Physical Review · 1958 · 126 citations · 1 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsInorganic ChemistrySolid State PhysicsFerroelectric MaterialsPhase TransitionsPiezoelectric MaterialsFerroelectric PropertiesFerroelectric StructureFerroelectricityPolarizationSpontaneous PolarizationTriclinic System
(N${\mathrm{H}}_{4}$)HS${\mathrm{O}}_{4}$ is ferroelectric in the temperature range between -3\ifmmode^\circ\else\textdegree\fi{}C and -119\ifmmode^\circ\else\textdegree\fi{}C. The symmetry of the room-temperature phase is $\frac{P{2}_{1}}{c}$; the ferroelectric phase is also monoclinic, with space group $\mathrm{Pc}$; and the lowest phase, which is piezoelectric, has triclinic symmetry $P1$. All three phases are pseudo-orthorhombic. The coercive field is very low: about 150 v/cm at -13\ifmmode^\circ\else\textdegree\fi{}C. The spontaneous polarization ${P}_{s}$ is about 0.4 \ensuremath{\mu}coul/${\mathrm{cm}}^{2}$ at that temperature, and rises to a maximum of about 0.8 \ensuremath{\mu}coul/${\mathrm{cm}}^{2}$ just above -119\ifmmode^\circ\else\textdegree\fi{}C. ${P}_{s}$ falls to zero abruptly at the lower transition point. The higher transition is of second order, and the lower of first order.
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Ferroelectricity in Ammonium Sulfate
J. P. Remeika · Physical Review · 1956 · 127 citations