Van der Waals torque induced by external magnetic fields
arXiv:1010.4553 · doi:10.1063/1.3514152
Abstract
We present a method for inducing and controlling van der Waals torques between two parallel slabs using a constant magnetic field. The torque is calculated using the Barash theory of dispersive torques. In III-IV semiconductors such as , the effect of an external magnetic field is to induce an optical anisotropy, in an otherwise isotropic material, that will in turn induce a torque. The calculations of the torque are done in the Voigt configuration, with the magnetic field parallel to the surface of the slabs. As a case study we consider a slab made of calcite and a second slab made of . In the absence of magnetic field there is no torque. As the magnetic field increases, the optical anisotropy of increases and the torque becomes different from zero, increasing with the magnetic field. The resulting torque is of the same order of magnitude as that calculated using permanent anisotropic materials when the magnetic fields is close to 1 T.
to appear in Journal of Applied Physics
References in corpus (6)
- Casimir-Lifshitz Theory and Metamaterials
- On the torque on birefringent plates induced by quantum fluctuations
- Contribution of drifting carriers to the Casimir-Lifshitz and Casimir-Polder interactions with semiconductor materials
- Magnetoplasmons in layered graphene structures
- Results from electrostatic calibrations for measuring the Casimir force in the cylinder-plane geometry
- An alternative calculation of the Casimir forces between birefringent plates
Cited by in corpus (6)
- A Materials Perspective on Casimir and van der Waals Interactions
- Thermal Casimir and Casimir-Polder interactions in parallel 2D Dirac materials
- Mixing rules and the Casimir force between composite systems
- Maxwell Eigenmode approach to the Casimir-Lifshitz Torque
- Anomaly of the dielectric function of water under confinement and its role in Van der Waals interactions
- Effect of excess charge carriers and fluid medium on the magnitude and the sign of the Casimir-Lifshitz torque