The many-electron ground states of cylindrical parabolic quantum dots
in magnetic fields parallel to the cylindrical axis are investigated b
y means of an unrestricted Hartree-Fock method. The many-electron eige
nstates are assigned by two quantum numbers, L-z and S-z, the z-compon
ents of the total orbital angular momentum and the total spin, respect
ively. As the strength of the magnetic field increases, the spin state
of the ground state changes from the paramagnetic to the ferromagneti
c state according to Hund's rule. \L-z\ of the ground state increases
monotonically with magnetic held strength. In the extremely high-held
region of complete spin polarization, \L-z\ increases the electron num
ber N by N. From the total energy of the ground state, the chemical po
tential and the magnetic susceptibility of quantum dots are calculated
as functions of electron number up to 12. Magnetic field dependence o
f the chemical potential exhibits many cusps, caused by the transition
s of many-electron ground states. The chemical potential depends on th
e vertical extent of a quasi-two-dimensional dot only in weak and inte
rmediate fields where the spin polarization is incomplete, and it depe
nds only slightly on the spin Zeeman term for GaAs dots. The magnetic
susceptibility for an array of dots consists of two parts, paramagneti
c and diamagnetic, and shows oscillation with electron number at low t
emperatures.