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Room-Temperature Superconductivity at 298 K in Ternary La-Sc-H System at High-pressure Conditions (2510.01273v1)

Published 29 Sep 2025 in cond-mat.supr-con and cond-mat.mtrl-sci

Abstract: Room-temperature superconductor has been a century-long dream of humankind. Recent research on hydrogen-based superconductors (e.g., CaH6, LaH10, etc.) at high-pressure conditions lifts the record of superconducting critical temperature (Tc) up to ~250 kelvin. We here report the experimental synthesis of the first-ever room-temperature superconductor by compression on a mixture of La-Sc alloy and ammonia borane at pressures of 250-260 gigapascals (GPa) via a diamond anvil cell by a laser-heating technique. Superconductivity with an onset temperature of 271-298 kelvin at 195-266 GPa is observed by the measurement of zero electrical resistance and the suppression of Tc under applied magnetic fields. Synchrotron X-ray diffraction data unambiguously reveal that this superconductor crystallizes in a hexagonal structure with a stoichiometry LaSc2H24, in excellent agreement with our previous prediction1. Through thirteen reproducible experimental runs, we provide solid evidence of the realization of a room-temperature superconductor for the first time, marking a milestone in the field of superconductivity.

Summary

  • The paper demonstrates room-temperature superconductivity up to 298 K in LaSc₂H₂₄ at pressures around 260 GPa.
  • It employs diamond anvil cell synthesis with pulsed laser heating to form a hexagonal P6/mmm composite hydrogen network.
  • The study highlights scandium’s role in stabilizing unique hydrogen cage motifs and increasing the electron density conducive to superconductivity.

Room-Temperature Superconductivity in LaSc₂H₂₄ at Extreme Pressures

Introduction

The synthesis and characterization of LaSc₂H₂₄, a ternary lanthanum-scandium superhydride, exhibiting superconductivity at and above room temperature (up to 298 K) under high-pressure conditions, represents a significant advance in the field of high-TcT_c superconductivity. This work builds on the paradigm of hydrogen-rich clathrate hydrides, extending the compositional space from binary to ternary systems, and demonstrates the critical role of compositional and structural tuning in achieving unprecedented superconducting transition temperatures.

Experimental Synthesis and Characterization

Synthesis Protocol

LaSc₂H₂₄ was synthesized by compressing a La-Sc alloy (1:2 atomic ratio) with ammonia borane (NH₃BH₃) as a hydrogen source in a diamond anvil cell (DAC), followed by pulsed laser heating at pressures of 250–260 GPa. The synthesis protocol was optimized based on prior theoretical predictions of phase stability and superconducting properties, with the target phase predicted to be thermodynamically stable above 167 GPa.

Structural Determination

Synchrotron X-ray diffraction (XRD) confirmed the formation of a hexagonal P6/mmm phase, with lattice parameters in close agreement with theoretical predictions. The structure features two distinct hydrogen cages: H₂₄ cages surrounding Sc and H₃₀ cages surrounding La, forming a nested, composite hydrogen network not observed in binary hydrides. The refined stoichiometry, LaSc₂H₂₄, was validated by lattice volume analysis, with minor deviations attributed to hydrogen non-stoichiometry and dehydrogenation during decompression.

Electrical and Magnetic Measurements

Four-probe electrical transport measurements revealed abrupt resistance drops to zero at onset temperatures (TonsetT_\text{onset}) ranging from 271 K to 298 K at pressures between 195 and 266 GPa. The zero-resistance state was reproducibly observed in multiple independent DAC runs, with the highest TcT_c (298 K) at 260 GPa. The superconducting transition was further corroborated by the suppression of TcT_c under applied magnetic fields up to 12 T, with upper critical fields Hc2(0)H_{c2}(0) extrapolated to 89–228 T depending on the fitting model (Ginzburg-Landau, WHH, or linear). The extracted coherence lengths (1.3–1.9 nm) are consistent with type-II superconductivity.

Mechanism and Role of Scandium

The introduction of Sc into the La-H system is pivotal for the observed enhancement in TcT_c. Scandium, with its lighter atomic mass and smaller radius compared to La, enables the stabilization of unique hydrogen cage motifs and increases the hydrogen-derived density of states at the Fermi level. The absence of localized ff-electrons in Sc avoids magnetic pair-breaking effects, in contrast to other rare-earth dopants (e.g., Ce, Nd). The resulting structure is not a disordered solid solution but a well-ordered, composite clathrate, which is essential for the observed superconducting properties.

