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PISCES-2ET and Its Application Subsystems - Stanford Technology ...

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Material Properties for Heterostructures<br />

1 2 x ε 1 – 1<br />

------------- ( 1 – x) ε 2 – 1<br />

+ + -------------<br />

ε<br />

ε<br />

1 + 2 ε 2 + 2<br />

= ------------------------------------------------------------------------<br />

1 x ε 1 – 1<br />

– ------------- ( 1 – x) ε 2 – 1<br />

– -------------<br />

ε 1 + 2 ε 2 + 2<br />

(4.21)<br />

where ε 1<br />

is that of AlAs for both the materials, <strong>and</strong> ε 2<br />

is that of GaAs for AlGaAs <strong>and</strong> of InAs for<br />

AlInAs. The formulation applies to both high <strong>and</strong> low frequencies.<br />

The dielectric constants for Ge x Si 1-x are obtained by using the linear interpolation for those<br />

of Ge <strong>and</strong> Si. For the quaternary Ga x In 1-x As y P 1-y , the interpolation scheme in Eq. (4.18) is used based<br />

on the data for the constituent binaries.<br />

4.6 Mobilities<br />

Due to the lack of experimental data, the mobility dependences on composition, doping, lattice<br />

temperature, <strong>and</strong> field are not complete for most of the compound materials. Whenever data are not<br />

available constant mobility as listed in Section 3.1.1.1 is used. Readers are referred to [29] for data for<br />

many other materials, even though the collection of data is rather out-of-date (1971).<br />

4.7 Impact Ionization<br />

For relevant formulas <strong>and</strong> material parameters, see Section 3.3.1.1.<br />

<strong>PISCES</strong>-<strong>2ET</strong> – 2D Device Simulation for Si <strong>and</strong> Heterostructures 41

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