Ferroelectricityssä
Ferroelectricity is a property exhibited by certain dielectric materials that possess a spontaneous electric polarization which can be reversed by the application of an external electric field. This phenomenon is analogous to ferromagnetism, where materials exhibit spontaneous magnetization that can be switched by a magnetic field, hence the term "ferroelectric." The term was coined by Woldemar Voigt in 1921, though the effect was first observed in 1920 by Valasek in Rochelle salt (sodium potassium tartrate tetrahydrate).
Ferroelectric materials are typically crystalline and exhibit a phase transition between a paraelectric phase (above the
Key characteristics of ferroelectric materials include:
- Spontaneous polarization in the absence of an external electric field.
- The ability to switch polarization direction with an applied electric field.
- Hysteresis in the polarization-electric field loop, similar to the magnetization-magnetic field loop in ferromagnetic materials.
- Existence of a Curie temperature, above which the material loses its ferroelectric properties and becomes paraelectric.
Common ferroelectric materials include barium titanate (BaTiO₃), lead zirconate titanate (PZT), and lithium niobate (LiNbO₃). These