Abstract
This chapter is intended to provide an overview of experimental information about magnetotransport in systems involving ferromagnetic (F) metals. The simplest such systems are the three F-elements, Fe, Co, and Ni, and their F-alloys. Magneto-transport in these metals and alloys has been studied for decades and much is reasonably well understood.1 Of most current interest is magnetotransport in three different systems: (1) Alternating thin layers (multilayers), or granular composites, of F-metals and non-magnetic (N) metals. These are called giant magnetoresistance (GMR) systems.2–6 (2) F/I/F sandwiches, or granular composites of F-metals plus insulators (I). Here, we have tunneling MR (TMR).7 (3) Materials that undergo phase transitions with decreasing temperature or increasing magnetic field H from a paramagnetic insulator (PI) to a ferromagnetic metal (FM) state. These are called colossal MR (CMR) materials.8,9 All of these phenomena, plus others to be described, are now collected under the rubric spin-polarized transport (SPT), because they involve differences in scattering of electrons with spins along or opposite to the local sample magnetization M.
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Bass, J. (2003). Magnetotransport (Experimental). In: Chtchelkanova, A., Wolf, S., Idzerda, Y. (eds) Magnetic Interactions and Spin Transport. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-0219-7_4
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