Comparison with Binary and Other Ternary Hydrides

Previous records for TcT_c in hydride superconductors were held by binary LaH₁₀ (250 K at ~180 GPa) and related systems. Attempts to enhance TcT_c via random alloying or doping in binary hydrides have yielded only incremental improvements, primarily due to the lack of new structural motifs. In contrast, the LaSc₂H₂₄ phase represents a distinct structural prototype, with the formation of new hydrogen frameworks directly linked to the dramatic increase in TcT_c.

Limitations and Open Questions

  • Pressure Requirement: The necessity of pressures above 250 GPa for phase stability and high TcT_c remains a significant barrier to practical applications. The possibility of stabilizing this or related phases at lower pressures via chemical precompression or alternative compositional tuning is an open research direction.
  • Hydrogen Content and Stoichiometry: Precise determination of hydrogen positions and content is limited by current XRD capabilities. Dehydrogenation and non-stoichiometry during decompression introduce sample variability, affecting TcT_c and phase stability.
  • Direct Magnetic Characterization: While suppression of TcT_c under magnetic field is strong evidence for superconductivity, direct observation of the Meissner effect at these pressures remains technically challenging. Advances in quantum sensing and high-pressure NMR may address this gap.
  • Nature of Superconductivity: Isotope substitution (H/D) and tunneling spectroscopy are needed to definitively establish the pairing mechanism and gap symmetry, though the evidence points toward conventional phonon-mediated superconductivity.

Implications and Future Directions

The demonstration of room-temperature superconductivity in a well-characterized, structurally resolved ternary hydride provides a concrete platform for further exploration of multinary superhydrides. The results suggest that targeted compositional and structural engineering, guided by ab initio crystal structure prediction, can yield further increases in TcT_c and potentially reduce the required synthesis pressures. The unique hydrogen frameworks observed in LaSc₂H₂₄ may serve as templates for the design of new superconductors with tailored properties.

Future research should focus on:

  • Extending the compositional space to include other light elements or transition metals.
  • Developing synthesis strategies for metastable retention of high-TcT_c phases at lower pressures.
  • Employing advanced characterization techniques (e.g., high-pressure NMR, quantum magnetometry, tunneling spectroscopy) to probe the superconducting state and hydrogen sublattice.
  • Systematic isotope effect studies to confirm the conventional nature of the superconductivity.

Conclusion

The synthesis and characterization of LaSc₂H₂₄ establishes the existence of a room-temperature superconductor with a well-defined crystal structure and mechanism, underlining the potential of ternary and higher-order hydrides for achieving even higher TcT_c values. The work provides a robust experimental and theoretical framework for the rational design of next-generation superconductors, with significant implications for condensed matter physics and materials science.

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Explain it Like I'm 14

What this paper is about

This paper reports something scientists have dreamed about for over 100 years: a material that becomes a superconductor at room temperature. A superconductor lets electricity flow with zero resistance, which means no energy is lost as heat. The team says they made a new hydrogen-rich material, called LaSc2H24, that becomes superconducting around 298 K (about 25°C or 77°F). However, it only works when squeezed under extremely high pressure—about 2.5 million times the pressure of air at sea level.

The big questions the researchers asked

  • Can we actually create the predicted compound LaSc2H24 (made of lanthanum, scandium, and hydrogen) in the lab?
  • Does it really become a superconductor at room temperature under high pressure?
  • What crystal structure does it have (how are its atoms arranged)?
  • How does its superconducting temperature change with pressure and magnetic fields?

How they did it (in everyday terms)

To make and test this superconductor, the team used tools and ideas you can picture:

  • Squeezing between diamonds: They used a device called a diamond anvil cell. Imagine pressing a tiny speck of material between two super-strong diamond tips until it’s under enormous pressure—up to 260 gigapascals (GPa), which is roughly 2.5 million atmospheres.
  • Ingredients: They started with a lanthanum–scandium alloy (La and Sc metals in about a 1:2 ratio) and a solid chemical called ammonia borane (NH3BH3), which is good at releasing hydrogen when heated.
  • Flash heating: While under pressure, they heated the tiny sample with a laser for about a minute to make the elements react and form the new compound.
  • Checking if it’s superconducting: They measured electrical resistance using four tiny electrodes touching the sample. In a superconductor, resistance drops to zero. They also applied magnetic fields (up to 9 tesla—several times stronger than a hospital MRI) and watched the superconducting temperature go down, which is a classic sign of real superconductivity.
  • Seeing the atomic arrangement: They used synchrotron X-ray diffraction—basically, very bright X-rays—to “fingerprint” how atoms are arranged. The patterns matched a hexagonal structure called P6/mmm, consistent with LaSc2H24 that had been predicted earlier.

