  The bipartite quantum and thermal entanglement is quantified within pure and
mixed states of a mixed spin-(1/2,1) Heisenberg dimer with the help of
negativity. It is shown that the negativity, which may serve as a measure of
the bipartite entanglement at zero as well as nonzero temperatures, strongly
depends on intrinsic parameters as for instance exchange and uniaxial
single-ion anisotropy in addition to extrinsic parameters such as temperature
and magnetic field. It turns out that a rising magnetic field unexpectedly
reinforces the bipartite entanglement due to the Zeeman splitting of energy
levels, which lifts a two-fold degeneracy of the quantum ferrimagnetic ground
state. The maximal bipartite entanglement is thus reached within a quantum
ferrimagnetic phase at sufficiently low but nonzero magnetic fields on
assumption that the gyromagnetic g-factors of the spin-1/2 and spin-1 magnetic
ions are equal and the uniaxial single-ion anisotropy is a half of the exchange
constant. It is suggested that the heterodinuclear complex
[Ni(dpt)(H$_2$O)Cu(pba)]$\cdot$2H$_2$O (pba=1,3-propylenebis(oxamato) and
dpt=bis-(3-aminopropyl)amine), which affords an experimental realization of the
mixed spin-(1/2,1) Heisenberg dimer, remains strongly entangled up to
relatively high temperatures (about 140~K) and magnetic fields (about 140~T)
being comparable with the relevant exchange constant.
