Alexander A. Grabar
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Alexander A. Grabar has a total of 306 co-authors. Here are the top co-authors by number of shared publications:
- Yulian M. Vysochanskii
Uzhhorod University
27 shared publications - Oksana Mys
Ivan Franko National University of Lviv
11 shared publications I. M. Stoika
Uzhgorod National University 4 Institute of Solid State Physics and Chemistry 88 000 Uzhgorod, Ukraine
10 shared publicationsG. Montemezzani
Swiss Federal Institute of Technology (Switzerland)
8 shared publicationsGermano Montemezzani
8 shared publications- Iryna Martynyuk-Lototska
O. G. Vlokh Institute of Physical Optics
8 shared publications
Latest Publications
- Open Access
- 8 September 2026
- Published by Elsevier in Materials Today Physics
- Vol. 68
Manipulation and relaxation of domain-wall topologies in uniaxial triple-well ferroelectrics
- 8 September 2026
- Published by Elsevier in Materials Today Physics
- Vol. 68
Open AccessManipulation and relaxation of domain-wall topologies in uniaxial triple-well ferroelectrics
- 14 April 2026
- Published by Problems of Atomic Science and Technology in Problems of Atomic Science and Technology
PECULIARITIES OF FRAGMENTATION OF WATER AND AQUEOUS SOLUTIONS OF ALCOHOLS UNDER THE INFLUENCE OF RADIATION FACTORS OF DIFFERENT NATURE: PHYSICO-CHEMICAL AND BIOLOGICAL PARAMETERS
The results of conductometric and pH studies in the time evolution for the water and aqueous solutions of ethyl irradiated with different sort of nuclear particles are presented. Such parameters of liquids are determined by the peculiarities of the radiation fragmentation of their molecules. The influence of small and large doses of radiation on these parameters was studied using a microtron M-30 (18 MeV) and radiation stands (Pu-Be, 137Cs) capable of generating electron (e–), neutron (n), γ-, and mixed nuclear radiation. The high sensitivity of conductometric studies of irradiated liquids to nuclear e-, n-, and γ-irradiation has been established. It has been shown that, after irradiation, the physical properties of water are restored, and new chemical compounds can form in aqueous alcohol solutions according to the Lego game principle. The biological activity of irradiated liquids was also studied using several common test microorganisms. Data on the radiation-induced fragmentation of liquids are essential for understanding their biological activity.
- 14 April 2026
- Published by Problems of Atomic Science and Technology in Problems of Atomic Science and Technology
PECULIARITIES OF FRAGMENTATION OF WATER AND AQUEOUS SOLUTIONS OF ALCOHOLS UNDER THE INFLUENCE OF RADIATION FACTORS OF DIFFERENT NATURE: PHYSICO-CHEMICAL AND BIOLOGICAL PARAMETERS
The results of conductometric and pH studies in the time evolution for the water and aqueous solutions of ethyl irradiated with different sort of nuclear particles are presented. Such parameters of liquids are determined by the peculiarities of the radiation fragmentation of their molecules. The influence of small and large doses of radiation on these parameters was studied using a microtron M-30 (18 MeV) and radiation stands (Pu-Be, 137Cs) capable of generating electron (e–), neutron (n), γ-, and mixed nuclear radiation. The high sensitivity of conductometric studies of irradiated liquids to nuclear e-, n-, and γ-irradiation has been established. It has been shown that, after irradiation, the physical properties of water are restored, and new chemical compounds can form in aqueous alcohol solutions according to the Lego game principle. The biological activity of irradiated liquids was also studied using several common test microorganisms. Data on the radiation-induced fragmentation of liquids are essential for understanding their biological activity.
