Andrey Veniaminov

Dr. Andrey Veniaminov

ITMO University, St Petersburg, Russia
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Research Focus & Metrics

Academic Career Length

41Years (1986-Present)

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

Representative Publications

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10 December 2013 in Optics and Spectroscopy
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Andrey VeniaminovAndrey Veniaminov
Andrey Veniaminov
UMU. V. Mahilny
U. V. Mahilny
We present a review of information that has been published in the scientific literature on the mechanism of formation (development, enhancement) of holograms at the expense of the photochemical...

23 May 2002 in Journal of Optics A: Pure and Applied Optics
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Andrey VeniaminovAndrey Veniaminov
Andrey Veniaminov
EBEckhard Bartsch
Eckhard Bartsch
As a further development of the manufacture of holographic gratings by the diffusion of phenanthrenequinone in polymer glass, the traditionally employed poly(methyl methacrylate) is replaced by poly(bisphenol-A-carbonate). The post-exposure growth and decay of the gratings in the two materials are compared at different spatial periods and temperatures. The medium with polycarbonate demonstrates a fortunate combination of significantly improved stability of the gratings and their faster development. Our results indicate that the polycarbonate materials promise to be suitable media for holographic optical elements and data storage.

26 September 2018 in Photonics Research
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EKEsrom Kifle
Esrom Kifle
PLPavel Loiko
Pavel Loiko
JAJavier Vazquez de Aldana
Javier Vazquez de Aldana
CRCarolina Romero
Carolina Romero
Airan RodenasAiran Rodenas
Airan Rodenas
XFXavier Mateos Ferré
Xavier Mateos Ferré
Surface channel waveguides (WGs) were fabricated in a monoclinic Tm3+:KLu(WO4)2 crystal by femtosecond direct laser writing (fs-DLW). The WGs consisted of a half-ring cladding with diameters of 50 and 60 μm located just beneath the crystal surface. They were characterized by confocal laser microscopy and μ-Raman spectroscopy, indicating a reduced crystallinity and stress-induced birefringence of the WG cladding. In continuous-wave (CW) mode, under Ti:sapphire laser pumping at 802 nm, the maximum output power reached 171.1 mW at 1847.4 nm, corresponding to a slope efficiency η of 37.8% for the 60 μm diameter WG. The WG propagation loss was 0.7±0.3  dB/cm. The top surface of the WGs was spin-coated by a polymethyl methacrylate film containing randomly oriented (spaghetti-like) arc-discharge single-walled carbon nanotubes serving as a saturable absorber based on evanescent field coupling. Stable passively Q-switched (PQS) operation was achieved. The PQS 60 μm diameter WG laser generated a record output power of 150 mW at 1846.8 nm with η=34.6%. The conversion efficiency with respect to the CW mode was 87.6%. The best pulse characteristics (energy/duration) were 105.6 nJ/98 ns at a repetition rate of 1.42 MHz.

1 November 2005 in Optics and Spectroscopy
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Andrey VeniaminovAndrey Veniaminov
Andrey Veniaminov
EBE. Bartsch
E. Bartsch
Alexey PopovAlexey Popov
Alexey Popov
The specific features of the postexposure evolution of photoinduced (holographic) gratings in a model medium that consists of poly(methyl methacrylate) with distributed phenanthrenequinone and is...

11 March 2019 in Optics Express
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Journal Article
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EKEsrom Kifle
Esrom Kifle
PLPavel Loiko
Pavel Loiko
JAJavier Vazquez de Aldana
Javier Vazquez de Aldana
CRCarolina Romero
Carolina Romero
Airan RodenasAiran Rodenas
Airan Rodenas
XFXavier Mateos Ferré
Xavier Mateos Ferré
We report the generation of mid-infrared (~2 µm) high repetition rate (MHz) sub-100 ns pulses in buried thulium-doped monoclinic double tungstate crystalline waveguide lasers using two-dimensional saturable absorber materials, graphene and MoS2. The waveguide (propagation losses of ~1 dB/cm) was micro-fabricated by means of ultrafast femtosecond laser writing. In the continuous-wave regime, the waveguide laser generated 247 mW at 1849.6 nm with a slope efficiency of 48.7%. The laser operated at the fundamental transverse mode with a linearly polarized output. With graphene as a saturable absorber, the pulse characteristics were 88 ns / 18 nJ (duration / energy) at a repetition rate of 1.39 MHz. Even shorter pulses of 66 ns were achieved with MoS2. Graphene and MoS2 are therefore promising for high repetition rate nanosecond Q-switched infrared waveguide lasers.