Our system \(\mathcal {S}\) consists of two subsystems \(S_{1}\) and \(S_{2}\) being coupled locally to their own reservoirs \(R_{A}\) and \(R_{B}\), respectively. The two subsystems are bridged by the third reservoir \(R_{C}\), with which they…
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Reply to: Re-examining magnetic tuning of Casimir forces
Moazzami Gudarzi, M. & Aboutalebi, S. H. Re-examing magnetic tuning of Casimir forces. Nat. Phys. https://doi.org/10.1038/s41567-025-02845-5 (2025).
Klimchitskaya, G. L., Mostepanenko, V. M., Nepomnyashchaya, E. K. & Velichko, E. N. Impact of…
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Orbital Hall conductivity in a Graphene Haldane and Haldane Haldane bilayers
Orbital ferromagnetism in graphene
We break the I and TR symmetries in single-layer graphene by introducing the mass term (M) and next nearest neighbor hopping term (\(t_2\)) (as discussed in Sec. Tight-binding Hamiltonain). This results in…
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Association of LILRB3 variants with kidney transplant failure in African Americans
African American kidney transplant recipients exhibit a higher risk of graft failure than other racial and ethnic groups even after accounting for HLA mismatches and socioeconomic status, which suggests a role for other risk factors. Now,…
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Altermagnetic ground state in distorted Kagome metal CsCr3Sb5
Liu, Y. et al. Superconductivity under pressure in a chromium-based kagome metal. Nature 632, 1032–1037 (2024).
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Yin, J.-X., Lian, B. & Hasan, M. Z….
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Topological properties of magnet-superconductor hybrid systems due to atomic-scale non-coplanar spin textures
Ideal and distorted triple-Q state
The 3Q state—predicted more than 20 years ago29,30—is a non-coplanar spin structure with four spins in the magnetic unit cell pointing into the directions of a tetrahedron. This intriguing three-dimensional…
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Signal size and resolution of scanning thermal microscopy in air and vacuum
Pollock, H. M. & Hammiche, A. Micro-thermal analysis: Techniques and applications. J. Phys. D Appl. Phys. 34, R23. https://doi.org/10.1088/0022-3727/34/9/201 (2001).
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