2014
DOI: 10.1109/ted.2014.2361686
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Geometry Optimization of Planar Hall Devices Under Voltage Biasing

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Cited by 11 publications
(7 citation statements)
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“…Let us introduce the Lagrange multiplayers λ J and λ n corresponding to the constraints [Eq. (7)] so that the functional to be minimized reads now,…”
Section: Least-dissipation Principlementioning
confidence: 99%
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“…Let us introduce the Lagrange multiplayers λ J and λ n corresponding to the constraints [Eq. (7)] so that the functional to be minimized reads now,…”
Section: Least-dissipation Principlementioning
confidence: 99%
“…In contrast to usual non-equilibrium stationary sates, the presence of the static magnetic field leads to specific transverse boundary conditionsthe charge accumulation at the edges-that are not imposed directly by external constraints but by the system itself, according to the Le Chatelier-Braun principle. 2,3 This specificity of the boundary conditions for the Hall effect has been discussed within a large variety of theoretical models, [4][5][6][7][8][9][10][11][12] but the nature of the charge accumulation at the edges still remains rather mysterious. Indeed, the discovery of the extraordinary Hall effect at the turn of the millennium [13][14][15] and the recent developments about the Hall effect in ferromagnets 16,17 or about the spin-Hall effect 18,19 show that 140 years after his discovery, the classical Hall effect still deserves attention.…”
Section: Introductionmentioning
confidence: 99%
“…For planar HHDs with twofold symmetry, a high GV can approach the theoretical limit of 0.74 [21]. However, For VHDs with lower symmetry and additional degrees of freedom, the GV value is significantly reduced compared to that of the HHDs due to the value of the input resistance [22].…”
Section: Device Design and Tcad Simulationmentioning
confidence: 96%
“…However, a description that takes into account the non-equilibrium nature of the electric screening occurring in the SHE is still an open problem. One of the main difficulty is the same as for the classical Hall-effect [17][18][19][20][21][22][23][24][25][26]: it is due to the fact that the values of the charge accumulation at the edges of the Hall bar are not directly imposed by the external constraints. Instead, for the stationary state, the accumulation of electric charges and spins at the edges is generated by the system itself, in reaction to the action of the internal magnetic field (the spin-orbit effective magnetic field), together with to stationary current injected from the electric generator, and for a given geometry.…”
Section: Introductionmentioning
confidence: 99%