We construct an infinite family of one-dimensional equilibrium solutions for
purely magnetized quantum plasmas described by the quantum hydrodynamic model.
The equilibria depends on the solution of a third-order ordinary differential
equation, which is written in terms of two free functions. One of these free
functions is associated to the magnetic field configuration, while the other is
specified by an equation of state. The case of a Harris sheet type magnetic
field, together with an isothermal distribution, is treated in detail. In
contrast to the classical Harris sheet solution, the quantum case exhibits an
oscillatory pattern for the density.Comment: 2 figure
