1997
DOI: 10.1103/physrevlett.79.3744
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Quenching of Magnetoresistance by Hot Electrons in Magnetic Tunnel Junctions

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Cited by 529 publications
(418 citation statements)
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“…This feature is common in magnetic tunnel junctions 24 ͑MTJs͒ and ascribed in large part to magnon excitations at the electrode-barrier interfaces. 25 This mechanism is certainly also active here on the LSMO interface, but, since only one of the electrodes is magnetic, it cannot account for an approximately equal drop in positive and negative bias. A symmetric drop can only be due to magnon excitations inside the BMO barrier.…”
mentioning
confidence: 99%
“…This feature is common in magnetic tunnel junctions 24 ͑MTJs͒ and ascribed in large part to magnon excitations at the electrode-barrier interfaces. 25 This mechanism is certainly also active here on the LSMO interface, but, since only one of the electrodes is magnetic, it cannot account for an approximately equal drop in positive and negative bias. A symmetric drop can only be due to magnon excitations inside the BMO barrier.…”
mentioning
confidence: 99%
“…Yet tunnelling magnetoresistance ratios (TMRs) remain one order of magnitude below those predicted 17 . The impact of intrinsic effects such as magnon and phonon generation on TMR has been documented 18,19 . On the other hand, the impact of structural defects in MgO on tunnelling is only emerging in this otherwise widely studied, canonical spintronic system [20][21][22][23][24][25][26] .…”
mentioning
confidence: 99%
“…An important device merit is the TMR ratio and much theoretical and experimental efforts have been devoted to create MTJs with different ferromagnetic metals and insulating materials in order to generate a large ratio. While materials such as MgO and Al 2 O 3 are the most popular barrier materials in practical MTJs, [16][17][18][19][20] 2D materials graphene 21,22 and transition-metal dichalcogenides 23,24 have also been investigated in this context.…”
mentioning
confidence: 99%