We investigate a model with a massless fermion and a massive scalar field with the Yukawa interaction between these two fields. The model possess a discrete symmetry.The chiral condensate is calculated in one-loop approximation in (1 + 1)-dimensional spacetime. It was shown that the chiral condensate vanishes at two different values of the coupling constant. At the first of them there is a phase transition in which the discrete symmetry is restored. At the second zero of the chiral condensate it takes place a phase transition which distinguishes the positive µ 2 from the negative µ 2 , where µ 2 is an effective mass of the scalar field.