A2B′B″O6 perovskites: A review

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The Nature Of The Chemical Bond

The electronic structure of the perovskite LaCoO$_3$ for different spin states of Co ions was calculated in the LDA+U approach. The ground state was found to be a nonmagnetic insulator with Co ions in a low-spin state. Somewhat higher in energy we found two intermediate-spin states followed by a high-spin state at significantly higher energy. The calculation results show that Co 3$d$ states of $t_{2g}$ symmetry form narrow bands which could easily localize whilst $e_g$ orbitals, due to their strong hybridization with the oxygen 2$p$ states, form a broad $\sigma^*$ band. With the increase of temperature which is simulated by the corresponding increase of the lattice parameter, the transition from the low- to intermediate-spin states occurs. This intermediate-spin (occupation $t_{2g}^5e_g^1$) can develop an orbital ordering which can account for the nonmetallic nature of LaCoO$_3$ at 90 K$<$T$<$500 K. Possible explanations of the magnetic behavior and gradual insulating-metal transition are suggested.

https://arxiv.org/pdf/cond-mat/9709060.pdf

Intermediate-spin state and properties of LaCoO_3

We assess the performance of recent density functionals for the exchange-correlation energy of a nonmolecular solid, by applying accurate calculations with the GAUSSIAN, BAND, and VASP codes to a test set of 24 solid metals and nonmetals. The functionals tested are the modified Perdew-Burke-Ernzerhof generalized gradient approximation PBEsol GGA, the second-order GGA SOGGA, and the Armiento-Mattsson 2005 AM05 GGA. For completeness, we also test more standard functionals: the local density approximation, the original PBE GGA, and the Tao-Perdew-Staroverov-Scuseria meta-GGA. We find that the recent density functionals for solids reach a high accuracy for bulk properties lattice constant and bulk modulus. For the cohesive energy, PBE is better than PBEsol overall, as expected, but PBEsol is actually better for the alkali metals and alkali halides. For fair comparison of calculated and experimental results, we consider the zeropoint phonon and finite-temperature effects ignored by many workers. We show how GAUSSIAN basis sets and inaccurate experimental reference data may affect the rating of the quality of the functionals. The results show that PBEsol and AM05 perform somewhat differently from each other for alkali metal, alkaline-earth metal, and alkali halide crystals where the maximum value of the reduced density gradient is about 2, but perform very similarly for most of the other solids where it is often about 1. Our explanation for this is consistent with the importance of exchange-correlation nonlocality in regions of core-valence overlap.

https://dspace.mit.edu/openaccess-disseminate/1721.1/51869

Assessing the performance of recent density functionals for bulk solids

We report high magnetic field scanning tunneling microscopy and Landau level spectroscopy of twisted graphene layers grown by chemical vapor deposition. For twist angles exceeding ~3° the low energy carriers exhibit Landau level spectra characteristic of massless Dirac fermions. Above 20° the layers effectively decouple and the electronic properties are indistinguishable from those in single-layer graphene, while for smaller angles we observe a slowdown of the carrier velocity which is strongly angle dependent. At the smallest angles the spectra are dominated by twist-induced van Hove singularities and the Dirac fermions eventually become localized. An unexpected electron-hole asymmetry is observed which is substantially larger than the asymmetry in either single or untwisted bilayer graphene.

Single-Layer Behavior and Its Breakdown in Twisted Graphene Layers

Using first principles density functional theory, we have studied the interaction mechanism of NO2 and SO2 gas molecules on an MoB2 monolayer, for gas sensing applications. The selectivity for a particular gas by the sensor has been analyzed through electronic structure calculations and adsorption studies. The calculations have been performed by considering the fact that the MoB2 monolayer as a sensing material encounters a change in its electrical properties, when gas molecules with different orientations get adsorbed on the surface. From the density of states study, we find better selectivity for NO2 as compared to SO2, as the latter leaves the electronic structure of the sensing material unaffected. Further, the adsorption curves support the above fact as the larger value of adsorption energy (Ead ∼ −1 eV) for NO2 indicates stronger adsorption. The chemisorptive nature for NO2, in contrast with the relatively weaker physisorption for SO2, additionally supports the fact that NO2 gas has a better perspective for MoB2 sensor application. Charge density plots for each case are in good agreement with the above conclusions. The faster recovery time attributes the MoB2 monolayer better as a sensor material for NO2 interaction.

An ab initio study of sensing applications of MoB2 monolayer: a potential gas sensor.

Structural, electrical and magnetic phase evolution of Cr substituted GdMn1−xCrxO3 (0 ⩽ x ⩽ 0.2) manganites

We report the effect of strontium (Sr) doping on dielectric, magnetization, and thermodynamic properties of polycrystalline Y1−xSrxMnO3 (x = 0.1, 0.2) samples prepared by conventional solid-state reaction method. The temperature dependent dielectric permittivity and specific heat curves noticeably show the anomalies near its magnetic transition point, i.e., Neel temperature (TN), which are probably generated by the frustrated Mn3+ spins (S = 2) on a triangular Mn lattice showing the magneto-electric coupling between the electric and magnetic orders. However, the magnetic transition is not clearly evident in the magnetic susceptibility due to the frustration on the Mn triangular lattice and the dominating paramagnetic susceptibility of the Y3+ spins. The electronic transport mechanism in these materials was analyzed within the framework of conventional Arrhenius Law, i.e., ρ(T) = C exp(Ea/kBT) applied to low frequency ac resistivity data, and through the peak method employed to the permittivity and loss ta...

Dielectric, magnetic, and thermodynamic properties of Y1−xSrxMnO3 (x = 0.1 and 0.2)

Colossal electroresistance in Sm0.55Sr0.45MnO3

We have investigated the thermal properties of electron doped perovskite manganite CaMnO3, the end member () of the Ruddlesden–Popper (RP) calcium manganates series with cation doping at the A-site. In this paper the functional relation between the lattice distortions and the thermal properties is determined and compared to available reports. The temperature dependence of the lattice specific heat (Cv(lattice)) of Ca1−xLnxMnO3 (x = 0.05, 0.10, 0.15, 0.20) with Ln(= La, Ce, Pr, Nd, Th, Bi) doping at the A-site has been studied as a function of temperature (10 K≤T≤500 K) by means of a rigid ion model (RIM) after modifying its framework to incorporate the van der Waals interactions. Strong electron–phonon interactions are present in these compounds, which are responsible for the variation of the lattice specific heat with cation doping of varying size and valency. We have found that the calculated thermal properties reproduce well the corresponding experimental data, implying that modified RIM represents properly the nature of these perovskite manganite systems. We demonstrate that the electron concentration, size mismatch and Jahn–Teller (JT) effects are the dominant factors, whereas charge mismatch and buckling of Mn–O–Mn angle influence the thermal properties to a lesser degree in the ferromagnetic state. In the insulating paramagnetic state, JT distortions vary linearly and influence the thermal properties. These specific heat results can be further improved by including the ferromagnetic spin wave and charge order contributions to the specific heat.

https://iopscience.iop.org/article/10.1088/0953-8984/21/9/096001/pdf

N. K. Gaur

Papers

An ab initio study of sensing applications of MoB2 monolayer: a potential gas sensor.

Structural, electrical and magnetic phase evolution of Cr substituted GdMn1−xCrxO3 (0 ⩽ x ⩽ 0.2) manganites

Dielectric, magnetic, and thermodynamic properties of Y1−xSrxMnO3 (x = 0.1 and 0.2)

Colossal electroresistance in Sm0.55Sr0.45MnO3

The role of lattice distortions in determining the thermal properties of electron doped CaMnO3