Abstract

The authors experimentally resolve the pulse- and temperature-dependent limits of single-shot alloptical magnetic switching in the compensated three dimensional ferrimagnet, revealing that the process is driven by exchange relaxation.

Highlights

  • Discovering how ultrashort laser pulses can manipulate magnetic materials on nonequilibrium timescales is a key goal of both ultrafast magnetism [1,2] and spintronics [3,4]

  • As a point of comparison, we studied a GdFeCo thin film structure Si3N4(60)/Gd25Fe65.6Co9.4(20)/Si3N4(5)/glass, which compensates at 320 K [32], and is known to exhibit singleshot All-optical switching (AOS) [6]

  • We found that switching can be achieved using far-infrared pulses, showing that the half metallicity of MRG is not an obstacle to the process, and suggesting that demagnetization of both sublattices evolves via exchange relaxation

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Summary

Introduction

Discovering how ultrashort laser pulses can manipulate magnetic materials on nonequilibrium timescales is a key goal of both ultrafast magnetism [1,2] and spintronics [3,4]. All-optical switching (AOS) of magnetization using a single ultrashort laser pulse in the absence of a magnetic field [5] was first identified in amorphous ferrimagnetic Gdx(FeCo)100−x thin films (hereafter referred to as GdFeCo) in 2012 [6]. Advances in the synthesis of fully compensated half metals [9] have recently resulted in the breakthrough discovery that ≈ 200-fs-long pulses can activate single-shot AOS in thin films of the Heusler alloy Mn2RuxGa [10] (hereafter referred to as MRG). In combination with its half metallicity [9], the potential to feature a perpendicular magnetic anisotropy field above 10 T and highly efficient intrinsic spinorbit torques [11] due to the absence of structural inversion symmetry, MRG’s ability to be switched all-optically renders it a compelling candidate for integration in future ultrafast spintronic technology [12,13,14]. While GdFeCo and MRG are both ferrimagnetic metals exhibiting compensation points where the constituent sublattices have equal but opposite magnetization [15], there are important material

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