- 29 May 2025
- Published by Elsevier in Optical Materials
- Vol. 166
Photorefractive properties of double-doped SnPS ferroelectrics- 29 May 2025
- Published by Elsevier in Optical Materials
- Vol. 166
Photorefractive properties of double-doped SnPS ferroelectrics- Open Access
- 13 December 2024
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 136 (22)
Dual role of Te ions as electron traps and hole traps in ferroelectric Sn2P2S6 crystals
Tin hypothiodiphosphate (Sn2P2S6) is a ferroelectric semiconductor with electro-optic and photorefractive relevance. The lattice contains Sn2+ ions and (P2S6)4− anionic groups. In the present work, an Sn2P2S6 crystal is doped with Te during growth. Our results show that the Te ions occupy Sn sites and S sites, where they serve as electron and hole traps, respectively. Electron paramagnetic resonance (EPR) spectra from five trapped holes and one trapped electron are observed at low temperatures after exposure to 633 nm light. Spin-Hamiltonian parameters are extracted from the angular dependence of each spectrum. Holes are localized on (P2TeS5)4− units and form (P2TeS5)3− anions, with the five defects corresponding to Te on different S sites within the anion. These defects have large g shifts caused by the tellurium spin–orbit coupling parameter. Four of the five also have an isotropic hyperfine interaction with one Sn ion, which suggests that they have an adjacent Sn vacancy (leaving just one close Sn neighbor). Three trapped-hole spectra are photoinduced at 20 K and two appear after removing the light, warming to 120 K, and then returning to 20 K. Electrons are trapped in pairs at Te4+ ions occupying Sn2+ sites when the crystal is exposed to 633 nm light while at 20 K. The Te2+ ions that are formed have no observable EPR spectrum. Warming to 100 K releases one electron from Te2+ ions that have an adjacent Sn vacancy, and an EPR spectrum from Te3+ ions (5s25p) is seen when the crystal is returned to lower temperatures.
- 13 December 2024
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 136 (22)
Open AccessDual role of Te ions as electron traps and hole traps in ferroelectric Sn2P2S6 crystals
Tin hypothiodiphosphate (Sn2P2S6) is a ferroelectric semiconductor with electro-optic and photorefractive relevance. The lattice contains Sn2+ ions and (P2S6)4− anionic groups. In the present work, an Sn2P2S6 crystal is doped with Te during growth. Our results show that the Te ions occupy Sn sites and S sites, where they serve as electron and hole traps, respectively. Electron paramagnetic resonance (EPR) spectra from five trapped holes and one trapped electron are observed at low temperatures after exposure to 633 nm light. Spin-Hamiltonian parameters are extracted from the angular dependence of each spectrum. Holes are localized on (P2TeS5)4− units and form (P2TeS5)3− anions, with the five defects corresponding to Te on different S sites within the anion. These defects have large g shifts caused by the tellurium spin–orbit coupling parameter. Four of the five also have an isotropic hyperfine interaction with one Sn ion, which suggests that they have an adjacent Sn vacancy (leaving just one close Sn neighbor). Three trapped-hole spectra are photoinduced at 20 K and two appear after removing the light, warming to 120 K, and then returning to 20 K. Electrons are trapped in pairs at Te4+ ions occupying Sn2+ sites when the crystal is exposed to 633 nm light while at 20 K. The Te2+ ions that are formed have no observable EPR spectrum. Warming to 100 K releases one electron from Te2+ ions that have an adjacent Sn vacancy, and an EPR spectrum from Te3+ ions (5s25p) is seen when the crystal is returned to lower temperatures.
- 23 February 2021
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 129 (8) , 085702
Photoinduced trapping of charge at sulfur vacancies and copper ions in photorefractive Sn2P2S6 crystals
Electron paramagnetic resonance (EPR) is used to monitor photoinduced changes in the charge states of sulfur vacancies and Cu ions in tin hypothiodiphosphate. A Sn2P2S6 crystal containing Cu+ (3d10) ions at Sn2+ sites was grown by the chemical vapor transport method. Doubly ionized sulfur vacancies ( ) are also present in the as-grown crystal (where they serve as charge compensators for the Cu+ ions). For temperatures below 70 K, exposure to 532 or 633 nm laser light produces stable Cu2+ (3d9) ions, as electrons move from Cu+ ions to sulfur vacancies. A g matrix and a 63,65Cu hyperfine matrix are obtained from the angular dependence of the Cu2+ EPR spectrum. Paramagnetic singly ionized ( ) and nonparamagnetic neutral ( ) charge states of the sulfur vacancies, with one and two trapped electrons, respectively, are formed during the illumination. Above 70 K, the neutral vacancies ( ) are thermally unstable and convert to vacancies by releasing an electron to the conduction band. These released electrons move back to Cu2+ ions and restore Cu+ ions. Analysis of isothermal decay curves acquired by monitoring the intensity of the Cu2+ EPR spectrum between 74 and 82 K, after removing the light, gives an activation energy of 194 meV for the release of an electron from a vacancy. Warming above 120 K destroys the vacancies and the remaining Cu2+ ions. The photoinduced EPR spectrum from a small concentration of unintentionally present Ni+ ions at Sn2+ sites is observed near 40 K in the Sn2P2S6 crystal.- 23 February 2021
