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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Heikkilä, Tero
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Topics
Publications (7/7 displayed)
- 2019Electron Induced Massive Dynamics of Magnetic Domain Walls
- 2019Dynamics of Strongly Driven Diffusive Josephson Junctions
- 2019Non-linear spin torque, pumping and cooling in superconductor/ferromagnet systems
- 2018Competition of electron-phonon mediated superconductivity and Stoner magnetism on a flat bandcitations
- 2017Spin Pumping and Torque Statistics in the Quantum Noise Limitcitations
- 2016Flat-band superconductivity in strained Dirac materialscitations
- 2006Opportunities for mesoscopics in thermometry and refrigeration: Physics and applicationscitations
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document
Electron Induced Massive Dynamics of Magnetic Domain Walls
Abstract
We study the dynamics of domain walls (DWs) in a metallic, ferromagnetic nanowire. We develop a Keldysh collective coordinate technique to describe the effect of conduction electrons on rigid magnetic structures. The effective Lagrangian and Langevin equations of motion for a DW are derived. The DW dynamics is described by two collective degrees of freedom: position and tilt-angle. The coupled Langevin equations therefore involve two correlated noise sources, leading to a generalized fluctuation-dissipation theorem (FDT). The DW response kernel due to electrons contains two parts: one related to dissipation via FDT, and another `inertial' part. We prove that the latter term leads to a mass for both degrees of freedom, even though the intrinsic bare mass is zero. The electron-induced mass is present even in a clean system without pinning or specifically engineered potentials. The resulting equations of motion contain rich dynamical solutions and point toward a new way to control domain wall motion in metals via the electronic system properties. We discuss two observable co nsequences of the mass, hysteresis in the DW dynamics and resonant response to ac current.