Helpful analogies:

  • Electron-phonon coupling: Think of electrons “surfing” on tiny vibrations of atoms; in some materials, this lets them pair up and move without resistance.
  • Hydrogen cages: The structure has hydrogen atoms forming cage-like shells around metal atoms, a bit like soccer balls surrounding marbles.

What they found and why it matters

Main results:

  • Superconductivity near room temperature: They saw the resistance drop begin (the “onset”) between 271 K and 298 K at pressures from 195 GPa to 266 GPa. In some runs, resistance went all the way to zero at around room temperature.
  • Magnetic check: When they turned on a magnetic field up to 9 T, the superconducting temperature decreased by about 11 K. That behavior—magnetic fields lowering the superconducting temperature—supports that it’s genuine superconductivity.
  • Structure match: X-ray data matched a hexagonal LaSc2H24 structure that theory had predicted, including special hydrogen “cages” (H24 around Sc and H30 around La).
  • Stability window: The phase stayed stable down to about 194 GPa; below that, signs of breakdown appeared.
  • Strong superconductor: Extrapolations suggest an “upper critical field” (the field that destroys superconductivity) that could exceed 100 T at low temperature, indicating very robust superconductivity.

Why this is important:

  • It’s the first time a material is reported to superconduct at true room temperature with clear evidence like zero resistance and magnetic-field suppression.
  • It supports a powerful design idea: mixing metals in hydrogen-rich compounds can create new “hydrogen cage” structures that boost superconductivity.

What makes LaSc2H24 special

  • Scandium’s role: Scandium is lighter and smaller than lanthanum but has similar outer electrons, which helps build new hydrogen cage types and can strengthen the electron–vibration “glue” that pairs electrons.
  • Unique hydrogen cages: The structure forms two new cage types—H24 and H30—that pack lots of hydrogen close to the metals. Hydrogen’s light mass helps raise the superconducting temperature.

What this could mean next

  • Big promise, big challenge: Room temperature is a huge milestone, but the required pressure (hundreds of GPa) is far beyond everyday use. The next goal is to find ways to keep or approach this behavior at much lower pressures.
  • Design roadmap: The success of a ternary hydride (La + Sc + H) suggests exploring more “three-element” and multi-element hydrides to discover even better superconductors.
  • More tests to cement the case: Future work could include:
    • Isotope tests (replacing hydrogen with deuterium) to check the expected shift in superconducting temperature.
    • Direct magnetic measurements of the Meissner effect at these high pressures.
    • Tunneling spectroscopy to measure the superconducting energy gap.

In short: The authors present strong evidence that LaSc2H24 is a room-temperature superconductor under extreme pressure, with a crystal structure that matches predictions. If confirmed and extended to lower pressures, this approach could move us closer to practical, lossless power systems, faster electronics, and powerful magnets—transforming how we use energy and build technology.

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Knowledge Gaps

Below is a concise list of the paper’s unresolved knowledge gaps, limitations, and open questions to guide future work:

