“…The majority of the performed measurements is devoted to the longitudinal dielectric permittivity ε x (or its real part ε ′ x for low frequency alternating current measurements) mainly in the region of the high-temperature phase transition for DMAGaS and the corresponding phase transition in DMAAS. Such data are reported in the works [5,8,9,11] (DMAGaS) and [4,7,8] (DMAAS); only in the paper [7] the temperature behaviour of all permittivity components (ε ′ a , ε ′ b , ε ′ c ) for DMAAS crystal in the wide range of temperatures (from ≃ 90 K to ≃ 280 K) was measured. In some papers the dependence of spontaneous polarization on temperature in the ferroelectric phase was investigated and coercivity fields were measured [8,9] (the value of P s in the state close to saturation is about 1.4-1.9 C/m 2 for DMAAS and 0.9-2.0 C/m 2 for DMAGaS).…”