  It is shown that the {\em complex} $d_{xy}$ component is generated in d-wave
superconductor in the magnetic field. As one enters superconducting state at
finite field the normal to superconducting transition occurs into bulk
$d_{x^2-y^2}+i d_{xy}$ state . The driving force for the transition is the
linear coupling between magnetic field and non zero magnetization of the
$d_{x^2-y^2}+i d_{xy}$ condensate. The external magnetic field violates parity
and time reversal symmetries and the nodal quasiparticle states respond by
generating the $id_{xy}$ component of the order parameter, with the magnitude
estimated to be on the order of few Kelvin. Parity (P) and time reversal (T)
symmetries are violated in this state.
