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FEATURES of FETs

 Field Effect Transistors ( FET ) are three terminal devices and
  its current controlled mechanism is based on an electric field
  established by the voltage applied to the controlled terminal.

 Just as there are npn and pnp BJTs, there are n-channel and
  p-channel FETs

 The current is conducted by only one type of carrier
  ( electrons or holes ) depending on the type of FET ( n-
  channel or p-channel ), which gives the FET another name,
  the unipolar transistors.

 The primary difference between BJTs and FETs is the fact that
  BJT is a current controlled device while FET is a voltage
  controlled device.
                                                S. Kal,   IIT-Kharagpur



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FEATURES of FETs

 The most important characteristics of FET is its high input
  impedance (meg Ohms) compared to that of BJT (K Ohms).

 FETs are more temperature stable than BJTs.

 FETs are usually smaller in construction than BJTs, making
  them more useful in IC chips

 Two types of FETs : (1) Junction Field Effect transistor
  ( JFET ) and (2) Metal Oxide Semiconductor Field Effect
  Transistors ( MOSFET )

 Three terminals of FETs are known as Source, Drain and
  Gate
                                             S. Kal,   IIT-Kharagpur


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JUNCTION FIELD EFFECT TRANSISTOR (JFET)
JFET is a three terminal device with one terminal capable of
controlling the current between the other two.
The major part of the structure
is the n-type material that forms
the channel between two p-type
layers which are connected to
form the Gate ( G ) terminal. The
two ends of the channel are
connected via Ohmic contact to
form Drain (D) and Source (S).
In the absence of any applied
potential, the two p-n junctions
form depletion region – void of
free carriers and unable to
support conduction through the
region.
                                              S. Kal,   IIT-Kharagpur
                                              4
JUNCTION FIELD EFFECT TRANSISTOR (JFET)




  A positive voltage VDS is applied across the channel and
  the gate has been connected directly to the source such
  that VGS = 0 V.
                                          S. Kal,   IIT-Kharagpur

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JUNCTION FIELD EFFECT TRANSISTOR (JFET)
 As the voltage VDS is increased from 0 to a few volts, the
  current will increase as determined by Ohm’s law ; as V DS
  approaches VP, depletion region widens causing reduction in
  channel width and channel resistance increases. The
  resistance approaches infinite Ohms in the horizontal region.
   The level of VDS at which two
   depletion region touches, is
   known as pinch-off voltage and
   is denoted by VP. ID maintains a
   saturation level defined as IDSS -
   the maximum value of drain
   current for a JFET.
   Once VDS > VP, the JFET has
   the characteristics of a current
   source.                                       S. Kal,   IIT-Kharagpur
                                                 6
N-Channel J-FET Characteristics
 The level of VGS that results in ID = 0 mA is defined by VGS = VP,
  with VP being a negative voltage for n-channel devices and +ve
  voltage for p-channel JFETs.

  When VGS< 0, depletion
 regions will be
 established similar to
 those obtained at VGS = 0
 but at a lower level of
 VDS.

  Pinch-off voltage
 continues to drop in a
 parabolic manner as VGS
 becomes more and more
 negative.                                           S. Kal,   IIT-Kharagpur


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TRANSFER CHARACTERISTICS OF A JFET

 The transfer curve [plot of output (or drain) current versus input
 controlling quantity (gate-source voltage) ] has extended use in
 JFET amplifiers.

 The input and output relationship of a JFET is not linear. The
 relationship between ID and VGS is defined by Schockley’s equation:




 The squared term of the equation will result in a nonlinear
  relationship between ID and VGS, producing a curve that grows
  exponentially with increasing values of VGS.
                                                      S. Kal,   IIT-Kharagpur
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TRANSFER CHARACTERISTICS OF A JFET
 The transfer curve can be obtained using Shockley’s
  equation or from the output characteristics as shown
  below.
 When VGS = 0, ID = IDSS, and VGS = VP, ID = 0




                                                  S. Kal,   IIT-Kharagpur

                                                  9
Metal-Oxide-Semiconductor FET (MOSFET)
Since late 1970s, MOSFET has been extremely popular.
 Compared to BJT, MOS transistor can be made quiet small and
  their manufacturing process is relatively simple.
 Analog, digital and combined analog-digital circuits (VLSI) are
  designed efficiently using MOS transistors.




                                                   S. Kal,   IIT-Kharagpur
                                                 10
Metal-Oxide-Semiconductor FET (MOSFET)
• Two classes of MOSFETs are available – Enhancement type
  and Depletion type

 Heavily doped n-type regions, indicated as n+ source and n+
  drain are created in the p-substrate. A thin (0.02 – 1 µm ) layer
  of SiO2, which is an insulator covers the area between source
  and drain. Metal is deposited on top of the oxide layer to form
  gate electrode. Metal contact is also made to source, drain and
  substrate, which is known as body. The gate electrode is
  electrically insulated from the device body which causes the
  current in the gate terminal to be extremely small ( ~ 10 -15 A )
 Current – voltage relation in the saturation region of NMOS is
  given by
              ID = ½ µ 0 Cox (W/L) (VGS – VT)2
                                                    S. Kal,   IIT-Kharagpur


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Enhancement MOSFET




             (a)                                   (b)
(a) Physical structure of the enhancement-type NMOS transistor
(b) iD-vDS characteristics of NMOSFET for VGS > Vt
                                            S. Kal,   IIT-Kharagpur


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Enhancement MOSFET




                   (a)                                   (b)
(a)   Enhancement NMOS as VDS is increased. The induced channel
      acquires a tapered shape and its resistance increases. V GS is
      kept constant at a value > Vt
(b)   ID – VDS (Drain) characteristics of a typical NMOS transistor
                                                         S. Kal, IIT-Kharagpur
                                                          13
N-Channel Depletion-Mode MOSFET




• Circuit symbol and physical structure of typical
  depletion-type MOSFET
                                      S. Kal,   IIT-Kharagpur

                                           14
Depletion Mode NMOS Transistor




 Drain (ID – VDS) and Transfer (ID – VGS) characteristics of a typical
depletion-mode MOSFET
                                                     S. Kal,   IIT-Kharagpur


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Complementary MOSFET




 Cross-section schematic diagram of a CMOS transistor (a
well also called a tub, is produced by an extra diffusion
step).
                                         S. Kal,   IIT-Kharagpur


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Complementary MOS (CMOS)

 Complementary devices makes possible many powerful
  circuit – design possibilities and is the most useful of all the
  IC MOS technologies

 It is a combination of PMOS and NMOS transistor

 NMOS is implemented directly in the p-type substrate, PMOS
  is fabricated in a specially created n region, called n well

 The two devices are isolated from each by a thick region of
  oxide that function as an insulator. This oxide is known as
  field oxide
                                                S. Kal,   IIT-Kharagpur




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