Observing differential spin currents by resonant inelastic X-ray scattering
Uchida, K. et al. Observation of the spin Seebeck effect. Nature 455, 778–781 (2008). Article PubMed ADS CAS …
Transient domain boundary drives ultrafast magnetisation reversal
Time-resolved magnetic soft-X-ray spectroscopy We investigate a typical nanometre-scale heterostructure consisting of an amorphous ferrimagnetic Gd25Co75 alloy with…
Unidirectional perfect absorption induced by chiral coupling in spin-momentum locked waveguide magnonics
Lodahl, P. et al. Chiral quantum optics. Nature 541, 473 (2017). ADS CAS PubMed Google Scholar Hentschel, M.,…
Origin and stability of generalized Wigner crystallinity in triangular moiré systems
Classical phase diagram and competing charge-ordered states To develop an intuition for the GWC problem, we first construct…
Néel spin-orbit torque in antiferromagnetic quantum spin and anomalous Hall insulators
Formalism We extend the Kane-Mele model by including a collinear AFM order which is exchange coupled to the…
Atomic-scale visualization of strain-tailored noncollinear spin textures in an antiferromagnetic ultrathin film
Growth of Mn atomic bilayer on Ag(111) Figure 1a represents the STM topographic overview of 1.0 ± 0.1 atomic layers of…
Fast optical control of a coherent hole spin in a microcavity
DiVincenzo, D. P. The physical implementation of quantum computation. Fortschr. Phys. 48, 771–783 (2000). Google Scholar Kimble, H.…
Pressure tuning of Kitaev spin liquid candidate Na3Co2SbO6
Kitaev, A. Anyons in an exactly solved model and beyond. Ann. Phys. 321, 2–111 (2006). MathSciNet Google Scholar …
Terahertz control of linear and nonlinear Magno-phononics
In our experiment, we measure the MPs by tracking the polarization state of an ultrashort, 800 nm probe…
High-temperature quantum coherence of spinons in a rare-earth spin chain
Connecting theory and experiment While spin-1/2 chains in magnetic crystals have been studied in the past31,32,33,34, to our…
Electric control of magnetic exchange in a molecular spin triangle
Cu3 crystallizes in the P31c non-centrosymmetric polar space group32. Each copper(II) ion is coordinated by four nitrogen and…
A sensitive MOKE and optical Hall effect technique at visible wavelengths: insights into the Gilbert damping
The experimental setup is based on the polar MOKE geometry illustrated in Fig. 1b. It consists of two orthogonally…