SearcharxivSearch

arXiv · cond-mat/0208511

On the stability of vortex-plane solitons: The solution of the problem of Josephson-vortex structure in layered superconductors and stacked junctions

Abstract

By determining the type of all stationary points of the Gibbs free energy functional for layered superconductors in parallel magnetic fields, we establish the classification of all solutions to coupled static sine-Gordon equations for the phase differences with respect to their stability. We prove that the only minimizers of the free energy are the Meissner solution (the "vacuum" state) and soliton vortex-plane solutions [S. V. Kuplevakhsky, Phys. Rev. B vol. 60, 7496 (1999); ibid. vol. 63, 054508 (2001); cond-mat/0202293]. They are the actual equilibrium field configurations. We present a topological classification of these solutions. In contrast, previously proposed non-soliton configurations ("isolated fluxons", "triangular Josephson-vortex lattices", etc.) are absolutely unstable and unobservable: They are nothing but saddle points of the Gibbs free-energy functional and are not even stationary points of the Helmholtz free-energy functional (obtained from the former by a Legendre transformation). (Physically, non-soliton configurations violate conservation laws for the current and the flux.) The obtained results allow us to explain dynamic stability of vortex planes, noticed in numerical simulations, and to provide a unified interpretation of the available experimental data. We hope that the paper will stimulate interest in the subject of specialists in different fields of physics and in applied mathematics.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Sergey V. Kuplevakhsky. 2002-08-27. On the stability of vortex-plane solitons: The solution of the problem of Josephson-vortex structure in layered superconductors and stacked junctions. https://arxiv.org/abs/cond-mat/0208511

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

KEEP EXPLORING

Related papers

Out-of-equilibrium relaxation dynamics of the superconducting order parameter in CsV$_3$Sb$_5$

The application of a time-varying strain field drives a superconducting order parameter out of equilibrium. How the order parameter relaxes back to equilibrium depends both on the structure of the superconducting gap and on the nature of quasiparticle scattering. We report the discovery of an ultrasonic attenuation peak inside the superconducting state of the kagome superconductor CsV$_3$Sb$_5$. This peak is the natural consequence of the order parameter relaxation time matching the ultrasonic drive frequency near $T_{\rm c}$. From the measured frequency dependence of the peak, we extract a microscopic scattering time of $\tau_N = 25$ ps. This timescale is two orders of magnitude longer than the elastic scattering time as determined by resistivity measurements, but is comparable to the inelastic scattering time determined by thermal transport. Within the conventional framework of order-parameter relaxation, this implies that elastic scattering is ineffective at relaxing the superconducting condensate, consistent with a sign-preserving $s$-wave state obeying Anderson's theorem.

cond-mat.supr-con

Eight-unit-cell electronic modulations in cuprates originating from local molecular orbitals

The pair density wave (PDW) state with eight-unit-cell (8a0) periodicity has been widely regarded as the primary order in cuprates, yet its existence and origin remain subjects of intense debate. Using spectroscopic imaging scanning tunneling microscopy, we observe spatial modulations of the electronic states with approximately 8a0 periodicity in both the superconducting and insulating regimes of hole-doped Ca2CuO2Cl2 cuprate. We find that the 8a0 spatial patterns are generated by the formation of molecular orbitals by doped holes, which organize into 4a0*4a0 plaquettes as the basic unit. Our results identify the 4a0 molecular orbital as the fundamental electronic building block in cuprates, while the 8a0 PDW represents a spatial subharmonic that emerges at sufficiently high doping.

cond-mat.supr-con

Record-Breaking Elemental Superconductivity in Tetralayer Kagome Borophene

Superconductivity above the liquid-nitrogen temperature remains rare in two-dimensional elemental crystals, where strong covalent bonding often yields high phonon frequencies but insufficient electron-phonon coupling. Here, using first-principles calculations and fully anisotropic Migdal-Eliashberg theory, we predict tetralayer kagome borophene (TKB) stabilized by ABAB covalent stacking, as a liquid-nitrogen-temperature elemental superconductor. With a predicted critical temperature of 102 K, TKB sets a record-high value among previously reported elemental superconductors. Unlike known high-Tc boron-based superconductors dominated by in-plane sigma-bonding states and high-frequency in-plane B-B stretching modes, TKB realizes an out-of-plane s-pz-bonding-mediated pairing mechanism, in which interlayer s-pz bonding states at the Fermi level are strongly coupled to low-frequency out-of-plane vibrations of boron atoms. These results reveal a distinct out-of-plane pairing channel in multilayer borophene and establish covalent stacking engineering as a potential route for high-Tc superconductivity in two-dimensional materials.

cond-mat.supr-con