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Introduction to MOSFET
Dr. Varun Kumar
Dr. Varun Kumar (IIIT Surat) 1 / 8
Outlines
1 Introduction to MOSFET
2 Enhancement type MOSFET
3 Threshold voltage
Dr. Varun Kumar (IIIT Surat) 2 / 8
Introduction to MOSFET
⇒ MSFET→ Metal-oxide-semiconductor-field-effect-transistor.
⇒ It is more commercially viable than the JFET.
⇒ Enhancement-type n-channel MOSFET.
⇒ On a lightly doped n-type substrate, two highly doped p+ regions are
diffused.
⇒ These two p+ sections are called as source and drain. Both terminals
are separated by a distance 5 − 10µm
Dr. Varun Kumar (IIIT Surat) 3 / 8
Continued–
⇒ A thin 0.1µm − 0.2µm layer of insulating silicon dioxide (SiO2) is
grown over the surface of the structure.
⇒ Holes are cut into the oxide layer, allowing contact with source and
drain.
⇒ Gate-metal area is overlaid on the oxide, covering the entire channel.
⇒ Contact metal over channel is called as gate-terminal.
⇒ Chip area is only about 5% of that required by BJT.
⇒ Metal area of the gate, in conjunction with insulating di-electric oxide
layer and semi-conductor channel form a parallel-plate capacitor.
⇒ SiO2 layer results in an extremely high input resistance (1010 − 1015Ω)
Dr. Varun Kumar (IIIT Surat) 4 / 8
Enhancement MOSFET
⇒ Ground the substrate and apply the negative voltage at the gate
terminal.
⇒ Electric field will be directed ⊥ through the oxide.
⇒ The field will end on “induces” positive charges on the semiconductor
site.
⇒ +Ve charges forms an inversion layer.
⇒ When negative gate voltage increases, the induced +Ve charge in the
semiconductor also increases.
⇒ Region beneath the oxide now has p-type carriers, the conductivity
increases, and the current flows from source to drain through the
induced channel.
⇒ Here the drain current is “enhanced” by -Ve gate voltage. Hence, this
device is called an enhancement type MOS.
Dr. Varun Kumar (IIIT Surat) 5 / 8
Continued–
(a) Drain characteristics
(b) Transfer curve (for VDS = 10 V )
Threshold Voltage
⇒ The current IDSS ∼ nA at VGS ≥ 0
⇒ VGS is made negative, the current |ID| increases slowly.
⇒
Dr. Varun Kumar (IIIT Surat) 6 / 8
Low VT
It allow
1 The use of a small power supply voltage
2 Compatible operation with bipolar device.
3 Smaller switching time due to smaller voltage swing during switching.
4 Higher packing densities.
Dr. Varun Kumar (IIIT Surat) 7 / 8
Methods for reducing the VT
1 High threshold MOSFET uses a silicon crystal with < 111 >
orientation. If orientation is < 100 > direction, it is found half that of
the < 111 > orientation.
2 Silicon nitride approach makes use of a layer of Si3N4 and SiO2.
3 Polycrystalline silicon doped with Boron is used as the gate electrode
instead of aluminum.
Dr. Varun Kumar (IIIT Surat) 8 / 8

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Introduction to MOSFET

  • 1. Introduction to MOSFET Dr. Varun Kumar Dr. Varun Kumar (IIIT Surat) 1 / 8
  • 2. Outlines 1 Introduction to MOSFET 2 Enhancement type MOSFET 3 Threshold voltage Dr. Varun Kumar (IIIT Surat) 2 / 8
  • 3. Introduction to MOSFET ⇒ MSFET→ Metal-oxide-semiconductor-field-effect-transistor. ⇒ It is more commercially viable than the JFET. ⇒ Enhancement-type n-channel MOSFET. ⇒ On a lightly doped n-type substrate, two highly doped p+ regions are diffused. ⇒ These two p+ sections are called as source and drain. Both terminals are separated by a distance 5 − 10µm Dr. Varun Kumar (IIIT Surat) 3 / 8
  • 4. Continued– ⇒ A thin 0.1µm − 0.2µm layer of insulating silicon dioxide (SiO2) is grown over the surface of the structure. ⇒ Holes are cut into the oxide layer, allowing contact with source and drain. ⇒ Gate-metal area is overlaid on the oxide, covering the entire channel. ⇒ Contact metal over channel is called as gate-terminal. ⇒ Chip area is only about 5% of that required by BJT. ⇒ Metal area of the gate, in conjunction with insulating di-electric oxide layer and semi-conductor channel form a parallel-plate capacitor. ⇒ SiO2 layer results in an extremely high input resistance (1010 − 1015Ω) Dr. Varun Kumar (IIIT Surat) 4 / 8
  • 5. Enhancement MOSFET ⇒ Ground the substrate and apply the negative voltage at the gate terminal. ⇒ Electric field will be directed ⊥ through the oxide. ⇒ The field will end on “induces” positive charges on the semiconductor site. ⇒ +Ve charges forms an inversion layer. ⇒ When negative gate voltage increases, the induced +Ve charge in the semiconductor also increases. ⇒ Region beneath the oxide now has p-type carriers, the conductivity increases, and the current flows from source to drain through the induced channel. ⇒ Here the drain current is “enhanced” by -Ve gate voltage. Hence, this device is called an enhancement type MOS. Dr. Varun Kumar (IIIT Surat) 5 / 8
  • 6. Continued– (a) Drain characteristics (b) Transfer curve (for VDS = 10 V ) Threshold Voltage ⇒ The current IDSS ∼ nA at VGS ≥ 0 ⇒ VGS is made negative, the current |ID| increases slowly. ⇒ Dr. Varun Kumar (IIIT Surat) 6 / 8
  • 7. Low VT It allow 1 The use of a small power supply voltage 2 Compatible operation with bipolar device. 3 Smaller switching time due to smaller voltage swing during switching. 4 Higher packing densities. Dr. Varun Kumar (IIIT Surat) 7 / 8
  • 8. Methods for reducing the VT 1 High threshold MOSFET uses a silicon crystal with < 111 > orientation. If orientation is < 100 > direction, it is found half that of the < 111 > orientation. 2 Silicon nitride approach makes use of a layer of Si3N4 and SiO2. 3 Polycrystalline silicon doped with Boron is used as the gate electrode instead of aluminum. Dr. Varun Kumar (IIIT Surat) 8 / 8