Svetlana S. Aleshkina

Dr. Svetlana S. Aleshkina

Dianov Fiber Optics Research Center, Prokhorov General Physics Institute of the Russian Academy of Sciences, 38 Vavilov Street, 119333 Moscow, Russia
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Research Focus & Metrics

Academic Career Length

17Years (2010-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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20 October 2017 in Optics Express
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KBKonstantin Bobkov
Konstantin Bobkov
AAAlexey Andrianov
Alexey Andrianov
MKMaxim Koptev
Maxim Koptev
SMSergey Muravyev
Sergey Muravyev
ALAndrei Levchenko
Andrei Levchenko
MLMikhail E. Likhachev
Mikhail E. Likhachev
We demonstrate a novel amplification regime in a counter-pumped, relatively long (2 meters), large mode area, highly Yb-doped and polarization-maintaining tapered fiber, which offers a high peak power directly from the amplifier. The main feature of this regime is that the amplifying signal propagates through a thin part of the tapered fiber without amplification and experiences an extremely high gain in the thick part of the tapered fiber, where most of the pump power is absorbed. In this regime, we have demonstrated 8 ps pulse amplification to a peak power of up to 0.76 MW, which is limited by appearance of stimulated Raman scattering. In the same regime, 28 ps chirped pulses are amplified to a peak power of 0.35 MW directly from the amplifier and then compressed with 70% efficiency to 315 ± 10 fs, corresponding to an estimated peak power of 22 MW.

11 March 2021 in Optics Express
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Journal Article
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ZMZe-Long Ma
Ze-Long Ma
JLJin-Gan Long
Jin-Gan Long
WLWei Lin
Wei Lin
WHWeiyi Hong
Weiyi Hong
HCHu Cui
Hu Cui
Ai-Ping LuoAi-Ping Luo
Ai-Ping Luo
We report the spatiotemporal mode-locked multimode fiber laser operating at 1.55 µm based on semiconductor saturable absorber mirrors with the mode-locking threshold as low as 104 mW. Benefiting from the multimode interference filtering effect introduced in the laser cavity not only the central wavelength can be continuously tuned from 1557 nm to 1567 nm, but also the number of the output pulses can be adjusted from 1 to 4 by simply adjusting the polarization controllers. This work provides a new platform for exploring the dynamic characteristics of spatiotemporal mode-locked pulses at negative dispersion regime. Moreover, this kind of tunable laser has potential applications in fields of all-optical signal processing, fiber sensing and information coding.

29 November 2017 in IEEE Photonics Technology Letters
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Svetlana S. AleshkinaSvetlana S. Aleshkina
Svetlana S. Aleshkina
ALAndrei E. Levchenko
Andrei E. Levchenko
OMOleg I. Medvedkov
Oleg I. Medvedkov
KBKonstantin K. Bobkov
Konstantin K. Bobkov
MBMikhail M. Bubnov
Mikhail M. Bubnov
MLMikhail E. Likhachev
Mikhail E. Likhachev
We propose a novel saddle-shaped Yb-doped fiber design for high power generation in the spectral range near 0.976 μm. The fiber has a central single-mode part with a core diameter of approximately 12 μm and an ultra-thin silica clad of approximately 49 μm. At both ends of the fiber, the core/clad diameters were adiabatically increased up to 20/80 μm to be compatible with ordinary passive fibers. A monolithic 976-nm single-mode continuous wave laser based on the proposed fiber was created. The laser’s power was a record high compared to all-fiber laser schemes, with an output power of 10.6 W. Utilization of a photodarkening-free core glass matrix has allowed us to demonstrate perfect long-term stability (without any power degradation) of the developed laser over 45 hours.

25 June 2010 in Optics Letters
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DGD. A. Gaponov
D. A. Gaponov
SFS. Février
S. Février
MDM. Devautour
M. Devautour
PRP. Roy
P. Roy
MLM. E. Likhachev
M. E. Likhachev
AGA. N. Guryanov
A. N. Guryanov
Very large-mode-area Yb3+-doped single-mode photonic bandgap (PBG) Bragg fiber oscillators are considered. The transverse hole-burning effect is numerically modeled, which helps properly design the PBG cladding and the Yb3+-doped region for the high-order mode content to be carefully controlled. A ratio of the Yb3+-doped region diameter to the overall core diameter of 40% allows for single-mode emission, even for small spool diameters of 15cm. Such a fiber was manufactured and subsequently used as the core element of a cw oscillator. Very good beam quality parameter M2=1.12 and slope efficiency of 80% were measured. Insensitivity to bending, exemplified by the absence of temporal drift of the beam, was demonstrated for curvature diameter as small as 15cm.

11 January 2021 in Optics Express
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KBKonstantin Bobkov
Konstantin Bobkov
ALAndrey Levchenko
Andrey Levchenko
TKTatiana Kashaykina
Tatiana Kashaykina
Svetlana S. AleshkinaSvetlana S. Aleshkina
Svetlana S. Aleshkina
MBMikhail Bubnov
Mikhail Bubnov
MLMikhail E. Likhachev
Mikhail E. Likhachev
Prospects for average power scaling of sub-MW output peak power picosecond fiber lasers by utilization of a Yb-doped tapered fiber at the final amplification stage were studied. In this paper, it was shown experimentally that a tapered fiber allows the achievement of an average power level of 150 W (limited by the available pump power) with a peak power of 0.74 MW for 22 ps pulses with no signs of transverse mode instability. Measurements of the mode content using the S2 technique showed a negligible level of high order modes (less than 0.3%) in the output radiation even for the maximum output power level. Our reliability tests predict no thermal issues during long-term operation (105 hours) of the developed tapered fiber laser up to kilowatt output average power levels.

9 September 2011 in Optics Letters
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Svetlana S. AleshkinaSvetlana S. Aleshkina
Svetlana S. Aleshkina
MLMikhail E. Likhachev
Mikhail E. Likhachev
APAndrey D. Pryamikov
Andrey D. Pryamikov
DGDmitry A. Gaponov
Dmitry A. Gaponov
ADAlexander Denisov
Alexander Denisov
SFSébastien Février
Sébastien Février
A design of a polarizing all-glass Bragg fiber with a microstructure core has been proposed for the first time. This design provides suppression of high-order modes and of one of the polarization states of the fundamental mode. The polarizing fiber was fabricated by a new, simple method based on a combination of the modified chemical vapor deposition (MCVD) process and the rod-in-tube technique. The mode field area has been found to be about 870 μm2 near λ=1064 nm. The polarization extinction ratio better than 13 dB has been observed over a 33% wavelength range (from 1 to 1.4 μm) after propagation in a 1.7 m fiber piece bent to a radius of 70 cm.