Upload
others
View
2
Download
0
Embed Size (px)
Citation preview
MOSFET PRIMER
Sameer Sonkusalehttp://nanolab.ece.tufts.edu
2EE12: MOSFET PRIMERSameer Sonkusale
MOSFET
Metal Oxide Semiconductor Field Effect Transistor
Gate electrode is used to control the electric field in the channel region – which in turn controls the flow of charges between source and drain
3EE12: MOSFET PRIMERSameer Sonkusale
Quick Look At MOS Vs BJT Structure
In BJT, current conduction is due to both holes and electrons – hence the nameBipolar Transistor
In MOSFET, current conduction is due to one carrier – either holes or electrons
4EE12: MOSFET PRIMERSameer Sonkusale
Dissecting the MOSFET Structure
• Source-Drain are either p-type or n-type
• Gate is metal or polysilicon
5EE12: MOSFET PRIMERSameer Sonkusale
Views and Types of MOSFET
N-channel MOSFETNMOS
P-channel MOSFETPMOS
6EE12: MOSFET PRIMERSameer Sonkusale
NMOS as a switch
7EE12: MOSFET PRIMERSameer Sonkusale
PMOS as a switch
8EE12: MOSFET PRIMERSameer Sonkusale
N-channel MOSFET and P-channel MOSFET on same Substrate
9EE12: MOSFET PRIMERSameer Sonkusale
Array of FETs in an Integrated Circuit Environment
FOX – Field oxideN-well process example is shown above
Next problem : how do you connect these transistors ?- metal layers
10EE12: MOSFET PRIMERSameer Sonkusale
Metal layers and connections
11EE12: MOSFET PRIMERSameer Sonkusale
Side view showing metal interconnect layers in an IC environment
12EE12: MOSFET PRIMERSameer Sonkusale
Studying NMOS Regions of Operation
13EE12: MOSFET PRIMERSameer Sonkusale
Control the channel in NMOS
14EE12: MOSFET PRIMERSameer Sonkusale
Linear Region (Vgs > Vt and Vds small)
15EE12: MOSFET PRIMERSameer Sonkusale
MOSFET in linear region resembles a resistor (small Vds)
16EE12: MOSFET PRIMERSameer Sonkusale
As Vds is increased, channel tapers
17EE12: MOSFET PRIMERSameer Sonkusale
Pinch-Off
When pinch-off is reached, the amount of charge in the channel remains fixed* and therefore the current saturates.
18EE12: MOSFET PRIMERSameer Sonkusale
I-V characteristics of the MOSFET
19EE12: MOSFET PRIMERSameer Sonkusale
ID vs VGS
Square Law
20EE12: MOSFET PRIMERSameer Sonkusale
The iD–vDS characteristics for a device with k’n (W/L) = 1.0 mA/V2.
I-V characteristics of the MOSFET
21EE12: MOSFET PRIMERSameer Sonkusale
Figure 4.15 Increasing vDS beyond vDSsat causes the channel pinch-off point to move slightly away from the drain, thus reducing the effective channel length (by DL).
Actually Pinch-off point moves as Vds increases
22EE12: MOSFET PRIMERSameer Sonkusale
I-V characteristics showing finite output impedance
23EE12: MOSFET PRIMERSameer Sonkusale
Equations
Cut-off: VGS < VT ID = 0
24EE12: MOSFET PRIMERSameer Sonkusale
Key Observations
Control the ratio of Width and Length of the transistor to control transistor properties
It is a square law device. BJT was an exponential device
Terminologies for Triode and Saturation for MOSFETs are different than in BJT
25EE12: MOSFET PRIMERSameer Sonkusale
Symbol for NMOS
26EE12: MOSFET PRIMERSameer Sonkusale
Large Signal Model For MOSFET
27EE12: MOSFET PRIMERSameer Sonkusale
PMOS
OFF
ON
28EE12: MOSFET PRIMERSameer Sonkusale
Table 4.1
Large Signal Models Revisited