  • Lack of direct magnetic confirmation of superconductivity (Meissner effect) at >200 GPa; no AC susceptibility or NV-center magnetometry measurements reported.
  • No isotope-substitution (H→D) paper to test the phonon-mediated (conventional) mechanism and quantify the isotope coefficient α.
  • Hydrogen positions are not experimentally resolved; XRD refinement constrains only the metal sublattice, leaving the H24/H30 cage topology unverified.
  • Hydrogen stoichiometry is inferred indirectly from lattice volume with significant uncertainty; no direct quantification (e.g., high-pressure NMR, inelastic X-ray scattering) of H content or site occupancy.
  • Absence of tunneling spectroscopy (e.g., high-pressure point-contact or planar) to measure the superconducting gap Δ(T), coupling strength (2Δ/kBTc), and gap symmetry.
  • No phonon spectra (Raman/IR/IXS) under identical conditions to correlate electron-phonon coupling with Tc.
  • Upper critical field Hc2(0) is extrapolated from low fields (≤9 T); high-field measurements are needed to validate Hc2 magnitude, Pauli limiting, and possible strong-coupling effects.
  • Anisotropy of superconductivity (Hc2 anisotropy for hexagonal lattice) is not determined; field-orientation-dependent data are missing.
  • Critical current density Jc, current–voltage characteristics, and self-field/flux-pinning behavior are unmeasured.
  • Absolute resistivity and residual resistivity ratio (RRR) are not reported due to unknown sample geometry/thickness; transport is discussed only in relative terms.
  • Transition widths and criteria (onset vs mid vs zero) are not systematically quantified; broadening and cell-to-cell variability of transitions remain unexplained.
  • Negative resistance and anomalous features at ~195 GPa indicate possible circuit or sample instabilities; the origin and mitigation strategies are not established.
  • Pressure–temperature–composition phase diagram is incomplete; the optimal pressure range, Tc dome, and decomposition boundaries are not mapped.
  • Synthesis window is narrow and very high (≈250–260 GPa); it remains unknown whether LaSc2H24 can be reproducibly synthesized at lower pressures or via alternative hydrogen sources/paths.
  • Reaction pathway and kinetics during laser heating are uncharacterized (e.g., transient phases, target temperatures, time–temperature profiles); synthesis parameters vs phase purity are not systematized.
  • Phase purity is not rigorously established; the possible presence of LaH10 or other La–Sc–H/B/N phases (from NH3BH3) is not excluded by in-situ chemical/structural mapping.
  • Potential incorporation of B/N from ammonia borane is not assessed; no post-reaction chemical analysis to exclude ternary/quaternary contaminants.
  • Microstructural features (grain size, texture, strain) and their impact on transport are not characterized; single-crystal-like diffraction hints at preferred orientation but is not followed up.
  • Dehydrogenation upon decompression is inferred but not directly tracked chemically; the dependence of Tc on hydrogen off-stoichiometry x in LaSc2H24±x is unquantified.
  • Structural evolution below ~194 GPa (peak splitting, partial decomposition) is not resolved into identifiable phases by XRD; the nature and superconductivity of decomposition products are unknown.
  • No time-dependent stability/aging data at fixed P,T; the role of diffusion-driven hydrogen loss and its kinetics on Tc and structure is not quantified.
  • Mechanistic claims (Sc enabling novel H24/H30 cages and enhanced DOS/EPC) are not experimentally corroborated by spectroscopy or direct H-site imaging.
  • No comparison between measured properties (Tc(P), dHc2/dT, Δ) and ab initio anharmonic EPC calculations for the experimentally refined lattice parameters.
  • Magnetic impurities and their effect on Tc (e.g., from gasket, electrodes, Sc/La impurities) are not analyzed; no magnetic characterization of the normal state.
  • Penetration depth λ, coherence length ξ (beyond GL estimate), and Ginzburg–Landau parameter κ are not measured; type-II character is inferred but not fully quantified.
  • Thermal transport (κ) and heat-capacity signatures (jump at Tc) are unmeasured, leaving thermodynamic confirmation open.
  • Reproducibility across laboratories is untested; independent replication and inter-lab standards for measurements/analysis are absent.
  • Influence of La:Sc ratio deviations and controlled substitution (e.g., partial replacement of La or Sc) on structure stability and Tc is unexplored.
  • Relationship between this stoichiometric LaSc2H24 phase and reported substituted-type (La,Sc)H12 phases near ~190 GPa is unclear; no systematic structural/compositional taxonomy across pressures.
  • Electrode/sample interface effects and potential extrinsic artifacts (e.g., contact resistance evolution under P,T, possible Pt hydride formation) are not ruled out via complementary geometries or contact-insensitive methods.
  • Hall effect and carrier density/mobility in the normal state are not measured, leaving the electronic structure (e.g., multiband behavior) unconstrained.
  • Environmental robustness (exposure sensitivity, quenchability, retrievability, cycling endurance) and pathways toward lower-pressure or ambient-pressure stabilization are not addressed.
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Practical Applications

Below is an overview of practical, real-world applications that flow from the paper’s findings, methods, and innovations. Items are grouped by immediacy and, where relevant, linked to sectors. Each entry notes key assumptions or dependencies affecting feasibility.

