Field Effect Transistors CHAPTER 8 1 Introduction FET

Field Effect Transistors CHAPTER 8 1

Introduction FET’ stands for Field Effect Transistor p FET has 3 terminals p Those terminals are; gate, source, drain p Voltage controlled device p FET has 2 type of channels: n-channel, pchannel p 2

Introduction p Differences: -FET’s are voltage controlled devices whereas BJT’s are current controlled devices. -FET’s also have a higher input impedance, but BJT’s have higher gains. -FET’s are less sensitive to temperature variations and more easily integrated on IC’s. - FET’s are also generally more static sensitive than BJT’s. p Similarities: -Amplifiers -Switching devices -Impedance matching circuits 3

Classification scheme for field effect transistors. 4

Construction and characteristics of JFET p p p Major part of structure is n-type material. Top of the n-type channel is connected through an ohmic contact to a terminal referred to as the drain (D) The lower end-connected through an ohmic contact to a terminal referred as source (S) P-type materials are connected together and to the gate (G) terminal. JFET has two p-n junctions under no-bias conditions. 5

SYMBOL p p Fig. 30 -2 (a) is the schematic symbol for the n-channel JFET, and Fig. 30 -2 (b) shows the symbol for the p-channel JFET. The only difference is the direction of the arrow on the gate lead. Fig. 30 -2 (a) Copyright © The Mc. Graw-Hill Companies, Inc. Permission required for reproduction or display. Fig. 30 -2 (b) 6

TEO TYPES OF JFET P-Channel N-Channel Fig. 8. 1 7

How JFET Function p p The gate is connected to the source. Since the pn junction is reverse-biased, little current will flow in the gate connection. The potential gradient established will form a depletion layer, where almost all the electrons present in the n-type channel will be swept away. The most depleted portion is in the high field between the G and the D, and the leastdepleted area is between the G and the S. 8

How JFET Function p p p Because the flow of current along the channel from the (+ve) drain to the (-ve) source is really a flow of free electrons from S to D in the n -type Si, the magnitude of this current will fall as more Si becomes depleted of free electrons. There is a limit to the drain current (ID) which increased VDS can drive through the channel. This limiting current is known as IDSS (Drain-to-Source current with the gate shorted to the source). 9

Construction and characteristics of JFET p JFET operation can be compared to a water spigot: p The source of water pressure – accumulated electrons at the negative pole of the applied voltage from Drain to Source The drain of water – electron deficiency (or holes) at the positive pole of the applied voltage from Drain to Source. The control of flow of water – Gate voltage that controls the width of the n-channel, which in turn controls the flow of 10 electrons in the n-channel from source to drain. p p

Construction and characteristics of JFET N-Channel JFET Circuit Layout 11

JFET Operating Characteristics There are three basic operating conditions for a JFET: A. VGS = 0, VDS increasing to some positive value B. VGS < 0, VDS at some positive value C. Voltage-Controlled Resistor 12

VGS = 0, VDS increasing to some positive value Three things happen when VGS = 0 and VDS is increased from 0 to a more positive voltage: • the depletion region between p-gate n n and n-channel increases as electrons from n-channel combine with holes from p-gate. increasing the depletion region, decreases the size of the n-channel which increases the resistance of the n-channel. But even though the n-channel resistance is increasing, the current (ID) from Source to Drain through the n-channel is increasing. This is because VDS is increasing. 13

VGS = 0, VDS increasing to some positive value p p The flow of charge is relatively uninhibited and limited solely by the resistance of the n-channel between drain and source. The depletion region is wider near the top of both p-type materials. ID will establish the voltage level through the channel. The result: upper region of the p-type material will be reversed biased by about 1. 5 V with the lower region only reversed biased by 0. 5 V (greater applied reverse bias, the wider depletion region). 14

