The anisotropy energy of a uniaxial crystal lattice is proportional to the square of this quantity's z component. The formation of Landau levels in a Fermi gas is responsible for the oscillations in this quantity as a function of applied field, a phenomenon known as the de Haas-van Alphen effect. For a type I superconductor, this quantity goes to zero discontinuously above the critical field, but in type II superconductors, it has a well defined maximum at the first critical value of applied field, after which it goes smoothly to zero. A hysteresis loop is formed when plotting this value against the applied field for a ferromagnetic material and the presence of this bulk quantity induces a bound current given by the curl of this vector quantity. Proportional in lin
The anisotropy energy of a uniaxial crystal lattice is proportional to the square of this quantity's z component. The formation of Landau levels in a Fermi gas is responsible for the oscillations in this quantity as a function of applied field, a phenomenon known as the de Haas-van Alphen effect. For a type I superconductor, this quantity goes to zero discontinuously above the critical field, but in type II superconductors, it has a well defined maximum at the first critical value of applied field, after which it goes smoothly to zero. A hysteresis loop is formed when plotting this value against the applied field for a ferromagnetic material and the presence of this bulk quantity induces a bound current given by the curl of this vector quantity. Proportional in linear materials to the applied field by the magnetic susceptibility, for 10 points, identify this bulk quantity, defined as the magnetic dipole moment per unit volume.
The anisotropy energy of a uniaxial crystal lattice is proportional to the square of this quantity's z component.
magnetization