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Papers on “room temperature superconductivity materials”

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1. Hydrogen Clathrate Structures in Rare Earth Hydrides at High Pressures: Possible Route to Room-Temperature Superconductivity.

   Feng Peng, Ying Sun, Chris J. Pickard, et al. · 2017 · Physical review letters · 564 cites

2. Room-temperature superconductivity in a carbonaceous sulfur hydride

   Elliot Snider, N. Dasenbrock-Gammon, Raymond McBride, et al. · 2020 · Nature · 481 cites

3. The 2021 room-temperature superconductivity roadmap

   L. Boeri, R. Hennig, P. Hirschfeld, et al. · 2021 · Journal of Physics: Condensed Matter · 165 cites

   Designing materials with advanced functionalities is the main focus of contemporary solid-state physics and chemistry. Research efforts worldwide are funneled into a few high-end goals, one of the oldest, and most fascinating of which is the search for an ambient temperature superconductor (A-SC). The reason is clear: superconductivity at ambient conditions implies being able to handle, measure and access a single, coherent, macroscopic quantum mechanical state without the limitations associated with cryogenics and pressurization. This would not only open exciting avenues for fundamental research, but also pave the road for a wide range of technological applications, affecting strategic area

4. Can Doping Graphite Trigger Room Temperature Superconductivity? Evidence for Granular High‐Temperature Superconductivity in Water‐Treated Graphite Powder

   T. Scheike, W. Böhlmann, P. Esquinazi, et al. · 2012 · Advanced Materials · 77 cites

5. Hole-doped room-temperature superconductivity in H3S1-xZ (Z=C, Si)

   Yanfeng Ge, Fan Zhang, R. Dias, et al. · 2020 · arXiv: Superconductivity · 62 cites

   We examine the effects of the partial substitution of S atoms by C and Si atoms on the superconductivity of H$_3$S with the $Im\bar{3}m$ structure at megabar pressure. The low-level substitution can fine-tune the Fermi energy to reach the electronic density-of-states peak maximizing the electron-phonon coupling. This can boost the critical temperature from the original 203 K to 289 K and 283 K, respectively, for H$_3$S$_{0.962}$C$_{0.038}$ at 260 GPa and H$_3$S$_{0.960}$Si$_{0.040}$ at 230 GPa. The former may provide an explanation for the recent experimental observation of room-temperature superconductivity in a highly compressed C-S-H system [Nature 586, 373-377 (2020)]. Our work opens a n

6. Room Temperature Superconductivity: the Roles of Theory and Materials Design

   W. Pickett · 2022 · 48 cites

   For half a century after the discovery of superconductivity, materials exploration for better superconductors proceeded without knowledge of the underlying mechanism. The 1957 BCS theory cleared that up: the superconducting state occurs due to pairing of electrons over the Fermi surface. Over the following half century higher critical temperature T$_c$ was achieved only serendipitously as new materials were synthesized. Meanwhile the formal theory of phonon-coupled superconductivity at the material-dependent level became highly developed: given a known compound, its value of T$_c$, the superconducting gap function, and several other properties of the superconducting state became available in

7. Lifshitz transitions and zero point lattice fluctuations in sulfur hydride showing near room temperature superconductivity

   Antonio Bianconi, Thomas Jarlborg · 2015 · Novel Superconducting Materials · 27 cites

   AbstractEmerets’s experiments on pressurized sulfur hydride have shown that H3S metal has the highest known superconducting critical temperature Tc = 203 K. The Emerets data show pressure induced changes of the isotope coefficient between 0.25 and 0.5, in disagreement with Eliashberg theory which predicts a nearly constant isotope coefficient.We assign the pressure dependent isotope coefficient to Lifshitz transitions induced by pressure and zero point lattice fluctuations. It is known that pressure could induce changes of the topology of the Fermi surface, called Lifshitz transitions, but were neglected in previous papers on the H3S superconductivity issue. Here we propose thatH3S is a mult

8. Room temperature superconductivity dome at a Fano resonance in superlattices of wires

   Maria Vittoria Mazziotti, T. Jarlborg, A. Bianconi, et al. · 2021 · Europhysics Letters · 14 cites

   Recently room temperature superconductivity with degrees Celsius has been discovered in a pressurized complex ternary hydride, CSH x , which is a carbon- and hydrogen-doped H3S alloy. The nanoscale structure of H3S is a particular realization of the 1993 patent claim of superlattice of quantum wires for room temperature superconductors and the maximum T C occurs at the top of a superconducting dome. Here we focus on the electronic structure of materials showing nanoscale heterostructures at the atomic limit made of a superlattice of quantum wires like hole-doped cuprate perovskites, and organics focusing on A15 intermetallics and pressurized hydrides. We provide a perspective of the theory o