Ultrafast spin-lattice relaxation in ferromagnets including effective spin-orbit fields
arXiv:1709.04253 · doi:10.1103/PhysRevB.96.140408
Abstract
We investigate ultrafast demagnetization due to electron-phonon interaction in a model band-ferromagnet. We show that the microscopic mechanism behind the spin dynamics due to electron-phonon interaction is the interplay of scattering and the precession around momentum-dependent effective internal spin-orbit magnetic fields. The resulting magnetization dynamics can only be mimicked by spin-flip transitions if the spin precession around the internal fields is sufficiently fast (compared to the scattering time) so that it averages out the transverse spin components.
References in corpus (11)
- Universal Intrinsic Spin-Hall Effect
- Super-Diffusive Spin-Transport as a Mechanism of Ultrafast Demagnetization
- Semiconductor Spintronics
- Spin dynamics in semiconductors
- Ultrafast demagnetization of ferromagnetic transition metals: The role of the Coulomb interaction
- Ab initio investigation of Elliott-Yafet electron-phonon mechanism in laser-induced ultrafast demagnetization
- Electron-phonon-scattering dynamics in ferromagnetic metals and its influence on ultrafast demagnetization processes
- Many-body theory of ultrafast demagnetization and angular momentum transfer in ferromagnetic transition metals
- Role of Spin Flips versus Spin Transport in Non Thermal Electrons Excited by Ultrashort Optical Pulses in Transition Metals
- Reexamination of the Elliott-Yafet spin-relaxation mechanism
- Magnetization dynamics and damping due to electron-phonon scattering in a ferrimagnetic exchange model
Cited by in corpus (5)
- Tuning the laser-induced ultrafast demagnetization of transition metals
- Ultrafast electron dynamics in altermagnetic materials
- Off-resonant all-optical switching dynamics in a ferromagnetic model system
- Ultrafast electron-phonon scattering in antiferromagnetic Dirac semimetals
- Interplay of electron-magnon scattering and spin-orbit induced electronic spin-flip scattering in a two-band Stoner model