2020
DOI: 10.1038/s42005-020-0329-z
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Moving flux quanta cool superconductors by a microwave breath

Abstract: Almost any use of a superconductor implies a nonequilibrium state. Remarkably, the nonequilibrium states induced by a microwave stimulus and the dynamics of magnetic flux quanta (Abrikosov vortices) can give rise to strikingly contrary effects: A sufficiently high-power electromagnetic field of GHz frequency can stimulate superconductivity, whereas fast vortex motion can trigger an instability abruptly quenching the superconducting state. Here, we advance or delay such dynamical quenching of the vortex state i… Show more

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Cited by 11 publications
(11 citation statements)
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“…The distinctive feature of the direct-write Nb-C superconductor is a close-toperfect edge barrier which orders the vortex motion at large current values and allows for the description of the spatial evolution of the FFI relying upon the edge-barrier-controlled FFI model. The observed high vortex velocities in Nb-C-FIBID make accessible studies of far-from-equilibrium superconductivity 61 and vortex matter driven by large currents, opening prospects for Cherenkov-like generation of other excitations by the fast-moving vortex lattice in ferromagnet/superconductor hybrid structures. In addition, the small electron diffusion coefficient D ≈ 0.5 cm 2 s −1 , the low superconducting transition temperature T c = 5.6 K, and high I c values exceeding 70% of the depairing current render Nb-C-FIBID to be an interesting candidate material for fast singlephoton detectors.…”
Section: Discussionmentioning
confidence: 99%
“…The distinctive feature of the direct-write Nb-C superconductor is a close-toperfect edge barrier which orders the vortex motion at large current values and allows for the description of the spatial evolution of the FFI relying upon the edge-barrier-controlled FFI model. The observed high vortex velocities in Nb-C-FIBID make accessible studies of far-from-equilibrium superconductivity 61 and vortex matter driven by large currents, opening prospects for Cherenkov-like generation of other excitations by the fast-moving vortex lattice in ferromagnet/superconductor hybrid structures. In addition, the small electron diffusion coefficient D ≈ 0.5 cm 2 s −1 , the low superconducting transition temperature T c = 5.6 K, and high I c values exceeding 70% of the depairing current render Nb-C-FIBID to be an interesting candidate material for fast singlephoton detectors.…”
Section: Discussionmentioning
confidence: 99%
“…[747] Furthermore, the combination of superconductors with ferromagnets in curvilinear geometries should open novel prospects for superconducting spintronics, [748] proximity-induced spin-triplet superconductivity, [651,749] magnetic cloaking, [667,750] hybrid superconductor-ferromagnetic metamaterials [751][752][753] and the improvement of current-carrying ability of superconductors. [754,755] In addition, ferromagnetic decoration of curvilinear superconductors is expected to modify the signatures of vortex guiding [756,757] and ratchet effects, [758] flux-flow instability, [722,756,759] microwavestimulated superconductivity in the vortex state, [716,760] thereby advancing the development of 3D fluxonic circuits. [29,30]…”
Section: Discussionmentioning
confidence: 99%
“…[711] We note that while the microscopic derivation of the TDGL was originally done for a gapless superconductor with paramagnetic impurities, [712] the TDGL is also widely used for studying various aspects of current-driven vortex matter in gapped superconductors with nonmagnetic impurities [710,711] including the vortex dynamics at high vortex velocities [713,714] and at GHz ac frequencies. [715,716] For in-depth discussions of the applicability of the TDGL and its mathematical aspects we refer to refs. [710,711,715,717].…”
Section: Theoretical Description: Tdgl Equationmentioning
confidence: 99%
“…Beyond I c in the flux-flow regime, vortices, which are accelerated by the Lorentz force F L = I b × φ0 with I b being the bias current and φ0 the flux quantum, can move with high velocity v, [20,21] and eventually leads to a quench of the superconducting state at I * as a consequence of vortex instability (flux-flow instability, FFI), resulting in a sudden voltage jump in the currentvoltage curves. [6,7,[22][23][24][25][26] The maximal vortex velocity is therefore associated with the FFI phenomena. Researchers have demonstrated vortex velocities of a few km/s in traditional disordered and amorphous superconducting thin films, [27][28][29][30] and slightly faster vortex dynamics in unconventional high T c thick films.…”
Section: Introductionmentioning
confidence: 99%