Immediate Applications

  • High-pressure superconductivity testbeds and workflows for discovery (academia; instrumentation; software)
    • Use the demonstrated DAC + laser-heating protocol with ammonia borane and CALYPSO-guided targets to rapidly explore multinary superhydrides beyond binary LaH10, focusing on cage engineering (H24/H30) and atomic-radius mismatch.
    • Tools/workflows: standardized DAC synthesis procedures; four-probe transport with cryogen-free magnets; synchrotron-based micro-XRD refinement pipelines; iterative theory–experiment loops using CALYPSO/DFT.
    • Dependencies: access to megabar DAC infrastructure (≥200 GPa), synchrotron beamlines, and high-power lasers; micrometer-scale sample handling; specialized expertise; reproducibility across laboratories.
  • Structure-guided materials design principles for hydride superconductors (academia; software; education)
    • Apply the “nested hydrogen cage” motif and metal-site differentiation (MgB2-type sublattice with La@H30 and Sc@H24) as a design heuristic to predict new high-Tc candidates (e.g., La–Sc–X systems).
    • Tools/products: computational screening platforms integrating CALYPSO, phonon/electron-phonon coupling and anharmonicity modules; course modules or training kits for high-pressure materials design.
    • Dependencies: high-throughput HPC resources; robust anharmonic calculations; validated crystal-chemistry rules (e.g., atomic-radius mismatch thresholds).
  • Instrumentation innovation and commercialization opportunities (industry: precision hardware; sensors)
    • Demand for improved DACs, pulsed-laser heating optics, pressure metrology (Raman edge calibrations), and microelectrode fabrication for ultrahigh pressure transport.
    • Near-term productization: NV-center diamond anvils for magnetometry above 200 GPa; high-pressure NMR probes to resolve hydrogen positions; integrated cryogen-free field systems tailored for DACs.
    • Dependencies: manufacturing tolerances and reliability at multimegabar pressures; sensitivity of sensors for ~10–20 µm samples; alignment and thermal management in constrained geometries.
  • Verification and standards for high-pressure superconductivity claims (policy; academia)
    • Establish community protocols emphasizing multi-signal validation (zero resistance, field suppression, eventual Meissner imaging), independent replication, and open data (raw resistance traces, XRD fits, EOS).
    • Tools/workflows: inter-lab round-robin validation; repositories for DAC metadata, pressure calibrations, and EOS-based hydrogen-content estimates.
    • Dependencies: consensus among journals/funders; secure data-sharing platforms; access to reference materials and calibrants.
  • EOS-based hydrogen content estimation as an operational workflow (academia; software)
    • Use lattice-volume expansion relative to elemental volumes (La, Sc, H) to estimate hydrogen stoichiometry in superhydrides where direct H-positioning is limited.
    • Tools: plug-in calculators for EOS curve fitting and hydrogen-content back-calculation, embedded in refinement packages (e.g., GSAS-II).
    • Dependencies: accurate elemental volume references at target pressures; error handling for pressure gradients and sample inhomogeneity.
  • Workforce development in extreme-conditions materials (education; academia; industry)
    • Train students and engineers in DAC operation, laser heating, micro-XRD analysis, and transport under high fields; design lab curricula aligned with the protocols reported.
    • Tools: hands-on modules, virtual/remote beamline sessions; simulation environments mimicking DAC workflows.
    • Dependencies: institutional access to beamlines and high-pressure facilities; safety frameworks for hydrogen sources; funding for specialized training.

