Lab 8 - ECE 420L 

Authored by Silvestre Solano,

Email: Solanos3@unlv.nevada.edu

4-17-2015

 

This lab will use the CD4007 transistor array.

 

Experimentally generate, for the NMOS device, plots of: 

    1. ID v. VGS (0 < VGS < 3 V) with VDS = 3 V 
    2. ID v. VDS (0 < VDS < 5 V) for VGS varying from 1 to 5 V in 1 V steps, and 
    3. ID v. VGS (0 < VGS < 5 V) with VDS = 5 V for VSB varying from 0 to 3 V in 1 V steps. 
 
The following plots were generated with the use of Excel. The data used to make this plots was created in lab by using a 1k resistor and measuring the voltage across it. Then using Ohms law, I was able to calculate the current. This took a lot longer than it should have.
 
ID v. VGS (0 < VGS < 3 V) with VDS = 3 VID v. VDS (0 < VDS < 5 V) for VGS varying from 1 to 5 V in 1 V stepsID v. VGS (0 < VGS < 5 V) with VDS = 5 V for VSB varying from 0 to 3 V in 1 V steps
 
 
  
Assuming that the length of the NMOS is 5 um and its width is 500 um calculate the oxide thickness if Cox (= C'ox*W*L) = 5 pF.
 
Using the parameters Cox = 5 pF, W = 500 um, L = 5 um, e0 = 8.85*10^-18 F/um, and er = 3.97 , tox (oxide thickness) is calculated as follows.
 

 

 
The oxide thickness (tox)  is calculated to be about 17.6 mm.
 
 
 
From this measured data create a Level = 1 MOSFET model with (only) parameters: VTO, GAMMA, KP, and TOX.
 
From the ID vs. VGS (VSB = 0), VTO is about 1 V. TOX = 17.6 mm. KP is estimated by taking the data from the ID vs VDS (VGS varying) and using the square law equations to solve for KP. Of course, only the part of the graph that is clearly in saturation was used. After avaraging the current in a given curve and using the square law equation, then avaraging the result, KP is roughly 7 uA/V^2. GAMMA is determined by assuming that Vfp is equal to VB and solving for GAMMA according to the equation below. GAMMA was found to be about 2.15 V^0.5.
 

 
The final text file that models the NMOS is shown below.
 

 
 
 
Compare the experimentally measured data above (the 3 plots) to LTspice-generated data (again, 3 plots) and adjust your model accordingly to get better matching.
 
The plots for the NMOS simulations are shown below.
 
ID v. VGS (0 < VGS < 3 V) with VDS = 3 VID v. VDS (0 < VDS < 5 V) for VGS varying from 1 to 5 V in 1 V stepsID v. VGS (0 < VGS < 5 V) with VDS = 5 V for VSB varying from 0 to 3 V in 1 V steps

 
 
 
Repeat the above steps for the PMOS device where VDS, VGS, and VSB are replaced with VSD, VSG, and VBS respectively.
   
ID v. VSG (0 < VSG < 3 V) with VSD = 3 VID v. VSD (0 < VSD < 5 V) for VSG varying from 1 to 5 V in 1 V steps

 
TOX is calculated the same way assuming W and L are unchanged from the NMOS. TOX = 17.6 mm. From the above graphs, VTO is about 0.75 volts. KP is estimated the same way the KP for the NMOS was. The KP is estimated to be about 4 uA/V^2. Since I did not have enough time to do the varying VBS part for the PMOS, I will estimate the GAMMA paramater to be smaller than the NMOS. GAMMA is probably something like 1.23. The text file with the model parameters is shown below.
 

 
The following table shows the simulated PMOS graphs.
 
ID v. VSG (0 < VSG < 3 V) with VSD = 3 VID v. VSD (0 < VSD < 5 V) for VSG varying from 1 to 5 V in 1 V steps

 
 
 
Experimentally, similar to what is seen on the datasheet (AC test circuits seen on page 3 of the datasheet), measure the delay of an inverter using these devices (remember the loading of the scope probe is around 15 pF and there is other stray capacitance, say another 10 pF).
 
Using the CD4007 chip, the following scope picture was taken for the inverter. The delay is apparently 23.1 nS.
 

 
The simulation is shown  below.
 

 
As always, I will back up my work as shown below.
 

 
   

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