I don't understand the first question about the many-boson state. The ##N##-boson states can be written as superpositions of totally symmetriced tensor products of ##N## single-particle states. One possibility is that all ##N## boson states occupy the same single-particle state, i.e., it's the ##N##-fold tensor product of this one single-particle state. For the BEC this single-particle state is the one-particle ground state.
As to the Pauli principle on fermions. There you have the totally antisymmetrized tensor products of single-particle states as a basis, and of course two electrons localized at far distances have to be antisymmetrized. Any two electrons in the universe are antisymmetrized two-particle states or superpositions of those (or statistical operators living in this fermionic many-body Hilbert space), but for far-distant experiments this doesn't play a big role as long as you do only local experiments, i.e., you do cannot observe possible correlations due to a possible entanglement of far-distant electrons except you do coincidence experiments on the two far distant places on the entangled electron pairs ("linked-cluster theorem").