Search arXivSearch

arXiv · 2106.10732

Aspects of strong electron-phonon coupling in superconductivity of compressed metal hydrides MH6 with Im-3m structure

Abstract

Recently YH6, compound from a group of theoretically predicted stable compressed MH6 hydrides (M/ Ca, Mg, Y, Sc) with bcc Im-3m crystal structure, was successfully experimentally realized. Superconductivity of pressurized YH6 was confirmed experimentally, Tc / 224 K at 166 GPa, but with critical temperature considerably lower than value predicted by Migdal-Eliashberg (ME) theory. Here we present theoretical reinvestigation of superconductivity in MH6 hydrides. Our results confirm that YH6 and ScH6 with Im-3m structure at corresponding GPa pressures are superconductors but with an antiadiabatic character of superconducting ground state and a multiple gap structure in one-particle spectrum. Transition into superconducting state is driven by strong electron-phonon coupling with phonon modes of H atom vibrations. Based on antiadiabatic theory, calculated critical temperature in YH6 is 231 K which is by 7 K higher than experimental value. For ScH6 calculated critical temperature is 196 K, which is in this case higher by 27 K than former theoretical prediction -169 K.Important results of applied antiadiabatic theory concerns CaH6 and MgH6 in Im-3m structure at corresponding GPa pressures. Theory indicates that these hydrides are not superconductors. It is in sharp contradiction to former predictions based on ME theory which for these hydrides calculated not only Tc well above 200 K, but for MgH6 critical temperature was predicted substantially higher than 300 K. Unfortunately, high pressure synthesis of CaH6, MgH6 nor ScH6, in Im-3m structure has not been realized until present.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Pavol Baňacký, Jozef Noga. 2021-09-03. Aspects of strong electron-phonon coupling in superconductivity of compressed metal hydrides MH6 with Im-3m structure. https://doi.org/10.1063/5.0062162

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Short-Range Modulated Electron Lattice and d-Wave Superconductivity in Cuprates: A Phenomenological Ginzburg-Landau Framework

A short-range charge modulation near 0.3 reciprocal lattice units along the Cu-O bond is present in every hole-doped cuprate family. Resonant x-ray scattering now shows that superconductivity does two opposite things to it at once: below Tc the modulation weakens yet becomes more phase coherent. We trace this split to symmetry: the modulation's envelope carries lattice momentum, which leaves a d-wave condensate exactly two ways to couple to it at quartic order, through the modulation's amplitude or through its phase. The first moves amplitude, coherence, and superfluid stiffness together; the second buys coherence at the expense of stiffness, so the two are separately measurable. We call this Ginzburg-Landau framework the modulated electron lattice (MEL). Classical Monte Carlo on 120x120 lattices with quenched disorder places the x-ray observation, read as a single component, at competing amplitude coupling and cooperative phase coupling, where the model gives no stiffness gain. But the measured intensity sums bond-centred and site-centred components. A two-component simulation gives the same pair of bulk signatures, intensity down and coherence up, both with a stiffness loss and with a stiffness gain, depending on the strength of the bond channel. Bulk data therefore cannot say whether this charge order stiffens the superconductor or softens it. What settles the question is the bond-channel amplitude, which form-factor-resolved scattering and phase-resolved tunnelling measure. The response follows the local pairing amplitude, so its onset need not be sharp at Tc. We also compute vortex pinning in the modulated landscape and obtain an in-plane penetration depth of about 124 nm once the transition temperature fixes the energy scale. This version corrects the first: its linear envelope coupling was symmetry-forbidden, and all numerical results are new.

cond-mat.supr-con

Collective excitation-mediated transport in nanoscale Josephson junctions that exhibit quantum confinement

Quantum confinement can strongly modify transport through Josephson junctions. Here, we study local tunneling transport through nanoscale Josephson junction stacks in the Coulomb blockade regime, where the metallic layers exhibit strong vertical quantum confinement. We find that quasiparticle transport is strongly enhanced by a collective excitation mode intrinsic to the junction and localized in the isolated metallic overlayer. We quantify both the collective-mode energy and the Coulomb gap and show that both exhibit strong layer-dependent modulation, consistent with the modulation of the underlying quantum well states. We further investigate how the collective excitation responds to various perturbations, including mechanical motion and an applied magnetic field. Our results suggest that this collective mode is sensitive to quasiparticles near the Fermi level and may therefore provide an indirect probe of the superconducting state.

cond-mat.supr-con

Universal Dzyaloshinski-Moriya interaction dictates pairing in unconventional superconductor families

The collinear-antiferromagnetic spin-fluctuation paradigm has long guided unconventional superconductivity research, yet fails to reconcile the noncollinear spin phenomena observed across cuprates, iron-based superconductors, and nickelates. Using extensive first-principles calculations and unbiased large-scale DMRG simulations, we show that Dzyaloshinski-Moriya interaction (DMI)-arising from local inversion-symmetry breaking-is a common ingredient across these families. This DMI unifies hallmark observations in parent compounds-incommensurate orders, spin-wave gaps, and noncollinear textures. Under hole doping, strong DMI drives spin vortices to merge with pi-shifted hole stripes, forming hybrid vortex-hole stripe phases. These phases stabilize charge order while supporting, not suppressing, superconductivity. By contrast, under electron doping, these vortices pin holes and suppress long-range superconductivity. Our results establish DMI as a unifying link between noncollinear magnetism and superconductivity, identifying hole-strip-vortex coupling as a microscopic pairing engine. Given that DMI is common across major superconductor families, these findings challenge the prevailing pairing mechanism and offer an experimentally testable roadmap for materials optimization.

cond-mat.supr-con