2020
DOI: 10.1103/physrevb.102.214418
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Accelerating the laser-induced demagnetization of a ferromagnetic film by antiferromagnetic order in an adjacent layer

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Cited by 7 publications
(6 citation statements)
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“…For the NiMn composition of Ni 31 Mn 69 and the thickness of 20 ML, the antiferromagnetic ordering temperature of NiMn can be estimated to about 360 K [33,36,49]. Above its ordering temperature, the NiMn layer does not influence the Co layer magnetically [36], but the presence of the additional layer and of exchange-coupled magnetic moments at the interface to the Co layer may be influential via transient nonlocal effects such as the interchange or the reflection of electronic spin currents at the Co/NiMn interface [15]. However, from the comparison to the existing results on Co/Cu(001) from literature mentioned above, a significant role of the additional interface between Co and the magnetically disordered NiMn layer for the ultrafast dynamics of the Co layer can not be discerned.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…For the NiMn composition of Ni 31 Mn 69 and the thickness of 20 ML, the antiferromagnetic ordering temperature of NiMn can be estimated to about 360 K [33,36,49]. Above its ordering temperature, the NiMn layer does not influence the Co layer magnetically [36], but the presence of the additional layer and of exchange-coupled magnetic moments at the interface to the Co layer may be influential via transient nonlocal effects such as the interchange or the reflection of electronic spin currents at the Co/NiMn interface [15]. However, from the comparison to the existing results on Co/Cu(001) from literature mentioned above, a significant role of the additional interface between Co and the magnetically disordered NiMn layer for the ultrafast dynamics of the Co layer can not be discerned.…”
Section: Resultsmentioning
confidence: 99%
“…Such studies are essential for the understanding of ultrafast magnetization dynamics and have led to substantial insight into the underlying physical mechanisms and their theoretical description, such as, for example, the microscopic three-temperature model [6]. Combining ultrashort soft-x-ray probe pulses with near-infrared pump pulses to follow the magnetic response of an excited system [7][8][9][10][11][12][13][14][15][16] contributes an invaluable method to this field to meet the high demands of time-and element-resolved studies of ultrafast magnetism. It is particularly the elemental resolution of this approach that has helped to identify the role of the different timescales of demagnetization of 3d and 4f elements in ferrimagnetic alloys for the ultrafast laser-induced alloptical magnetic switching [10], prove the presence of nonlocal spin transport in ultrafast demagnetization [11], and has led to a number of investigations disentangling the complex evolution of the magnetic system, spin and electron scattering, as well as transport upon intense optical excitation [10,11,13,16].…”
Section: Introductionmentioning
confidence: 99%
“…[21] In the meantime, the exchange bias of the Co/IrMn interface is only affected by laser heating and the interacted AFM spin configuration itself. [27] In Fig. 3, we can note that the maximum amplitude of the exchange bias switching at the IrMn/CoGd interface decreases with the increased IrMn thickness.…”
Section: Laser-induced Ultrafast Antiferromagnet Rearrangementmentioning
confidence: 86%
“…Several reports have suggested that photoexcitation of the AFM/FM interface induces significant modulations in the exchange bias field on ultrashort timescales. [17][18][19] Detailed time-resolved studies of dynamics showed that the characteristic timescale of laserinduced exchange bias quenching in a polycrystalline Co/IrMn bilayer is 0.7 ± 0.5 ps, attributing the rapid decrease in exchange coupling to a spin disorder at the interface created by laser heating. [17] In our case, the demagnetization and switching dynamics after a 40 fs laser pulse illumination of the annealed IrMn(5)/Co 77 Gd 23 (4) sample have been studied as a function of time for various laser fluences (Figure 3a) and for different applied fields intensities (Figure 3b).…”
Section: Exchange Bias Switchingmentioning
confidence: 99%