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Strong laser pulses can control superconductivity, inducing nonequilibrium transient pairing by leveraging strong-light matter interaction. Here, we demonstrate theoretically that equilibrium ground-state phonon-mediated superconductive pairing can be affected through the vacuum fluctuating electromagnetic field in a cavity. Using the recently developed ab initio quantum electrodynamical density-functional theory approximation, we specifically investigate the phonon-mediated superconductive behavior of MgB[Formula: see text] under different cavity setups and find that in the strong light-matter coupling regime its superconducting transition temperature T[Formula: see text] can be enhanced at most by [Formula: see text]10% in an in-plane (or out-of-plane) polarized and realistic cavity via photon vacuum fluctuations. The results highlight that strong light-matter coupling in extended systems can profoundly alter material properties in a nonperturbative way by modifying their electronic structure and phononic dispersion at the same time. Our findings indicate a pathway to the experimental realization of light-controlled superconductivity in solid-state materials at equilibrium via cavity materials engineering.
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http://dx.doi.org/10.1073/pnas.2415061121 | DOI Listing |
Adv Mater
July 2025
Department of Physics and Astronomy, Center for Materials Theory, Rutgers University, Piscataway, NJ, 08854, USA.
Fundamental upper bounds on the electron-phonon interaction strength and superconducting transition temperature T in metals are established based on the intrinsic instability of the equilibrium between electrons and the crystal lattice under strong interaction. This instability explains why observed electron-phonon coupling constants are limited to λ ≲ 4. The theory also accounts for the mechanism of metastable superconductivity with enhanced T, which emerges near the instability threshold.
View Article and Find Full Text PDFSci Rep
July 2025
Extreme Conditions Physics Research Laboratory and Center of Excellence in Physics of Energy Materials (CE:PEM), Department of Physics, Faculty of Science, Chulalongkorn University, Bangkok, 10330, Thailand.
Predicting high-temperature superconductivity in hydrogen-rich dense metallic states under pressure remains a significant challenge. The discovery of new phases of metal hydrides is vital for advancing this area of research. In our study, we present the superconducting phases of ThCeH using a search strategy based on potential energy surfaces and evolutionary algorithms under pressure.
View Article and Find Full Text PDFPhys Chem Chem Phys
July 2025
School of Physics and Physical Engineering, Qufu Normal University, Qufu 273165, China.
Topological superconductivity is a fascinating quantum property in the field of condensed matter physics. The exploration of topological superconductivity in two-dimensional (2D) materials has become one of the current hot topics. Based on first-principles calculations, we predict that 2D MXC materials (M:X = In:As, Se:As, In:Te and As:Te) are thermodynamically and dynamically stable.
View Article and Find Full Text PDFNPJ Quantum Mater
June 2025
Max Planck Institute for the Structure and Dynamics of Matter, 22761 Hamburg, Germany.
The nonlinear driving of collective modes in quantum materials can lead to a number of striking non-equilibrium functional responses, which merit a comprehensive exploration of underlying dynamics. However, the coherent coupling between nonlinearly-driven modes frequently involves multiple mode coordinates at once, and is often difficult to capture by one-dimensional pump probe spectroscopy. One example is phonon-mediated amplification of Josephson plasmons in YBaCuO, a phenomenon likely associated with the mysterious superconducting-like optical response observed in this material.
View Article and Find Full Text PDFJ Chem Phys
May 2025
Institute of Atomic and Molecular Physics, Jilin University, Changchun 130023, China.
We report the discovery of two 2D Be4C3 monolayers-o-Be4C3 and m-Be4C3-as the lowest-energy structures, each exhibiting unique planar hypercoordinate carbon bonding characteristics. Both monolayers feature a C≡C triply bonded motif formed between planar tetracoordinate carbon (ptC) and planar pentacoordinate carbon (ppC) centers, coordinating with three Be atoms in o-Be4C3 and four Be atoms in m-Be4C3. Bonding analysis reveals dual behavior: the p-orbital electrons in the C≡C bonds remain primarily localized, while other ptC atoms coordinated with four Be atoms exhibit fully delocalized electron density across the Be4C framework.
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