arXiv subjects

M. S. Barabashko

Publications and source records attributed to M. S. Barabashko.

7 recordsLinked to original sources

arXiv2025

Heat Capacity of Thermally Reduced Graphene Oxide: Compaction and Thermal Annealing Effects

We present a comprehensive investigation of the low-temperature heat capacity of thermally reduced graphene oxide (trGO) as a function of compaction pressure and annealing temperature. Graphene oxide was synthesized using a modified Hummers method and subsequently thermally reduced at 300\,°C, 500\,°C, and 700\,°C under vacuum to systematically vary the oxygen content and structural ordering. The specific heat data in the 2--300\,K range reveal that the thermal response is governed by phonons, including contributions from a Schottky-type anomaly, a defect-related linear term, a Debye term, and a dispersive term with a negative coefficient associated with out-of-plane flexural (ZA) phonons. Increasing compaction pressure alters interlayer coupling and leads to non-monotonic changes in heat capacity, while higher annealing temperatures enhance graphitization, reduce disorder, and modify phonon dispersion. The absence of a boson peak -- similar to that observed in carbon nanotubes -- supports the dominance of two-dimensional vibrational modes. These findings elucidate the relationship between dimensionality, structural disorder, and processing parameters in shaping the phonon dynamics of trGO, providing guidance for tailoring its thermal behavior in advanced carbon-based functional materials.

cond-mat.mtrl-sci↗

arXiv2025

Low-Temperature Heat Capacity and Phonon Dynamics in Expanded Graphite and EG--MWCNTs Composites

The specific heat of expanded graphite (EG) and EG--multiwalled carbon nanotube (MWCNT) composites (1.0 and 3.0 wt.\% MWCNTs) was measured between 2 and 300~K. The low-temperature heat capacity is dominated by out-of-plane flexural phonons with quadratic dispersion, characteristic of two-dimensional layered systems. Compared with crystalline graphite, EG exhibits enhanced heat capacity due to increased defect density and reduced interlayer coupling. Structural characterization (XRD, Raman, EDS) confirmed variations in stacking order and defect concentration. The data were fitted using a three-term model ($C_{1}T + C_{3}T^{3} + C_{5}T^{5}$), where the negative $C_{5}$ term indicates quadratic phonon dispersion. The results demonstrate the influence of MWCNT integration and structural disorder on phonon dynamics and anisotropic heat capacity in EG-based composites.

cond-mat.mtrl-sci↗

arXiv2023

Proportional correlation between heat capacity and thermal expansion of atomic, molecular crystals and carbon nanostructures

Correlation between thermal expansions $β(T)$ and heat capacity $C(T)$ of atomic and molecular crystals, amorphous materials with a structural disorder, carbon nanomaterials (fullerite C$_{60}$, bundles SWCNTs of single-walled carbon nanotubes) was analyzed. The influence of the contribution to the coefficient of linear thermal expansion $α_\textrm{Xe}(T)$ of Xe atoms adsorbed on the SWCNTs bundles is considered. The proportional correlation was found between the contribution to the coefficient of linear thermal expansion $α_\textrm{Xe}(T)$ and the normalized to the gas constant heat capacity $C_\textrm{Xe}(T)/R$ of Xe atoms adsorbed on the SWCNTs bundles. The proportional correlation $(β/β^*) \sim (C_\textrm{V}/R)$ with the parameter $β^*$ for the bulk thermal expansion coefficient for cryocrystals is proposed. In the case of atomic crystals such as Xe and Ar, the proportional correlation $(β/β^*) \sim (C_\textrm{V}/R)$ is observed in the temperature range from the lowest experimental to temperatures where $C_\textrm{V}/R \approx 2.3$. The correlation is not observed in the temperatures where $2.3<C_V/R<3$ (classical Dulong-Petit law). It was found that the universal proportional correlation is also observed for molecular crystals with linear symmetry, such as CO$_{2}$, CO, and N$_{2}$O if the normalized heat capacity below the values $C_\textrm{V}/R \approx 3 ÷3.5$.

