Anisotropic magnetoresistance (AMR) is a ubiquitous and versatile probe of ferro-, ferri-and antiferromagnetic order in contemporary spintronics research. Its origins are usually ascribed to spin-dependent electron scattering, whereas scattering-independent (intrinsic) contributions are neglected. Here, we measure AMR of the standard ferromagnets Co, Ni, Ni 81 Fe 19 and Ni 50 Fe 50 over the very wide frequency range from DC to 28 THz, which covers the regimes of both diffusive and ballistic transport. Analysis of the broadband response based on Boltzmann-Drude theory reveals that the AMR not only has the familiar scattering-dependent contribution, but also contains a sizeable scattering-independent component. In polycrystalline Co, this component is frequency-independent up to 28 THz and amounts to more than 2/3 of the AMR contrast of 1%, thereby making it interesting for applications in terahertz spintronics and terahertz photonics. Our results show that broadband terahertz electromagnetic pulses provide new insights into magneto-transport phenomena of magnetic materials on ultrafast time scales.
Reliable modulation of terahertz electromagnetic waveforms is important for many applications. Here, we rapidly modulate the direction of the electric field of linearly polarized terahertz electromagnetic pulses with 1–30 THz bandwidth by applying time-dependent magnetic fields to a spintronic terahertz emitter. Polarity modulation of the terahertz field with more than 99% contrast at a rate of 10 kHz is achieved using a harmonic magnetic field. By adding a static magnetic field, we modulate the direction of the terahertz field between angles of, for instance, −53° and 53° at kilohertz rates. We believe our approach makes spintronic terahertz emitters a promising source for low-noise modulation spectroscopy and polarization-sensitive techniques such as ellipsometry at 1–30 THz.
We introduce a wide-field magneto-optical microscope to probe magnetization dynamics with femtosecond temporal and sub-micrometer spatial resolution. We carefully calibrate the non-linear dependency between the magnetization of the sample and the detected light intensity by determining the absolute values of the magneto-optical polarization rotation. With that, an analytical transfer function is defined to directly map the recorded intensity to the corresponding magnetization, which results in significantly reduced acquisition times and relaxed computational requirements. The performance of the instrument is characterized by probing the magnetic all-optical switching dynamics of GdFe in a pump-probe experiment. The high spatial resolution of the microscope allows for accurately subdividing the laser-excited area into different fluence-regions in order to capture the strongly non-linear magnetization dynamics as a function of the optical pump intensity in a single measurement.
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