Long-Term Applications

  • Scalable, room-temperature superconductors for energy transmission and storage (energy; utilities; policy; daily life)
    • Lossless power grids, compact transformers, and low-heat data centers contingent on stabilizing high-Tc phases at ambient or near-ambient pressures or via chemical/structural stabilization.
    • Products: superconducting cables without cryogenics; fault-current limiters; high-efficiency grid components.
    • Dependencies: achieving ambient-pressure stability or practical pressure-retention strategies; manufacturable bulk or wire forms; mechanical robustness and jointing methods; safety/regulatory approvals.
  • Next-generation magnets and transport systems (healthcare; transportation; robotics; industry)
    • Room-temp MRI/NMR systems, maglev transport, compact high-field motors, and actuators using type-II superconductors with very high upper critical fields (Hc2).
    • Products: cryogen-free medical imaging suites; high-field laboratory magnets; maglev infrastructure; lightweight robotic actuators.
    • Dependencies: scalable conductor forms; flux pinning engineering; AC loss mitigation; economic viability compared with existing cryogenic superconductors.
  • Low-power, high-performance electronics and computing (software/hardware; semiconductors; quantum)
    • Superconducting interconnects, logic elements, and high-speed links at ambient temperature; hybrid classical–quantum architectures with reduced thermal loads.
    • Products: superconducting processors/interposers; ultra-low-noise amplifiers; energy-efficient data-center interconnects.
    • Dependencies: materials compatible with device fabrication; stable thin films/coatings; integration with CMOS processes; long-term reliability; standardized packaging.
  • Fusion and high-energy physics enabling components (energy; research infrastructure)
    • Room-temperature superconducting coils for compact fusion devices; accelerators with reduced operational overhead.
    • Products: high-field tokamak/stellarator magnets; lighter accelerator modules.
    • Dependencies: conductor availability at scale; radiation tolerance; mechanical and thermal stability under large Lorentz forces.
  • Chemical precompression and metastability engineering for ambient performance (academia; industry)
    • Use ternary/multinary alloying, lattice-site engineering, and hydrogen cage stabilization (H24/H30 analogs) to lower required pressures or lock-in phases via kinetic barriers.
    • Tools/workflows: dopant selection guided by atomic-radius mismatches and valence electron configurations; in situ quenching; thin-film epitaxy under pressure; encapsulation strategies.
    • Dependencies: validated pathways from megabar to moderate/ambient pressures; retention of superconducting properties during decompression; avoidance of dehydrogenation.
  • Industrialization of extreme-pressure manufacturing (industry; policy)
    • Develop scalable high-pressure platforms (e.g., multi-anvil arrays, continuous high-pressure reactors) for batch synthesis of superhydrides or precursors that can be released at lower pressures.
    • Products: high-throughput high-pressure synthesis lines; pressure-retaining casings for components.
    • Dependencies: engineering breakthroughs in pressure generation beyond laboratory DACs; cost and energy economics; safety standards and certifications.
  • Standards and regulation for superconducting infrastructure at ambient temperatures (policy; finance; utilities)
    • Frameworks for grid integration, safety codes, insurance, and procurement once ambient or moderate-pressure superconductors become manufacturable.
    • Tools/workflows: certification protocols; lifecycle assessments; public–private funding models.
    • Dependencies: mature supply chains; proven reliability; interoperability with current grid and medical/transport standards.
  • Advanced characterization ecosystems for hydrogen-rich materials (academia; instrumentation; software)
    • Routine Meissner imaging above 200 GPa, high-pressure tunneling spectroscopy for gap measurements, and high-pressure NMR for hydrogen sites to accelerate validation.
    • Products: NV-anvil magnetometers; compact high-pressure spectrometers; data-analysis suites for anharmonic superconductivity.
    • Dependencies: sensor sensitivity and durability at multimegabar pressures; alignment with small samples; community adoption and training.

Assumptions and cross-cutting dependencies:

  • Current realization requires ultrahigh pressures (≈195–266 GPa), micrometer-scale samples, and specialized facilities; ambient or manufacturable conditions are not yet available.
  • Superconductivity is confirmed via zero resistance and magnetic-field suppression; direct Meissner-effect imaging at these pressures remains challenging but advancing.
  • Hydrogen stoichiometry and stability can vary with pressure and time (de-hydrogenation); EOS-based estimates carry uncertainties.
  • Scaling from proof-of-concept to products hinges on stabilizing phases at lower pressures, developing bulk or wire forms, ensuring mechanical robustness, and establishing supply chains and standards.
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Glossary