cond-mat.soft↗

arXiv2014

The low temperature heat capacity of solutions of methane isotopes in fullerite C60. Isotope effects

The heat capacity C(T) of the interstitial solid solution (CH4)0.4C60 has been investigated in the temperature interval 1.4-120 K. The contribution of CH4 molecules to the heat capacity has been separated. The contributions of CH4 and CD4 molecules to the heat capacity of the solutions (CH4)0.40C60 and (CD4)0.40C60 have been compared. It is found that above 80K the character of the rotational motion of CH4 and CD4 molecules changes from libration to hindered rotation. In the interval 14-35 K the heat capacities of CH4 and CD4 molecules are satisfactorily described by contributions of the translational and libration vibrations, as well as the tunnel rotation for the equilibrium distribution of the nuclear spin species. The isotope effect in heat capacity of CH4 and CD4 molecules is due, mainly, the difference in the frequencies of local tranlational and libration vibrations of molecules CH4 and CD4. The contribution of the tunnel rotation of the CH4 and CD4 molecules to the heat capacities of this gases is dominant below 8 K. The isotopic effect is caused by the difference between both the conversion rates and the rotational spectra of the nuclear spin species of CH4 and CD4 molecules. The conversion rate of CH4 molecules is several times lower than that of CD4 ones. Weak features observed in the curves of heat capacity of CH4 and CD4 near 6 K and 8 K, respectively, are most likely a manifestation of first-order phase transitions in the orientational glasses of these solutions.

cond-mat.mes-hall↗

arXiv2014

Thermally created vacancies in the 1D chains of xenon adsorbed in the grooves of single-walled carbon nanotube bundles

The heat capacity of 1D chains of Xe adsorbed in the outer grooves of bundles of closed single-walled carbon nanotubes have been investigated in the temperature range from 2 to 55 K. The experimental results of heat capacity are close to the theoretical calculation below 8 K. Above 8 K the experimental curve exceeds the theoretical one and excess increases monotonously with temperature. It was assumed that the sharp increase of the difference between the experimental and theoretical curves of heat capacity above 30 K is associated with the occurrence of the thermally created vacancies in the chains due to spatial redistribution of the xenon atoms. The molar enthalpy of vacancy formation in the chain has been calculated.

cond-mat.mes-hall↗

arXiv2013

The heat capacity of nitrogen chains in grooves of single-walled carbon nanotube bundles

The heat capacity of bundles of closed-cap single-walled carbon nanotubes (SWNT) with one-dimensional chains of nitrogen molecules adsorbed in the grooves has been first experimentally studied at temperatures from 2K to 40K using an adiabatic calorimeter. The contribution of nitrogen C(T) to the total heat capacity has been separated. In the region 2-8K the behaviour of the curve C(T) is qualitatively similar to the theoretical prediction of the phonon heat capacity of 1D chains of krypton (Kr) atoms localized in the grooves of SWNT bundles. Below 3K the dependence C(T) is linear. Above 8K the dependence C(T) becomes steeper in comparison with the case of Kr atoms. This behaviour of the heat capacity C(T) is due to the contribution of the rotational degrees of freedom of the nitrogen molecules.

cond-mat.mes-hall↗

arXiv2013

The specific heat and the radial thermal expansion of bundles of single-walled carbon nanotubes

The specific heat at constant pressure of bundles of single-walled carbon nanotubes closed at their ends has been investigated in a temperature interval of 2-120 K. It is found that the curve of heat capacity has features near 5, 36, 80, and 100 K. The experimental results on the heat capacity and the radial thermal expansion coefficient of bundles of SWNTs oriented perpendicular to the sample axis have been compared. It is found that the curves of the heat capacity and the radial thermal expansion coefficient exhibit a similar temperature behavior above 10 K. The temperature dependence of the Gruneisen coefficient has been calculated. The curve of the Gruneisen coefficient also has a feature near 36 K. Above 36 K the Gruneisen coefficient is practically independent of temperature. Below 36 K the Gruneisen coefficient decreases monotonically with lowering temperature and becomes negative below 6 K.

cond-mat.mes-hall↗