Table 1 Overview of magnetic mechanisms and relevant symmetries

From: Ultrafast terahertz emission from emerging symmetry-broken materials

Mechanism

Common structure

B field sensitivity

Pump polarization sensitivity

Broken symmetries

Inverse spin-Hall effect (ISHE)

FM/NM

Yes, through FM layer magnetization

No

\({\mathscr{P}}\) (interface) \({\mathscr{T}}\) (FM) \(\to\) separated \({\mathscr{P}}{\mathscr{T}}\)

Inverse Rashba-Edelstein effect (IREE)

FM/NM1/NM2

Yes, through FM layer magnetization

No

\({\mathscr{P}}\) (NM1/NM2 interface) \({\mathscr{T}}\) (FM) \(\to\) separated \({\mathscr{P}}{\mathscr{T}}\)

Inverse spin–orbit torque (ISOT)

FM/NM

Yes, through the FM layer magnetization

Phase change depending on circular polarization state

\({\mathscr{P}}\) & \({\mathscr{T}}\) (interface) \(\to\) local \({\mathscr{P}}{\mathscr{T}}\)

Coherent magnons

AFM

Possible, depending on material

Yes, specifics depend on structure

\({\mathscr{T}}\)