  • Akahama diamond Raman calibration: A pressure calibration method using the Raman edge of diamond, as established by Akahama, to determine pressures in diamond anvil cells. "Pressures were determined from the room-temperature first-order diamond Raman edge calibrated by Akahama74 75."
  • Alloy superhydrides: Non-stoichiometric hydrides where different metal atoms form an alloy within a hydrogen-rich lattice. "non-stoichiometric alloy superhydrides (e.g. (La, Y)H6, (La, Y)H10 (ref. 49), (La,Ce)H9-10 (refs 50,51), (La,Nd)H10 (ref. 52), (La,Sc)H12 (ref.53), and (La,Ca)H10 (ref. 54)"
  • Anharmonic approximation: A theoretical treatment that includes deviations from harmonic (ideal) lattice vibrations, important for accurate phonon and superconductivity predictions under extreme conditions. "based on anharmonic approximation1, which significantly impacts dynamic stability, phonon frequencies, and superconductivity25,33,34."
  • Antibonding states: Electronic states that, when occupied, weaken or oppose chemical bonding; their population can alter electronic properties. "hydrogen transforms from bonding to antibonding states, resulting in a high density of states at the Fermi level and enhancement of electron-phonon coupling."
  • CALYPSO (crystal structure prediction) method: A computational algorithm for predicting stable crystal structures under given conditions. "our theoretical study employing the crystal structure prediction (CALYPSO) method proposed a ternary high-Tc superhydride, LaSc2H24 (ref. 1)"
  • CeO2 standard: A calibration material (cerium dioxide) used to set geometric parameters in X-ray diffraction experiments. "The sample-to-detector distance and other geometric parameters were calibrated using a CeO2 standard."
  • Clathrate hydride: A hydrogen-rich structure where hydrogen forms cage-like frameworks enclosing metal atoms. "The 'clathrate hydride' paradigm was originally proposed for CaH6 in 2012 (ref. 19)"
  • Coherence length: The characteristic size over which superconducting pairs (Cooper pairs) remain correlated; related to the upper critical field. "The GL coherence length, derived from Hc2(0), is 1.70-1.92 nm, indicating that the synthesized superconducting hydride is a typical type-II superconductor."
  • Co-magnetron sputtering: A thin-film deposition technique using multiple sputtering targets to co-deposit different elements. "The precursor La-Sc alloy was prepared either by melting or double target co-magnetron sputtering."
  • Cooper pairs: Bound electron pairs responsible for superconductivity in conventional superconductors. "T decreases progressively with increasing fields due to the breaking of Cooper pairs via orbital and spin- paramagnetic effects."
  • Crystal structure prediction methods: Computational techniques to identify likely stable crystal structures before experiments. "until the advent of crystal structure prediction methods transformed the landscape."
  • Culet: The small, flat tip of a diamond anvil that contacts the sample at ultra-high pressures. "The edges of the La-Sc alloy precursor and diamond culet are marked with yellow and red dotted lines, respectively."
  • De-hydrogenation: Loss of hydrogen from a hydride compound, often occurring during pressure changes. "We also observed probable de-hydrogenation of the synthesized LaSc2H24+x (x ~- 1.1-1.4) during decompression"
  • Density of states at the Fermi level: The number of electronic states available at the Fermi energy; higher values can enhance superconductivity. "resulting in a high density of states at the Fermi level and enhancement of electron-phonon coupling."
  • Diamond anvil cell (DAC): A device that compresses tiny samples to extreme pressures between two diamond tips. "La-Sc alloy hydride was synthesized via the reaction of La-Sc alloy with NH3BH3 (Sigma-Aldrich, 97%) in a diamond anvil cell (DAC)."
  • Diamagnetism: A form of magnetism where materials create an opposing magnetic field when exposed to an external one; key to the Meissner effect. "Recently, diamagnetism associated with the Meissner effect was successfully detected in CeH9 up to about 140 GPa using nitrogen-vacancy quantum sensors implanted directly within anvil72."
  • Electron-phonon coupling: Interaction between electrons and lattice vibrations; central to conventional superconductivity. "resulting in a high density of states at the Fermi level and enhancement of electron-phonon coupling."
  • Energy-dispersive X-ray spectroscopy (EDS): An analytical technique to determine elemental composition using X-ray emission. "equipped for the energy dispersive X-ray spectroscopy (EDS)."
  • Equation of state (EOS): The relationship between pressure, volume, and temperature for a material, used to assess structural stability. "we constructed the equation of state (EOS) for the synthesized LaSc2H24 (Fig. 4(b))."
  • Fermi level: The highest occupied energy level at absolute zero; crucial for electronic properties. "resulting in a high density of states at the Fermi level and enhancement of electron-phonon coupling."
  • Four-probe van der Pauw method: A technique to measure material resistivity that minimizes contact resistance effects. "Resistances were measured via the four-probe van der Pauw method to eliminate contributions from sources other than the samples"
  • Ginzburg-Landau (GL) model: A phenomenological theory describing superconductivity near the critical temperature, used to estimate critical fields and coherence lengths. "using the Ginzburg-Landau (GL)62,63 model"
  • Gigapascal (GPa): A unit of pressure equal to one billion pascals, commonly used in high-pressure physics. "pressures of 250-260 gigapascals (GPa) via a diamond anvil cell"
  • Hexagonal close-packed (hcp) lattice: A crystal structure where atoms are closely packed in a hexagonal arrangement. "can be indexed by a hexagonal close-packed (hcp) lattice"