VGS = 0, VDS increasing to some positive value p IG=0 A p-n junction is reversebiased for the length of the channel results in a gate current of zero amperes. p As the VDS is increased from 0 to a few volts, the current will increase as determined by Ohm’s Law. p VDS increase and approaches a level referred to as Vp, the depletion region will widen, causing reduction in the channel width. (p large, n small). Reduced part of conduction causes the resistance to increase. If VDS is increased to a level where it appears that the 2 depletion regions would touch pinch-off will result. p p 15

VGS = 0, VDS increasing to some positive value p p p Vp = pinch off voltage. ID maintain the saturation level defined as IDSS Once the VDS > VP, the JFET has the characteristics of a current source. p As shown in figure, the current is fixed at ID = IDSS, the voltage VDS (for level >Vp) is determined by the applied load. p IDSS is derived from the fact that it is the drain-to-source current with short circuit connection from gate to source. p IDSS is the max drain current for a JFET and is defined by the conditions VGS=0 V and VDS > | Vp|. 16

VGS = 0, VDS increasing to some positive value At the pinch-off point: • any further increase in VGS does not produce any increase in ID. VGS at pinch -off is denoted as Vp. • ID is at saturation or maximum. It is referred to as IDSS. • The ohmic value of the channel is at maximum. 17

VGS < 0, VDS at some positive value p VGS is the controlling voltage of the JFET. p For n-channel devices, the controlling voltage VGS is made more and more negative from its VGS = 0 V level. p The effect of the applied negative VGS is to establish depletion regions similar to those obtained with VGS=0 V but a lower level of VDS to reach the saturation level at a lower level of VDS. 18

VGS < 0, VDS at some positive value p When VGS = -Vp will be sufficiently negative to establish saturation level that is essentially 0 m. A, the device has been ‘turn off’. p The level of the VGS that results in ID = 0 m. A is defined by VGS = Vp, with Vp being a negative voltage for n-channel devices and a positive voltage or p-channel JFETs. p In this region, JFET can actually be employed as a variable resistor whose resistance is controlled by the applied gate to source voltage. p A VGS becomes more and more negative; the slope of each curve becomes more and more horizontal. 19

VGS < 0, VDS at some positive value p The region to the right of the pinch-off locus of the figure is the region typically employed in linear amplifiers (amplifiers with min distortion of the applied signal) and is commonly referred to as the constantcurrent, saturation, or linear amplification region. 20

Characteristic curves for N-channel JFET 21

Voltage-Controlled Resistor p The region to the left of the pinch-off point is called the ohmic region. p The JFET can be used as a variable resistor, where VGS controls the drain-source resistance (rd). As VGS becomes more negative, the resistance (rd) increases. 22

p-Channel JFETS p-Channel JFET acts the same as the n-channel JFET, except the polarities and currents are reversed. 23

P-Channel JFET Characteristics As VGS increases more positively: p the depletion zone increases p ID decreases (ID < IDSS) p eventually ID = 0 A Also note that at high levels of VDS the JFET reaches a breakdown situation. ID increases uncontrollably if VDS> VDSmax. 24

Transfer Characteristics p The transfer characteristic of input-to-output is not as straight forward in a JFET as it was in a BJT. p In a BJT, indicated the relationship between IB (input) and IC (output). p In a JFET, the relationship of VGS (input) and ID (output) is a little more complicated: 25

Transfer Characteristics Transfer Curve From this graph it is easy to determine the value of ID for a given value of VGS. 26

Plotting the Transfer Curve Shockley’s Equation Methods. p Using IDSS and Vp (VGS(off)) values found in a specification sheet, the Transfer Curve can be plotted using these 3 steps: p Step 1: p Solving for VGS = 0 V: p Step 2: p Solving for VGS = Vp (VGS(off)): p Step 3: p Solving for VGS = 0 V to Vp: 27

Plotting the Transfer Curve Shorthand method VGS ID 0 IDSS 0. 3 VP IDSS/2 0. 5 IDSS/4 VP 0 m. A 28

Specification Sheet (JFETs) 29

Case Construction and Terminal Identification 30 This information is also available on the specification sheet.

