arXiv subjects

V. E. Minakova

Publications and source records attributed to V. E. Minakova.

10 recordsLinked to original sources

arXiv2025

Strain-induced splitting of the CCDW-NCCDW phase transition in 1T-TaS$_2$

The effects of uniaxial and biaxial tensile strain on the $ρ_{xx}$ and $ρ_{yy}$ components of the resistivity tensor, and the commensurable-nearly commensurate CDW (CCDW-NCCDW) transition temperature in 1T-TaS$_2$ are studied. At room temperature, uniaxial tensile strain increases the resistivity tensor components by a comparable magnitude both parallel and perpendicular to the strain axis. In the case of biaxial strain, up to 20~K decrease in the CCDW-NCCDW phase transition temperature is observed. In the case of uniaxial strain, a new phase with two different CCDW-NCCDW phase transition temperatures is observed, the splitting exceeds 10 K. The occurrence of such a phase is associated with the transition of the CDW into the commensurate state along the tensile strain direction while maintaining nearly commensurability along the perpendicular one. The results allow to justify various models widely used in analysis of transport properties of 1T-TaS$_2$ in commensurate and nearly commensurate states.

cond-mat.mtrl-sci↗

arXiv2025

Strain-induced proximity effect in topological insulator TaSe$_3$

The magnetoresistance of superconductor-topological insulator-superconductor structures, with indium as the superconductor and TaSe$_3$ as the topological insulator, shows steplike features on the resistance under magnetic fields. These resistance steps are resulted from the suppression of superconductivity, induced by the superconducting proximity effect in both the bulk and surface states of the topological insulator. The position and amplitude of the steps, occurring at approximately 0.1 T, show an unusual dependence on the magnitude of the uniaxial strain ($ε$), indicating their connection with surface states. This behavior follows the expected transition sequence: semi-metal $\rightarrow$ strong topological insulator $\rightarrow$ trivial insulator, and supports the presence of surface states at $0.46\% \lesssim ε\lesssim 0.85\%$.

cond-mat.supr-con↗

arXiv2019

A new type of charge-density-wave pinning in orthorhombic TaS$_3$ crystals with quenching defects

Diminishing in the concentration of quenching defects during thermocycling of orthorhombic TaS$_3$ samples in the temperature range below the Peierls transition temperature $T <T_P$ is observed. It makes it possible to study the character of pinning of the charge density wave (CDW) by these defects. A number of fundamental differences from pinning by ordinary local pinning centers - impurities and point defects - have been found. We conclude that quenching defects are extended (non-local) objects (presumably, dislocations) that can diffuse from the crystal during low-temperature termocycling due to their strong interaction with the CDW, which is intrinsic for the Peierls conductors. The presence of these defects leads to a previously unknown non-local type of CDW pinning that acts on $T_P$ and the threshold field for the onset of the CDW sliding, $E_T$, differently in comparison with the local pinning centers.

cond-mat.str-el↗

arXiv2015

Photoconduction and low-temperature Ohmic conduction of Peierls conductor o-TaS$_3$ under uniaxial strain

The effect of uniaxial strain on the photoconduction $δG$ and low-temperature Ohmic conduction $G$ of Peierls conductor o-TaS$_3$ have been studied. Four-contact structure on the base of high-quality o-TaS$_3$ crystal, containing a segment with a strain (1 \%) and one without it, separated by a buffer part, has been prepared for the study. Notable changes both $G(T)$ and $δG(T)$ have been observed below $T < 60$~K under uniaxial strain, namely: a plateau of $G(T)$ in the region of activation-law-change becomes wider under the strain, and an additional low-temperature maximum of $δG(T)$ appears, its value being even bigger than one of the main maximum of $δG(T)$, which is mainly due to single particle excitations. As a result the values of $G(T)$ and $δG(T)$ become one order bigger than the ones without strain. The relative changes of $G(T)$ and $δG(T)$ under the strain exhibit a sharp step-like growth upon cooling at slightly different temperatures ($\approx 10$~K). The observed features are consistent with a simple model implying strain-induced increase of concentration of solitons which contribute into both conduction and photoconduction.

