Abstract
At room temperature, GdMnO
3
is a paraelectric and paramagnetic with a distorted perovskite structure of orthorhombic symmetry (space group Pnma). On cooling, it undergoes a phase transition sequence to a magnetic incommensurate phase ( = δ (T)
*; T
c1 = 42 K) and a A-type antiferromagnetic phase (T
c2 = 27 K). At low temperatures (T ≤ 12 K), a magnetic field applied along the a-axis destabilizes the antiferromagnetic phase and induces a first order transition to a magnetic commensurate modulated phase (
= 1/4
*) that is also ferroelectric (
//
). This work analyses this field induced phase transition from the point of view of the symmetry and Landau theory.