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Kresse \ and\ author J

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  • method The results provide direct insight into how adsorbates can quench polaron conductivity, thereby establishing a clear link between atomistic charge transport and macroscopic sensing response. 2. Methods and Model The calculations were performed using density functional theory (DFT) employing the VASP software [15,16] using the PBE exchange correlation functional [17] as well as the PBE+U approach. The valence electrons were described using a plane wave basis with a 500 eV cutoff while the effect
  • method contact the sample in the chamber. No pressure medium was used for these measurements. Pressure was determined using the ruby scale. 6 Density Functional Calculations First-principles calculations based on density functional theory (DFT) [ 16] were carried out with the PBEsol exchange-correlation energy functional [17] as it is implemented in the V ASP software [ 18]. The projector -augmented wave method (PAW) [ 19] was employed to represent the ionic cores by considering the following electroni
  • method involved in this study are isolated Cu defects, Cu-B, Cu-P, and Cu-H complexes. We also re-examine the possible configurations for CuPL. Our calculated transition levels, obtained with finite-size corrections, show good consistency with experimental observations. 2. Methods Ourcalculationswerecarriedoutusingthe VASPcode[37], based on the generalized Kohn-Sham theory and the HSE06 hybrid functional [38]. The interactions between valence electrons and ionic cores were treated with the projected- a
  • method control that does not rely on SOC [59]. We believe our findings will facilitate the exper- imental exploration of the identified candidates, paving the way for the development of next-generation spintronic devices. 4 Materials and Methods First-principles Calculations All first-principles calculations are performed using the Vienna Ab initio Simulation Pack- age [60] based on DFT. The projector augmented-wave method is employed to describe 12 the interaction between core and valence electrons [6
  • method control the band gap, optical absorption, lattice stiffness, thermal transport, and Se ebeck response under ambient condition. . 2. COMPUTATIONAL DETAILS The optoelectronic and thermoelectric properties of cubic (F -43m) and hexagonal (P63mc) aluminum antimonide (AlSb ) were investigated using density functional theory as implemented in the Vienna ab initio simulation package (VASP) [31]. The interaction between electrons and ions was described using the projector augmented -wave (PAW) method, w
  • method , Furthm¨ uller, J.: Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Computational Materials Science6(1), 15-50 (1996) https://doi.org/10.1016/0927-0256(96)00008-0 [27] Bl¨ ochl, P.E.: Projector augmented-wave method. Physical Review B50(24), 17953 (1994) https://doi.org/10.1103/physrevb.50.17953 [28] Kresse, G., Furthm¨ uller, J.: Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Physic

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Coherent spin waves in a maximal entropy phase

cond-mat.str-el · 2026-04-26 · unverdicted · novelty 7.0

In YBaCuFeO5, disorder in a maximal-entropy mixed phase favors coherent dispersive spin waves with acoustic and optical branches rather than destroying them.

Towards Non-van der Waals 2D Topological Insulators

cond-mat.mtrl-sci · 2026-04-16 · unverdicted · novelty 7.0

SbTlO3 is a non-van der Waals 2D topological insulator with 229 meV SOC splitting and band inversion, verified by topological invariants and edge states; Pb substitution places the feature at the Fermi level.

A Unified microscopic picture of cation and anion migration in MAPbI$_3$

cond-mat.mtrl-sci · 2026-05-04 · unverdicted · novelty 6.0

Molecular dynamics simulations find that both I and MA defects in MAPbI3 diffuse rapidly at room temperature with barriers of 0.15-0.20 eV, with MA interstitials moving via concerted mechanisms and no MA vacancy migration observed.

Surface ferrimagnetic order in RuO2 film

cond-mat.mtrl-sci · 2026-04-12 · unverdicted · novelty 6.0

RuO2 is non-magnetic in bulk but exhibits surface ferrimagnetism with antiparallel Ru moments of +0.48 μB and -0.04 μB on oxygen-terminated surfaces, detected via spin-ARPES and supported by DFT.

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