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V. A. Kozlov

Publications and source records attributed to V. A. Kozlov.

11 recordsLinked to original sources
arXiv2024

Nonlinear scintillation effects in the intrinsic luminescence from Sc$_{1.318}$Y$_{0.655}$Si$_{1.013}$O$_{4.987}$ crystal excited by electrons and gamma-quanta

The spectral and kinetic properties of intrinsic luminescence from (Y$_2$Sc$_1$)$_{0.(3)}$(Sc)[Si]O$_5$ crystal are studied. The emission is excited by electrons and gamma-quanta. The composition (Y$_2$Sc$_1$)$_{0.(3)}$(Sc)[Si]O$_5$ is the congruent one for Sc$_2$SiO$_5$-Y$_2$SiO$_5$ solid solutions. It is found, that the crystal emits fairly bright intrinsic cathodololuminescence (CL) and radioluminescence (RL) at room temperature. In particular, the light yield of scintillation excited by -quanta with the energies of 661.7 keV is of 12000 photons/MeV. An increase in the beam flux by $\sim$20 times leads to the shift in the maximum CL energy spectral density from 315 to 340 nm and to the decrease in the CL decay time at 415 nm from 1377 +/- 3 ns to 1165 +/- 1 ns. Simultaneously, the decay time of RL excited by a photoelectron with the energy of 644.7 keV is of 1310 +/- 10 ns while a Compton electron with the energy of 477 keV excites RL with the decay time of 1050 +/- 10 ns. Also, we observed differences in the CL yield dependencies on the volume-averaged density of electronic excitations (EEs) at different wavelengths. An explanation of the results is given considering the nonlinear scintillation phenomena induced by an interaction between EEs. It is based on a conception that an increase in EE volume density leads to an increase in EEs nonradiative quenching due to these interactions.

physics.ins-det↗
arXiv2023

Luminescence from oxygen vacancies in Lu$_{2}$SiO$_{5}$ crystal and ceramics at room temperature

Photoluminescence (PL) of Lu$_{2}$SiO$_{5}$ crystal and ceramics with a high concentration of oxygen vacancies (about ~0.5 at.%) is studied. Oxygen vacancies were created using two ways. The first method is a growth of crystal from the non-stoichiometric Lu$_{2}$Si$_{0.98}$O$_{4.96}$ melt and the second one is a doping of Lu$_{2}$SiO$_{5}$ matrix with divalent Ca$^{2+}$ ions at the concentration of 1 at.%. For the first time we observe a fairly bright room-temperature ultraviolet PL of both crystal grown from the Lu$_{2}$Si$_{0.98}$O$_{4.96}$ melt and Lu$_{2}$SiO$_{5}$ ceramics doped with Ca$^{2+}$ ions. A band at 290 nm in the PL spectrum of the crystal and a band at 283 nm in the PL spectrum of the calcium-doped ceramics are observed. The spectral and kinetic properties of these bands are close to each other. This fact indicates similar origins of these bands. The results of the work show that the studied ultraviolet luminescence is related to oxygen vacancies in lutetium oxyorthosilicate.

physics.optics↗
arXiv2019

Trapped modes in armchair graphene nanoribbons

We study scattering on an ultra-low potential in armchair graphene nanoribbon. Using the continuous Dirac model and including a couple of artificial waves in the scattering process, described by an augumented scattering matrix, we derive a condition for the existence of a trapped mode. We consider the threshold energies, where the the multiplicity of the continuous spectrum changes and show that a trapped mode may appear for energies slightly less than a threshold and its multiplicity does not exceed one. For energies which are higher than a threshold, there are no trapped modes, provided that the potential is sufficiently small.

