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Phys. Rev. 111, 430–432 (1958)

Ferroelectricity in Di-Glycine Nitrate (NH2CH2COOH)2·HNO3

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R. Pepinsky, K. Vedam, S. Hoshino, and Y. Okaya
Department of Physics, The Pennsylvania State University, University Park, Pennsylvania

Received 18 March 1958; published in the issue dated July 1958

(Glycine)2·HNO3 is ferroelectric below -67°C. The room-temperature phase is monoclinic, space group P21/a, with a=9.496 A, b=5.107 A, c=9.350 A, β=98.8°, ρobs=1.5810 g/cc, and Z=2. The nitrate groups must be disordered or rotating in this phase, since they are at centers of symmetry. The symmetry of the ferroelectric phase is Pa, as established from systematic absences and the fact that spontaneous polarization appears along the room-temperature [101] direction below -67°C. The dielectric constant ε[101], at 10 kc/sec and 5 v/cm, is 14 at room temperature, rises to a sharp peak of ∼600 at -67°C, and falls to ∼12 at -180°C. The transition appears to be of second order. At -77°C the spontaneous polarization is 0.60 μcoul/cm2, and the coercive field is 400 volts/cm. A specific heat anomaly similar to that in (glycine)3·H2SO4 and (glycine)3·H2BeF4 is observed, with ΔE=0.15 kcal/mole and ΔS=0.74 cal/mole deg.

© 1958 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRev.111.430
DOI:
10.1103/PhysRev.111.430
PACS: