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Lecture handout including QS - Department of Materials Science ...

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BH34 Course B: <strong>Materials</strong> for Devices BH34<br />

Applications <strong>of</strong> Ferroelectrics<br />

Ferroelectrics are used in many commercial devices simply for their pyro- or piezo- electrical<br />

properties, or just as dielectrics: perovskite ferroelectrics have high κ values ⇒ BaTiO 3<br />

capacitors,<br />

e.g. for camera flashes (> 50% <strong>of</strong> the ceramic capacitor market).<br />

FE was discovered in 1921, and it’s always been obvious that the +P and –P states could be used to<br />

encode 0 and 1 for computing, but only relatively recently (~1995) has this become a reality.<br />

⇒ memory devices: FE-RAM - non-volatile, low voltage, small size & cost, fast, radiation hard.<br />

<strong>Materials</strong> requirements: high κ ; high P sat & P r ; (relatively) small E C ; high T C<br />

e.g. LiNbO 3<br />

, PbTiO 3<br />

, Pb(Zr x<br />

Ti 1-x<br />

)O 3<br />

(PZT), SrBi 2<br />

Ta 2<br />

O 9<br />

(SBT), fabricated as thin films<br />

(~ a few hundred nm) in order to minimise switching voltage.<br />

Wide-scale applications (cell phones, smart cards, video games) depend upon materials science:<br />

optimisation <strong>of</strong> composition, microstructure, interface quality with electrodes, control <strong>of</strong> nano-scale<br />

defects that pin domain walls.<br />

FE switching in a thin film memory device element:<br />

Thin Film, e.g. ~10 – 300 nm<br />

Start with a single-domain polarisation state [0]<br />

Reverse field ↓<br />

Nucleation <strong>of</strong> the opposite polarisation<br />

initiated at the surfaces<br />

Forward growth <strong>of</strong> needle-like domains<br />

parallel to the applied field<br />

Sideways growth <strong>of</strong> domains<br />

Reversed polarisation state [1]<br />

(switching takes ~ 50 ns)

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