Vladimir Bukin

Dr. Vladimir Bukin

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Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

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

Representative Publications

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14 March 2022 in Applied Physics Letters
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NCNikita Chernomyrdin
Nikita Chernomyrdin
MSM. Skorobogatiy
M. Skorobogatiy
DPDmitry Ponomarev
Dmitry Ponomarev
VBVladimir Bukin
Vladimir Bukin
Valery TuchinValery Tuchin
Valery Tuchin
KZKirill I. Zaytsev
Kirill I. Zaytsev
Unique effects of terahertz (THz)-wave–matter interaction push rapid progress in THz optoelectronics aimed at bridging the problematic THz gap. However, majority of modern methods of THz spectroscopy and imaging are still hampered by low spatial resolution. Common lens/mirror-based THz optics fails to overcome the Abbe barrier and usually provides resolution larger than a free-space wavelength λ (i.e., hundreds of micrometers or even few millimeters). To mitigate this difficulty, supperresolution THz imaging modalities were introduced recently, among which we particularly underline different methods of THz scanning-probe near-field microscopy. They not only rely on strong light confinement on sub-wavelength probes and provide resolution down to ∼10−1 –10−3λ but also suffer from small energy efficiency or presume an interplay among imaging resolution, signal-to-noise ratio, and performance. In this paper, we consider reflection-mode THz solid immersion (SI) microscopy that offers some compromise between the high imaging resolution of 0.15λ and high energy efficiency, which is due to the absence of any subwavelength probe in an optical scheme. Recent achievements, challenging problems, and prospects of SI microscopy are overviewed with an emphasis on resolving the inverse problem and applications in THz biophotonics.

26 January 2021 in Nanomaterials
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POPetr Obraztsov
Petr Obraztsov
VBVladislava Bulgakova
Vladislava Bulgakova
PCPavel Chizhov
Pavel Chizhov
AUAleksandr Ushakov
Aleksandr Ushakov
DGDmitry S. Gets
Dmitry S. Gets
VBVladimir Bukin
Vladimir Bukin
Hybrid organic–inorganic perovskites, while well examined for photovoltaic applications, remain almost completely unexplored in the terahertz (THz) range. These low-cost hybrid materials are extremely attractive for THz applications because their optoelectronic properties can be chemically engineered with relative ease. Here, we experimentally demonstrate the first attempt to apply solution-processed polycrystalline films of hybrid perovskites for the development of photoconductive terahertz emitters. By using the widely studied methylammonium-based perovskites MAPbI3 and MAPbBr3, we fabricate and characterize large-aperture photoconductive antennas. The work presented here examines polycrystalline perovskite films excited both above and below the bandgap, as well as the scaling of THz emission with the applied bias field and the optical excitation fluence. The combination of ultrafast time-resolved spectroscopy and terahertz emission experiments allows us to determine the still-debated room temperature carrier lifetime and mobility of charge carriers in halide perovskites using an alternative noninvasive method. Our results demonstrate the applicability of hybrid perovskites for the development of scalable THz photoconductive devices, making these materials competitive with conventional semiconductors for THz emission.

7 April 2023 in Optics Express
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Journal Article
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AKA. S. Kucheryavenko
A. S. Kucheryavenko
VZVladislav Zhelnov
Vladislav Zhelnov
DMD. G. Melikyants
D. G. Melikyants
NCNikita Chernomyrdin
Nikita Chernomyrdin
SLSergey Lebedev
Sergey Lebedev
GKG. M. Katyba
G. M. Katyba
To address a challenging problem of super-resolution terahertz (THz) endoscopy, in this paper, an antiresonant hollow-core waveguide was coupled with a sapphire solid immersion lens (SIL), aimed at subwavelength confinement of guided mode. The waveguide is formed by a polytetrafluoroethylene (PTFE)-coated sapphire tube, the geometry of which was optimized to ensure high optical performance. SIL was judiciously designed, fabricated of bulk sapphire crystal, and then mounted at the output waveguide end. Study of the field intensity distributions at the shadow side of the waveguide–SIL system revealed the focal spot diameter of ≃0.2λ at the wavelength of λ = 500 μm. It agrees with numerical predictions, overcomes the Abbe diffraction limit, and justifies super-resolution capabilities of our endoscope.

9 June 2021 in Applied Physics Express
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MPMariya Ponarina
Mariya Ponarina
Andrey Gordeevich OkhrimchukAndrey Gordeevich Okhrimchuk
Andrey Gordeevich Okhrimchuk
GAGrigory Alagashev
Grigory Alagashev
GOGalina Orlova
Galina Orlova
TDTimophey Dolmatov
Timophey Dolmatov
POPetr Obraztsov
Petr Obraztsov

29 November 2017 in JETP Letters
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AUAleksandr Ushakov
Aleksandr Ushakov
MMM. Matoba
M. Matoba
NNN. Nemoto
N. Nemoto
NKN. Kanda
N. Kanda
KKK. Konishi
K. Konishi
ASA. B. Savel’ev
A. B. Savel’ev
We report the first experimental observation of backward terahertz emission from the two-color laser induced plasma filament in air. The ratio of measured forward-to-backward terahertz radiation is ∼25/1. This result agrees with numerical simulations based on interferometric model assuming 0.3 mm long plasma source.

22 August 2023 in Journal of Applied Physics
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AGArsenii A. Gavdush
Arsenii A. Gavdush
GKGennadiy A. Komandin
Gennadiy A. Komandin
VBVladimir Bukin
Vladimir Bukin
KZKirill I. Zaytsev
Kirill I. Zaytsev
DPDmitry Ponomarev
Dmitry Ponomarev
Qiwu ShiQiwu Shi
Qiwu Shi
Phase-change alloy Ge2Sb2Te5 (GST) forms a favorable material platform for modern optics, photonics, and electronics thanks to a pronounced increase in conductivity with thermally induced phase transitions from amorphous (a-GST) into cubic (c-GST) and then hexagonal (h-GST) crystalline states at the temperatures of ≃150 and ≃300°C, respectively. Nevertheless, the data on broadband electrodynamic response of distinct GST phases are still missing, which hamper the design and implementation of related devices and technologies. In this paper, a-, c-, and h-GST films on a sapphire substrate are studied using broadband dielectric spectroscopy. For all GST phases, complex dielectric permittivity is retrieved using Drude and Lorentz models in the frequency range of 0.06–50 THz or the wavelength range of ≃5000–6 μm. A contribution from the free charge-carriers conductivity and vibrational modes to the broadband response of an analyte is quantified. In this way, the Drude model allows for estimation of the static (direct current—DC) and dynamic (at 1.0 THz) conductivity values, caused by motions of free charges only, which are as high as σDC≃15 and 40 S/cm and σ1.0THz≃8.8 and 28.6 S/cm for the c- and h-GSTs, respectively. This overall agrees with the results of electrical measurements of GST conductivity using the four-point probe technique. The broadband electrodynamic response models obtained for the three GST phases are important for further research and developments of GST-based devices and technologies.