We consider the 2D J1−J2 classical XY model on a square lattice. In the
frustrated phase corresponding to J2>J1/2, an Ising order parameter emerges
by an ``order due to disorder'' effect. This leads to a discrete symmetry plus
the O(2) global one. We formulate the problem in a Coulomb gas language and
show by a renormalization group analysis that only two phases are still
possible : a locked phase at low temperature and a disordered one at high
temperature. The transition is characterized by the loss of Ising and XY order
at the same point. This analysis suggests that the 2D J1−J2 XY model is in
the same universality class than XY-Ising models.Comment: 8 Pages, Latex, 1 ps figure, to be published in Europhysics Letter