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

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Physical Models<br />

where E t<br />

is the energy level for the recombination centers <strong>and</strong> E i<br />

is the intrinsic Fermi Energy. Carrier<br />

lifetimes, τ n<br />

<strong>and</strong> τ p<br />

, can be either constant or dependent upon the total doping concentration (parameter<br />

consrh in model card). The formula for the doping dependent is as follows:<br />

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

(3.45)<br />

1 + N tot ⁄ N SRH<br />

where N tot<br />

is the total doping concentration, <strong>and</strong> the default values for parameters τ 0<br />

<strong>and</strong> N srh<br />

are the<br />

–7<br />

16<br />

same for both types of carriers in silicon <strong>and</strong> τ s <strong>and</strong> cm -3 0 = 1×10<br />

N srh = 5×10<br />

. If the interfacial<br />

recombination is to be included, it is through the change of carrier lifetime in the following way:<br />

τ eff<br />

(3.46)<br />

where A <strong>and</strong> d are partial area <strong>and</strong> interface length associated with the node in the element,<br />

respectively, <strong>and</strong> is the interface recombination velocity.<br />

s int<br />

3.3.4 Auger Recombination<br />

1<br />

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

τ 0<br />

ds int 1<br />

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

A τ<br />

This is a three-carrier recombination process, involving either two electrons <strong>and</strong> one hole or two holes<br />

<strong>and</strong> one electron. The dependence on n <strong>and</strong> p is as follows:<br />

2<br />

u Aug ( n,<br />

p) = ( c n n + c p p) ( np – n i )<br />

(3.47)<br />

–31<br />

–32<br />

where the default values for c <strong>and</strong> in silicon are <strong>and</strong> cm 6 s -1 n c p 2.8×10 9.9×10<br />

, respectively.<br />

<strong>PISCES</strong>-<strong>2ET</strong> – 2D Device Simulation for Si <strong>and</strong> Heterostructures 31

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