  In this paper the entanglement of multi-qubit fermionic pseudo Hermitian
coherent states (FPHCS) described by anticommutative Grassmann numbers is
studied. The pseudo-Hermitian versions of the well known maximally entangled
pure states such as Bell and GHZ, W and biseparable states are introduced
through integrating over the tensor products of FPHCSs with suitable choice of
Grassmannian weight functions. Meanwhile as an illustration, the method is
applied to tensor product of 2 and 3 qubit pseudo Hermitian systems. Then the
measures of concurrence and average entropy are applied to quantify the
entanglement of the pseudo two and three qubit states respectively.
