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Ferroelectric capacitor is a
capacitor In electrical engineering, a capacitor is a device that stores electrical energy by accumulating electric charges on two closely spaced surfaces that are insulated from each other. The capacitor was originally known as the condenser, a term st ...
based on a ferroelectric material. In contrast, traditional capacitors are based on dielectric materials. Ferroelectric devices are used in digital electronics as part of ferroelectric RAM, or in analog electronics as tunable capacitors (varactors). In memory applications, the stored value of a ferroelectric capacitor is read by applying an
electric field An electric field (sometimes called E-field) is a field (physics), physical field that surrounds electrically charged particles such as electrons. In classical electromagnetism, the electric field of a single charge (or group of charges) descri ...
. The amount of charge needed to flip the memory cell to the opposite state is measured and the previous state of the cell is revealed. This means that the read operation destroys the memory cell state, and has to be followed by a corresponding write operation, in order to write the bit back. This makes it similar to (now obsolete) ferrite core memory. The requirement of a write cycle for each read cycle, together with the high but not infinite write cycle limit is a potential problem for some special applications.


Theory

In a short-circuited ferroelectric capacitor with a metal-ferroelectric-metal (MFM) structure, a charge distribution of screening charges forms at the metal-ferroelectric interface so as to screen the electric displacement of the ferroelectric. Due to these screening charges, there is a voltage drop across the ferroelectric capacitor with screening in the electrode layer that can be obtained using the Thomas-Fermi approach as follows: V = E_f d + E_e\left(2\lambda\right) Here d is the film thickness, E_f = \frac and E_e=\fracE_f - \fracP_s are the electric fields in the film and electrode at the interface, P_s is the spontaneous polarization, a=\frac, and \epsilon_f & \epsilon_e are the dielectric constants of the film and the metal electrode. With perfect electrodes, \lambda=0 or for thick films, with d \gg a the equation reduces to: V = E_f d \Rightarrow E_f=\frac{d}


See also

* Ferroelectricity * Ferroelectric RAM


External links


FeRAM Tutorial


References

Capacitors Ferroelectric materials ja:FeRAM