Field emission arrays using Si semiconductor emitters have been developed u
sing different technologies and configurations, including the field emissio
n microtriode (FEMT). Previously reported modeling results for FEMT structu
res considered metallic tips and, accordingly, used the Fowler-Nordheim (FN
) current density-electric field J(E) relationship. In this article, modifi
ed J(Si)(E) equations for Si semiconductor emitters are used. The FEMT mode
l takes;into account a volcano-shaped gate with an: emitter protruding thro
ugh the gate opening. The electric field distribution in the device is nume
rically computed solving the two-dimensional Laplace equation for the elect
rical potential using a lattice with a varying grid size. The field emissio
n current is obtained through integration of J(Si)(E) over the emitter surf
ace. No field enhancement and area factors are used. The FEMT field emissio
n: current is computed as function of the device parameters, and is compare
d to "standard":results derived using the FN J(E) relationship. Similar mod
eling trends are obtained for; the cases of FEMTs with metal and Si emitter
s. (C) 1999 American Vacuum Society. [S0734-211X(99)04202-X].