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 129 (8) , 085702
Photoinduced trapping of charge at sulfur vacancies and copper ions in photorefractive Sn2P2S6 crystals
Electron paramagnetic resonance (EPR) is used to monitor photoinduced changes in the charge states of sulfur vacancies and Cu ions in tin hypothiodiphosphate. A Sn2P2S6 crystal containing Cu+ (3d10) ions at Sn2+ sites was grown by the chemical vapor transport method. Doubly ionized sulfur vacancies ( ) are also present in the as-grown crystal (where they serve as charge compensators for the Cu+ ions). For temperatures below 70 K, exposure to 532 or 633 nm laser light produces stable Cu2+ (3d9) ions, as electrons move from Cu+ ions to sulfur vacancies. A g matrix and a 63,65Cu hyperfine matrix are obtained from the angular dependence of the Cu2+ EPR spectrum. Paramagnetic singly ionized ( ) and nonparamagnetic neutral ( ) charge states of the sulfur vacancies, with one and two trapped electrons, respectively, are formed during the illumination. Above 70 K, the neutral vacancies ( ) are thermally unstable and convert to vacancies by releasing an electron to the conduction band. These released electrons move back to Cu2+ ions and restore Cu+ ions. Analysis of isothermal decay curves acquired by monitoring the intensity of the Cu2+ EPR spectrum between 74 and 82 K, after removing the light, gives an activation energy of 194 meV for the release of an electron from a vacancy. Warming above 120 K destroys the vacancies and the remaining Cu2+ ions. The photoinduced EPR spectrum from a small concentration of unintentionally present Ni+ ions at Sn2+ sites is observed near 40 K in the Sn2P2S6 crystal.- 13 October 2020
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 153 (14) , 144503
Charge trapping by iodine ions in photorefractive Sn2P2S6 crystals
Electron paramagnetic resonance (EPR) is used to establish the role of iodine as an electron trap in tin hypothiodiphosphate (Sn2P2S6) crystals. Iodine ions are unintentionally incorporated when the crystals are grown by the chemical-vapor-transport method with SnI4 as the transport agent. The Sn2P2S6 crystals consist of Sn2+ ions and (P2S6)4− anionic groups. During growth, an iodine ion replaces a phosphorus in a few of the anionic groups, thus forming (IPS6)4− molecular ions. Following an exposure at low temperature to 633 nm laser light, these (IPS6)4− ions trap an electron and convert to EPR-active (IPS6)5− groups with S = 1/2. A concentration near 1.1 × 1017 cm−3 is produced. The EPR spectrum from the (IPS6)5− ions has well-resolved structure resulting from large hyperfine interactions with the 127I and 31P nuclei. Analysis of the angular dependence of the spectrum gives principal values of 1.9795, 2.0123, and 2.0581 for the g matrix, 232 MHz, 263 MHz, and 663 MHz for the 127I hyperfine matrix, and 1507 MHz, 1803 MHz, and 1997 MHz for the 31P hyperfine matrix. Results from quantum-chemistry modeling (unrestricted Hartree–Fock/second-order Møller–Plesset perturbation theory) support the (IPS6)5− assignment for the EPR spectrum. The transient two-beam coupling gain can be improved in these photorefractive Sn2P2S6 crystals by better controlling the point defects that trap charge.
- 13 October 2020
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 153 (14) , 144503
Charge trapping by iodine ions in photorefractive Sn2P2S6 crystals
Electron paramagnetic resonance (EPR) is used to establish the role of iodine as an electron trap in tin hypothiodiphosphate (Sn2P2S6) crystals. Iodine ions are unintentionally incorporated when the crystals are grown by the chemical-vapor-transport method with SnI4 as the transport agent. The Sn2P2S6 crystals consist of Sn2+ ions and (P2S6)4− anionic groups. During growth, an iodine ion replaces a phosphorus in a few of the anionic groups, thus forming (IPS6)4− molecular ions. Following an exposure at low temperature to 633 nm laser light, these (IPS6)4− ions trap an electron and convert to EPR-active (IPS6)5− groups with S = 1/2. A concentration near 1.1 × 1017 cm−3 is produced. The EPR spectrum from the (IPS6)5− ions has well-resolved structure resulting from large hyperfine interactions with the 127I and 31P nuclei. Analysis of the angular dependence of the spectrum gives principal values of 1.9795, 2.0123, and 2.0581 for the g matrix, 232 MHz, 263 MHz, and 663 MHz for the 127I hyperfine matrix, and 1507 MHz, 1803 MHz, and 1997 MHz for the 31P hyperfine matrix. Results from quantum-chemistry modeling (unrestricted Hartree–Fock/second-order Møller–Plesset perturbation theory) support the (IPS6)5− assignment for the EPR spectrum. The transient two-beam coupling gain can be improved in these photorefractive Sn2P2S6 crystals by better controlling the point defects that trap charge.
