The analysis of the relation between modular P1CT-symmetry -- a
consequence of the Unruh effect -- and Pauli's spin-statistics relation is
continued. The result in the predecessor to this article is extended to the
Lorentz symmetric situation. A model \G_L of the universal covering
\widetilde{L_+^\uparrow}\cong SL(2,\complex) of the restricted Lorentz group
L+↑ is modelled as a reflection group at the classical level. Based
on this picture, a representation of \G_L is constructed from pairs of
modular P1CT-conjugations, and this representation can easily be verified to
satisfy the spin-statistics relation