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   When a participant elects to relocate their LEO tokens across disparate blockchain networks, INLEO’s system implements a trust-minimized locking and minting (and conversely, burning and unlocking) architecture: specifically, a user deposits native LEO tokens into a cryptographic smart contract or analogous lock-module on the source chain; that contract irrevocably locks (escrows) those tokens, thereby removing them from liquid circulation on that origin chain. In response, an equivalent number of “wrapped” tokens (for example, wLEO on Ethereum, bLEO on Binance Smart Chain, or pLEO on Polygon) are algorithmically minted (or issued) on the target chain, subject to provable attestations via oracles or cross-chain relay/bridge protocols. If the user later desires reconversion, the wrapped tokens are irreversibly burned on the target chain, and the previously locked native tokens are released back to the user’s address on the source chain. This bi-directional mint-burn / lock-un...

Research unveils Rubik's cube-like Heusler materials with potential for thermoelectric applications



Researchers from the Hefei Institutes of Physical Science of the Chinese Academy of Sciences have designed Slater-Pauling (S-P) Heusler materials with a unique structure resembling a Rubik's cube. These materials exhibit semiconductor-like properties and have potential in thermoelectric applications. In traditional semiconductor Heusler alloys, the number of valence electrons follows a specific rule. However, these S-P Heusler compounds defy this rule while still displaying semiconductor behavior. In this study, the team focused on two Heusler systems: Ti-Fe-Sb and M-Co-Sn (M = Ti, Zr, Hf). Within these two systems, they predicted the thermodynamically stable TiFe1.5Sb and MCo1.33Sn S-P semiconductors. he researchers explained the unique properties of these compounds. In addition to the known half-Heusler (HH) and full-Heusler (FH) local geometries, these S-P structures contain defective-HH (DH) and defective-FH (DF) substructures. This is due to the partial occupation of Y atoms (Fe or Co) at the 4d Wyckoff site. Some off-stoichiometry Heusler compounds have been predicted to exhibit  characteristics. However, the bonding behavior in these S-P semiconductors and the relationship between their  and thermoelectric performance have remained unclear. This unique arrangement is key to the redistribution of electrons within the lattice, leading to the formation of a bandgap. It also reduces the phonon Debye temperature and enhances anharmonic vibrations, which in turn suppress the lattice thermal conductivityAs a result, these materials exhibit lower thermal conductivities compared to conventional HH and FH compounds. In particular, the calculated zT value of p-type ZrCo1.33Sn reaches 0.54 at 1,000 K, thanks to its high-power factor and low thermal conductivity.


        Heusler and half-Heusler compounds are ternary intermetallic compounds with highly tunable magnetic, topological, multiferroic, and electronic properties. They share a common crystal structure with more than 1000 members and compositions spanning most of the periodic table. Many of these compounds exhibit properties relevant to spintronics, such as magnetoresistance, variations of the Hall effectferro-antiferro-,and ferrimagnetismhalf- and semimetallicitysemiconductivity with spin filter ability, superconductivitytopological band structure and are actively studied as Thermoelectric materialsHeusler compounds are magnetic intermetallics with face-centered cubic crystal structure and a composition of XYZ (half-Heuslers) or X2YZ (full-Heuslers), where X and Y are transition metals and Z is in the p-blockTheir magnetism results from a double-exchange mechanism between neighboring magnetic ions. Manganese, which sits at the body centers of the cubic structure, was the magnetic ion in the first Heusler compound discovered.

        In condensed matter physics, the Slater–Pauling rule states that adding a element to a metal alloy will be reduce the alloy's saturation magnetization by an amount proportional to the number of valence electrons outside of the added element's d shell. Conversely, elements with a partially filled d shell will increase the magnetic moment by an amount proportional to number of missing electrons. Investigated by the physicists John C. Slater and Linus Pauling in the 1930s, the rule is a useful approximation for the magnetic properties of many transition metals.



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