- Open Access
- 21 July 2020
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 2 (3) , 032022
Slow light of dark pulses in a photorefractive crystal
Slowdown of Gaussian “dark pulses” in photorefractive crystal using a two-wave mixing method is shown at room temperature. In agreement with our theoretical model, the experiment shows the dependence of the dark pulse delay and the group velocity values on the photorefractive gain and the input pulse width . The use of dark pulses allows us to improve the time-delay values and achieve maximal fractional of about 1 for a pulse duration close to the crystal response time.- 21 July 2020
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 2 (3) , 032022
Open AccessSlow light of dark pulses in a photorefractive crystal
Slowdown of Gaussian “dark pulses” in photorefractive crystal using a two-wave mixing method is shown at room temperature. In agreement with our theoretical model, the experiment shows the dependence of the dark pulse delay and the group velocity values on the photorefractive gain and the input pulse width . The use of dark pulses allows us to improve the time-delay values and achieve maximal fractional of about 1 for a pulse duration close to the crystal response time. - 18 June 2020
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry C
- Vol. 8 (29) , 9975-9985
Customization of Sn2P2S6 ferroelectrics by post-growth solid-state diffusion doping
For the first time, we demonstrated successful post-synthesis incorporation of metal dopants at elevated temperature into a host structure of Sn2P2S6, known as the grandfather of dichalcogenide ferroelectrics with a formula M2P2X6 (M = metal and X = chalcogen).
- 18 June 2020
- Published by Royal Society of Chemistry (RSC) in Journal of Materials Chemistry C
- Vol. 8 (29) , 9975-9985
Customization of Sn2P2S6 ferroelectrics by post-growth solid-state diffusion doping
For the first time, we demonstrated successful post-synthesis incorporation of metal dopants at elevated temperature into a host structure of Sn2P2S6, known as the grandfather of dichalcogenide ferroelectrics with a formula M2P2X6 (M = metal and X = chalcogen).
- Open Access
- 11 March 2020
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 127 (10) , 103103
Near-infrared-sensitive photorefractive Sn2P2S6 crystals grown by the Bridgman method
Ferroelectric tin hypothiodiphosphate (Sn P S ) crystals are well-known for their significant piezoelectric, electro-optic, and nonlinear optical properties. These crystals have usually been grown by a vapor transport technique. We report in this paper on the first study of photorefractive nonlinearity in Sn P S crystals grown by the Bridgman method. Pronounced photorefraction is observed in the near-infrared region of the spectrum even with no preliminary optical sensitizing.- 11 March 2020
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 127 (10) , 103103
Open AccessNear-infrared-sensitive photorefractive Sn2P2S6 crystals grown by the Bridgman method
Ferroelectric tin hypothiodiphosphate (Sn P S ) crystals are well-known for their significant piezoelectric, electro-optic, and nonlinear optical properties. These crystals have usually been grown by a vapor transport technique. We report in this paper on the first study of photorefractive nonlinearity in Sn P S crystals grown by the Bridgman method. Pronounced photorefraction is observed in the near-infrared region of the spectrum even with no preliminary optical sensitizing. - 31 October 2016
- Published by AIP Publishing in Applied Physics Letters
- Vol. 109 (18) , 182104
Optical determination of the charge carrier mobility in Sn2P2S6
We determine both the lifetime and the mobility of photoexcited charge carriers in Sn2P2S6 using holographic time of flight in diffusion mode. From the build-up dynamics of space charge gratings created by pulsed interband illumination at 532 nm, we find a charge carrier lifetime of 2.6 ± 0.5 ns and a charge carrier mobility along the x-axis of 2.4 ± 0.6 cm2 V−1 s−1 at room temperature. This mobility is assigned to holes as more mobile carriers in tin hypothiodiphosphate (SPS), and it is found to decrease for decreasing temperature, a behavior consistent with small-polaron hopping.
- 31 October 2016
- Published by AIP Publishing in Applied Physics Letters
- Vol. 109 (18) , 182104
Optical determination of the charge carrier mobility in Sn2P2S6
We determine both the lifetime and the mobility of photoexcited charge carriers in Sn2P2S6 using holographic time of flight in diffusion mode. From the build-up dynamics of space charge gratings created by pulsed interband illumination at 532 nm, we find a charge carrier lifetime of 2.6 ± 0.5 ns and a charge carrier mobility along the x-axis of 2.4 ± 0.6 cm2 V−1 s−1 at room temperature. This mobility is assigned to holes as more mobile carriers in tin hypothiodiphosphate (SPS), and it is found to decrease for decreasing temperature, a behavior consistent with small-polaron hopping.