math-ph↗
arXiv2017

2.5 eV Pulsed Cathodoluminesce band of silicon dioxide

Room-temperature (RT) Pulsed Cathodoluminescence (PCL) spectra of a set of pure synthetic (both crystalline and amorphous) silicon dioxide materials were studied. It is shown, that the PCL spectra of all samples (both amorphous and crystalline) possess a separate band at 495 nm (2.5 eV). This band is the most intensive one in PCL spectra of disordered materials. The RT PCL band at 495 nm (2.5 eV) of α-quartz single crystal is polarized in XY crystalline plane (perpendicular to the $3^{rd}$ order symmetry axis). The structure of this band was detected. It consists of three peaks: at 480$\pm$2 nm (2.58$\pm$0.01 eV), 487$\pm$ nm (2.55$\pm$0.01 eV) and 493$\pm$2 nm (2.52$\pm$0.01 eV). Energy separation between peaks is equal in order of magnitude to energies of $Li_{x}O_{y}$ molecular vibrations and to the energy of optical phonon in α-quartz. It is shown, that the emission band at 495 nm (2.5 eV) in RT PCL spectra of α-quartz single crystal is related to the bulk emission centers, not to the surface-related ones. The annealing behaviors of the 495 nm (2.5 eV) bands in spectrum of amorphous and crystalline $SiO_{2}$ are close to each other. This fact may be the manifestation of identical origin of these bands. The following explanation of experimental data is proposed: the origin of 495 nm (2.5 eV) band in pure silicon dioxide is related to the recombination of non-bridging oxygen $NBO^{-}-Li^{+}$ centers.

cond-mat.mtrl-sci↗
arXiv2017

Trapped modes in zigzag graphene nanoribbons

We study a scattering on an ultra-low potential in zigzag graphene nanoribbon. Using mathematical framework based on the continuous Dirac model and augumented scattering matrix, we derive a condition for the existence of a trapped mode. We consider the threshold energies where the continuous spectrum changes its multiplicity and show that the trapped modes may appear for energies slightly less than a threshold and its multiplicity does not exceeds one. We prove that trapped modes do not appear outside the threshold, provided the potential is sufficiently small.

math-ph↗
arXiv2016

Pulsed Cathodoluminescence Spectra of Solid Oxides with Low Concentrations of Optically-Active Impurities

Pulsed cathodoluminescence (PCL) spectra of ultra-pure SiO2, GeO2, SnO2, TiO2, La2O3, Y2O3, Sc2O3, CaCO3 powders and α-quartz, Ca:YVO4, LiNbO3 and Sc:LiNbO3 crystals were studied under the same experimental conditions. It was found that PCL spectra of SiO2, SnO2, GeO2, TiO2, La2O3 and CaCO3 powders contain a common band with maximum intensity at 500 nm, PCL spectra of samples Y2O3, Sc2O3, PbWO4 and Ca:YVO4 contain a common band at 490 nm and PCL spectra of LiNbO3 and Sc:LiNbO3 crystals contain a common band at 507 nm. It was found that the average intensity of the PCL spectra and position of the maximum intensity of these common bands depend on the type of a band gap transition of the material. We suppose that these common bands have the same origin in PCL spectra of all the materials studied and are related to recombination of O2--O-oxygen complexes. These complexes appear in the vicinities of anionic and cationic vacancies, where the geometry and orientation of coordination polyhedrons are violated due to the stress in the lattice.

physics.optics↗
arXiv2005

Heat Content Asymptotics for Riemannian manifolds with Zaremba boundary conditions

The existence of a full asymptotic expansion for the heat content asymptotics of an operator of Laplace type with classical Zaremba boundary conditions on a smooth manifold is established. The first three coefficients in this asymptotic expansion are determined in terms of geometric invariants; partial information is obtained about the fourth coefficient.

math-ph↗
arXiv1993

Closed Abrikosov Vortices in a Superconducting Cylinder

The new type of solutions of the London equation for type-II superconductors is obtained to describe the ring-shaped (toroidal) Abrikosov vortices. The specific feature of these solutions is the self-consistent localization of both the supercurrent and the magnetic field, enabling one to construct compact magnetic structures inside a superconductor. The torus vortex contraction caused by the vortex instability leads to the destruction of the Cooper pairing and the formation of a normal electron stream in the vicinity of the torus axis. The thermodynamic condition for the excitation of a small closed vortex by a bunch of charged particles contains the fine-structure constant as a determining parameter.

cond-mat↗