cond-mat.str-el↗

arXiv2014

Charge-density waves physics revealed by photoconduction

The results of photoconduction study of the Peierls conductors are reviewed. The studied materials are quasi-one-dimensional conductors with the charge-density wave: K$_{0.3}$MoO$_3$, both monoclinic and orthorhombic TaS$_3$ and also a semiconducting phase of NbS$_3$ (phase I). Experimental methods, relaxation times, effects of illumination on linear and nonlinear charge transport, the electric-field effect on photoconduction and results of the spectral studies are described. We demonstrate, in particular, that a simple model of modulated energy gap slightly smoothed by fluctuations fits the available spectral data fairly well. The level of the fluctuations is surprisingly small and does not exceed a few percent of the optical energy gap value.

cond-mat.mes-hall↗

arXiv2014

Photoconduction in the Peierls conductor monoclinic TaS$_3$

Photoconduction in the monoclinic phase of quasi-one-dimensional conductor TaS$_3$ has been observed at $T < 70$~K. It was studied jointly with low-temperature ohmic and non-linear dark conduction. The strong sample quality dependence of both photoconduction and dark conduction at this temperature region has been observed. Together with a similarity of the main features of the photoconduction characteristic of both monoclinic ({\it m-}TaS$_3$) and orthorhombic ({\it o-}TaS$_3$) samples the following new peculiarities of photoconduction in {\it m-}TaS$_3$ were found: 1) the dependence of the activation energy of photoconduction on temperature, $T$, 2) the change of the recombination mechanism from the linear type to the collisional one at low $T$ with a sample quality growth, 3) the existence of a fine structure of the electric-field dependence of photoconduction. Spectral study gives the Peierls energy gap value $2Δ^*= 0.18$~eV.

cond-mat.str-el↗

arXiv2011

Photoconduction in CDW conductors

Photoconduction study of quasi-1D conductors allows to distinguish between the single-particle and collective {\it linear} conduction, investigate the effect of screening on collective transport and obtain interesting new details of the electronic energy structure of pure and doped CDW conductors. Here we present results of photoconduction study in quasi-1D conductors o-TaS$_3$, K$_{0.3}$MoO$_3$, and NbS$_3$(I).

cond-mat.mtrl-sci↗

arXiv2006

Evidence for collective linear conduction in the Peierls conductor o-TaS_3

Using photoconduction study we demonstrate that the low-temperature Ohmic conduction of TaS$_3$ is not provided by single-particle excitations -- electrons and holes excited over the Peierls gap. Instead, the low-temperature Ohmic conduction is mostly provided by collective excitations having the activation energy about half of the Peierls gap value and shunting the contribution of electrons and holes.

cond-mat.mtrl-sci↗

arXiv2004

Photoconduction and photocontrolled collective effects in the Peierls conductor TaS$_3$

Light illumination of thin crystals of CDW conductor TaS$_3$ is found to result in dramatic changes of both linear ($G$) and nonlinear conduction. The increase of $G$ is accompanied by suppression of the collective conduction, growth of the threshold field $E_T$, and appearance of the switching and hysteretic behavior in the nonlinear conduction. The effects in the nonlinear conduction are associated with increase of CDW elasticity due to illumination that leads in particular to appearance of a relation $E_T\propto G^{1/3}$ expected for the one-dimensional pinning.

cond-mat.str-el↗

arXiv2000

Convective Term and Transversely Driven Charge-Density Waves

We derive the convective terms in the damping which determine the structure of the moving charge-density wave (CDW), and study the effect of a current flowing transverse to conducting chains on the CDW dynamics along the chains. In contrast to a recent prediction we find that the effect is orders of magnitude smaller, and that contributions from transverse currents of electron- and hole-like quasiparticles to the force exerted on the CDW along the chains act in the opposite directions. We discuss recent experimental verification of the effect and demonstrate experimentally that geometry effects might mimic the transverse current effect.

cond-mat.str-el↗