  • Hume-Rothery rule: Empirical rules relating atomic size mismatch to solid solution formation and stability. "surpassing the 15% limit specified by the Hume- Rothery rule71."
  • Hydrogen cages (H24, H30): Specific hydrogen cage configurations surrounding metal atoms in clathrate hydrides. "resulted in the formation of two previously unreported hydrogen cages: H24 surrounding Sc and H30 surrounding La."
  • Inductively coupled plasma atomic emission spectroscopy: A technique for quantitative chemical analysis using plasma to excite atoms and measure their emission. "were confirmed by inductively coupled plasma atomic emission spectroscopy (Thermo Fisher iCAP PRO)"
  • Interstitial sites: Positions within a crystal lattice where smaller atoms can reside between the main lattice atoms. "or occupy interstitial sites within the parent binary hydrides."
  • Isotope substitution: Replacing an element with its isotope to probe mechanisms (e.g., phonon-mediated superconductivity). "the isotope substitution of hydrogen with deuterium could verify its conventional superconductivity."
  • Laser heating: Using focused laser light to raise the temperature of a sample, often inside a DAC. "Two-sided laser-heating experiments were performed using a pulsed YAG laser (1064 nm) with a spot size of ~10 um in diameter."
  • Meissner effect: The expulsion of magnetic flux from a superconductor upon transition to the superconducting state. "The Meissner effect, which describes the expulsion of magnetic flux from a superconductor, serves as key evidence for superconductivity alongside zero resistance."
  • Metastable: A state that is not the most stable thermodynamically but persists for observable timescales under given conditions. "and remains metastable above ~194 GPa at room temperature."
  • MgB2-type structure: A structural motif similar to magnesium diboride, used here to describe metal sublattice arrangement. "where La and Sc atoms occupy lattice sites of an MgB2-type structure"
  • Nitrogen-vacancy quantum sensors: Quantum defects in diamond used as sensitive magnetic field sensors under extreme conditions. "using nitrogen-vacancy quantum sensors implanted directly within anvil72."
  • Onset temperature (T.onset): The temperature at which the resistance first begins to drop, marking the start of the superconducting transition. "Superconductivity, with a maximum onset temperature (T.onset) of 298 K, was confirmed"
  • P6/mmm symmetry: A hexagonal space group designation describing the symmetry of the crystal lattice. "featuring hexagonal P6/mmm symmetry."
  • Phonon frequencies: The vibrational mode frequencies of a crystal lattice; crucial for electron-phonon mediated superconductivity. "which significantly impacts dynamic stability, phonon frequencies, and superconductivity25,33,34."
  • Rhenium gasket: A hard metal gasket used in DAC experiments to contain the sample at high pressures. "A rhenium gasket (thickness of 250 um) was precompressed to about 20 GPa to make an indent"
  • Rietveld refinement: A method to refine crystal structures by fitting calculated patterns to powder X-ray diffraction data. "Rietveld refinements were done using GSAS-II and EXPGUI packages77."
  • Solid solution: A homogeneous crystalline phase where different atoms share lattice sites, often with disorder. "leading to a disordered solid solution where the two metals randomly occupy equivalent sublattice positions"
  • Spin-paramagnetic effects: Pair-breaking effects due to Zeeman splitting of electron spins in a magnetic field, reducing Tc. "due to the breaking of Cooper pairs via orbital and spin- paramagnetic effects."
  • Stoichiometry: The exact atomic composition of a compound. "with a stoichiometry LaSc2H24, in excellent agreement with our previous prediction1."
  • Superhydride: An extremely hydrogen-rich compound, often with unusually high hydrogen content per metal. "Electrical transport measurements of the synthesized superhydride in cells 1, 3, 4, and 5 under different pressures."
  • Synchrotron X-ray diffraction: High-brightness XRD using synchrotron radiation to determine crystal structures under extreme conditions. "Synchrotron X-ray diffraction data unambiguously reveal that this superconductor crystallizes in a hexagonal structure"
  • Ternary hydrides: Hydrides comprising three elements, offering more structural and electronic tunability than binary hydrides. "Compared with binary hydrides, ternary hydrides have attracted growing interest owing to their greater elemental diversity and structural complexity36-38"
  • Tunneling spectroscopy: A technique to probe electronic density of states and superconducting gaps via quantum tunneling. "advanced ultra- high-pressure tunneling spectroscopy may uncover the superconducting gap"
  • Type-II superconductor: A superconductor that allows magnetic flux penetration in quantized vortices above a lower critical field. "indicating that the synthesized superconducting hydride is a typical type-II superconductor."
  • Upper critical magnetic field (Hc2): The magnetic field above which superconductivity is fully suppressed. "the upper critical magnetic field (uoHc2(T))"
  • Werthamer-Helfand-Hohenberg (WHH) model: A theory used to estimate Hc2 considering orbital and spin effects. "using the Werthamer-Helfand-Hohenberg (WHH)64 model"
  • Zeolite networks: Porous, cage-like frameworks known in silicates; referenced for comparison to hydrogen cage structures. "both of which are not observed in known clathrate or zeolite networks."
  • Zero electrical resistance: The defining transport signature of superconductivity where resistivity drops to zero. "the measurement of zero electrical resistance"
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