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