We demonstrate a Josephson diode effect mediated by Majorana zero modes at a junction between two Kitaev ladders. Each ladder consists of two spinless p-wave chains coupled by inter-leg hopping t⊥. A leg-to-leg phase φ within each ladder breaks time-reversal symmetry for φ ≠ 0, π (mod 2π), while a weak link between the ladders sets the across-junction phase θ. Interference between a phase-shifted intra-band channel, an unshifted inter-band channel, and the 4π Majorana channel near the topological transition yields a pronounced nonreciprocal current–phase relation. To our knowledge, this is the first explicit microscopic mechanism that links MZMs to the Josephson diode effect in a ladder–ladder junction.
Read the preprint on arXiv, and see also coverage by Quantum Zeitgeist.
The rare-earth free compound YCo₅ is a prototype uniaxial ferromagnet with large magnetic anisotropy, but it also shows very anisotropic magnetostriction: the in-plane value λₐ is nearly zero while the c-axis value λc is unusually large. We develop a phenomenological framework that links magnetostriction to elastic and magnetoelastic constants, and apply it to YCo₅ to obtain a simple relation λc = −B₃ /c₃₃. Tight-binding and first-principles calculations under controlled lattice distortions reveal that Co xz/yz bands near the Fermi level respond much more strongly to c-axis strain than to a-axis strain. This orbital-selective response produces a large magnetoelastic constant B₃ and implies an anomalously soft c-axis elastic constant, providing a microscopic explanation for the striking anisotropy of magnetostriction in YCo₅.
J. Inoue and H. Tsuchiura, Phys. Rev. Materials 8, 114403 (2024).
Figure for highlight: Fig. 3 (anisotropic change of Co-orbital DOS under a- and c-axis distortions).