3 research outputs found
Macroscopic Quantum Tunneling of a Domain Wall in a Ferromagnetic Metal
The macroscopic quantum tunneling of a planar domain wall in a ferromagnetic
metal is studied based on the Hubbard model. It is found that the ohmic
dissipation is present even at zero temperature due to the gapless Stoner
excitation, which is the crucial difference from the case of the insulating
magnet. The dissipative effect is calculated as a function of width of the wall
and is shown to be effective in a thin wall and in a weak ferromagnet. The
results are discussed in the light of recent experiments on ferromagnets with
strong anisotropy. PACS numbers:75.60.Ch, 03.65.Sq, 75.10.LpComment: 13page
Macroscopic Quantum Tunneling and Dissipation of Domain Wall in Ferromagnetic Metals
The depinning of a domain wall in ferromagentic metal via macroscopic quantum
tunneling is studied based on the Hubbard model. The dynamics of the
magnetization verctor is shown to be governed by an effective action of
Heisenberg model with a term non-local in time that describes the dissipation
due to the conduction electron. Due to the existence of the Fermi surface there
exists Ohmic dissipation even at zero temperature, which is crucially different
from the case of the insulator. Taking into account the effect of pinning and
the external magnetic field the action is rewritten in terms of a collective
coordinate, the position of the wall, . The tunneling rate for is
calculated by use of the instanton method. It is found that the reduction of
the tunneling rate due to the dissipation is very large for a thin domain wall
with thickness of a few times the lattice spacing, but is negligible for a
thick domain wall. Dissipation due to eddy current is shown to be negligible
for a wall of mesoscopic size.Comment: of pages 26, to appear in "Quantum Tunneling of Magnetization, ed. B.
Barbara and L. Gunther (Kluwer Academic Pub.), Figures available by FAX
(81-48-462-4649
Vortex Loop Phase Transitions in Liquid Helium, Cosmic Strings, and High-T_c Superconductors
The distribution of thermally excited vortex loops near a superfluid phase
transition is calculated from a renormalized theory. The number density of
loops with a given perimeter is found to change from exponential decay with
increasing perimeter to algebraic decay as T_c is approached, in agreement with
recent simulations of both cosmic strings and high-T_c superconductors.
Predictions of the value of the exponent of the algebraic decay at T_c and of
critical behavior in the vortex density are confirmed by the simulations,
giving strong support to the vortex-folding model proposed by Shenoy.Comment: Version to appear in Phys. Rev. Lett, with a number of corrections
and addition