Raja Ramanna Centre for Advanced Technology

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K. Thyagarajan

Indian Institute of Technology Delhi

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M. R. Shenoy

Indian Institute of Technology Delhi

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Rajpal Singh

Raja Ramanna Centre for Advanced Technology

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Srikanth Gurram

Raja Ramanna Centre for Advanced Technology

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B N Upadhyay

Raja Ramanna Centre for Advanced Technology

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Pushkar Misra

Raja Ramanna Centre for Advanced Technology

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