Ekaterina Mitina

Ms. Ekaterina Mitina


Research Focus & Metrics

Academic Career Length

6Years (2021-Present)

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

Representative Publications

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23 November 2021 in Laser Physics Letters
Verified
Journal Article
Closed access
EMEkaterina Mitina
Ekaterina Mitina
DUD Uryupina
D Uryupina
NZN Zhidovtsev
N Zhidovtsev
RVR Volkov
R Volkov
OKO Kosareva
O Kosareva
ASA Savel’eV
A Savel’eV
Multiple filament’s formation on a long atmospheric path was studied for an amplitude modulation of the terawatt femtosecond beam with the four and six hole masks. Filaments appeared at the distance that is determined by the Fresnel lens formed by a hole, not by the self focusing theory for the unrestricted (Gaussian like) beam. This lens focuses 1/3 of the energy passing through the hole to the beam spot ≈1 mm in diameter. The robust multifilament array 10–15 m in length was observed if the energy per hole was ≈1-1.5 mJ (pulse duration 50 fs), while each hole produces bundle of a few filaments at higher energies.

7 December 2022 in Optics & Laser Technology
Verified
Journal Article
Closed access
EMEkaterina Mitina
Ekaterina Mitina
DUD. Uryupina
D. Uryupina
INI. Nikolaeva
I. Nikolaeva
DSDaniil Shipilo
Daniil Shipilo
NPN. Panov
N. Panov
ASA. Savel’eV
A. Savel’eV

12 August 2023 in Photonics
Verified
Journal Article
Open access
PDF file
EMEkaterina Mitina
Ekaterina Mitina
DUDaria Uryupina
Daria Uryupina
DSDaniil Shipilo
Daniil Shipilo
INIrina Nikolaeva
Irina Nikolaeva
NPNikolay Panov
Nikolay Panov
ASAndrei Savel'ev
Andrei Savel'ev
Focused femtosecond beam filamentation after amplitude masks has been studied experimentally and numerically. We deduced conditions (energy per hole, diameter and geometrical composition of holes, focal length) providing for the formation of the regularized bundle of filaments or single on-axis filament at the given pulse duration and beam diameter. We showed that a light channel with small diameter (∼200 μm) and overcritical peak power may be formed well before both the focal distance and the Marburger length, and this channel collapses due to self-focusing and forms the filament. The start position of such a filament can be predicted based on the linear propagation equation, while a more sophisticated non-linear approach that takes into account the Kerr nonlinearity, plasma effects, etc., helps to describe the temporal structure of a filament, its frequency, and its angular spectrum.