MOS Capacitors
The ICS Instructions contain the basic procedures for
making measurements. This screen is intended to point out things
unique to using the MOSC model file.
There are five types of capacitors in the mask set:
- metal over field oxide with guard rings (A),
- metal over gate oxide (B),
- metal over field oxide (C),
- metal over diffusion 1 (D) and
- metal over diffusion 2 (E).
Each type has been implemented with 3 different geometries:
- The square capacitor is 300 x 300 microns
- The round capacitor radius equals 150 microns
- The finger capacitor has a center region of 100 x 100 microns and twelve 20 x 100 microns fingers.
Device Selection
Make the measurements on the round "B" capacitors. You can determine the
doping level of the silicon from the capacitance measurements. You
will also be able to determine the oxide thickness (Gate Oxide in
the case of the "B" capacitors.)
Probe Assignments
- SMU1/probe1/CM(H)---->Round "B Capacitor" pad
- SMU2/probe2---->Substrate (small square under the "B")
Theory
These are metal oxide semiconductor capacitors (MOSC), and the ece340
textbook has a description of what the capacitance vs. voltage curves
should look like, as well as some of the information that can be
determined from them.
Here are some brief highlights:
The capacitance of the oxide is given by:
Cox = εA/d
where:
- ε = dielectric constant of insulator = ε0εr
- A = area of the device
- d = distance between the plates (dielectric thickness)
Under a particular bias polarity, a depletion layer will form in
the silicon below the oxide, adding another capacitor in series with
the oxide capacitor. The differential capacitance, Cd, of the
semiconductor-space charge region is
Cd = (dielectric constant of silicon)*(Area)/(Thickness of depletion region)
The total capacitance is
Ctot = (Cox * Cd)/(Cox+Cd)
Here is a typical C-V curve for a MOS capacitor on a grounded n-type
substrate with v_aluminum applied to an aluminum contact on top of
the oxide. The flat regions corresponding to the oxide capacitance
and the total capacitance at maximum depletion width are evident.
It is possible to model the capacitors by separating the capacitance
into center and edge effects. The equations are similar to those
used for modeling the p-n junction capacitance.
The total capacitance per area is
Ctotal = P * Cedge + A * Carea,
where P equals the perimeter and A equals the area. Note that the
units of Cedge and Carea are pF/μm and
pF/μm2, respectively. By using two of the capacitors,
it is possible to solve for P and A.
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