MOSFETs have characteristics similar to JFETs and additional characteristics that make then very useful. There are 2 types: 1. 2. Depletion-Type MOSFET Enhancement-Type MOSFET 31

Depletion-Type MOSFET Construction The Drain (D) and Source (S) connect to the to n-doped regions. These Ndoped regions are connected via an n-channel. This n-channel is connected to the Gate (G) via a thin insulating layer of Si. O 2. The n-doped material lies 32 on a p-doped substrate that may have an additional terminal connection called SS.

Depletion-Type MOSFET Construction p VGS is set to 0 V by the direct connection from one terminal to the other. p VDS is applied across the drain-to-source terminals. p The result is an attraction for the positive potential at the drain by the free electron of the n-channel and a current similar to that established through the channel of the JFET. p In the figure, VGS has been set at a negative voltage ( -1 V) 33

Depletion-Type MOSFET Construction p p Negative potential at gate will tend to pressure electron towards the p-type substrate and attract holes from the p-type substrate. Depending on negative bias established by VGS, a level recombination between electron and hoes will occur. --- it will reduce the number of free electron in the n-channel available for conduction. The more negative bias, the higher the rate of recombination ID decrease, negative bias for VGS increase 34

Basic Operation A Depletion MOSFET can operate in two modes: Depletion or Enhancement mode. 35

Depletion-type MOSFET in Depletion Mode Depletion mode The characteristics are similar to the JFET. When VGS = 0 V, ID = IDSS When VGS < 0 V, ID < IDSS The formula used to plot the Transfer Curve still applies: 36

Depletion-type MOSFET in Enhancement Mode Enhancement mode VGS > 0 V, ID increases above IDSS The formula used to plot the Transfer Curve still applies: (note that VGS is now a positive polarity) 37

p-Channel Depletion-Type MOSFET The p-channel Depletion-type MOSFET is similar to the n-channel except that the voltage polarities and current directions are reversed. 38

Symbols 39

Enhancement-Type MOSFET Construction The Drain (D) and Source (S) connect to the to n-doped regions. These n-doped regions are connected via an n-channel. The Gate (G) connects to the p-doped substrate via a thin insulating layer of Si. O 2. There is no channel. The n-doped material lies on a p-doped substrate that may have an additional terminal connection called SS. 40

Enhancement-Type MOSFET Construction p p p VGS=0, VDS some value, the absence of an n-channel will result in a current of effectively 0 A VDS some positive voltage, VGS=0 V, and terminal SS is directly connected to the source, there are in fact 2 reversed-biased p-n junction between the n-doped regions and p substrate to oppose any significant flow between drain and source. VDS and VGS have been set at some positive voltage greater than 0 V, establishing the D and G at a positive potential with respect to the source The positive potential at the gate will pressure the holes in the p substrate along the edge of the Si. O 2 layer to leave the area and enter deeper regions of the p-substrate The result is a depletion region near the Si. O 2 insulating layer void of holes 41

Enhancement-Type MOSFET Construction p The electrons will in the p substrate will be attracted to the +G and accumulate in the region near the surface of the Si. O 2 layer p The Si. O 2 layer and its insulating qualities will prevent the negative carriers from being absorbed at the gate terminal VGS increase, the concentration of electrons near the Si. O 2 surface increase until eventually the induced n-type region can support a measurable flow between D and S The level of VGS that results in the significant increase in drain current is called the threshold voltage, VT. VGS increase beyond the VT level the density of the carriers in the induced channel will increase and ID also increase p p p 42

Enhancement-Type MOSFET Construction p p p If VGS constant and increase the level of VDS, ID will eventually reach a saturation level as occurred for the JFET Applying Kirchoff’s voltage law to the terminal voltage of the MOSFET VDG = VDS- VGS If VGS fixed at some value, 8 V, VDS increased from 2 – 5 V, the VDG will drop from -6 V to 3 V and the gate will become less and less positive with respect to the drain 43

Enhancement-Type MOSFET Construction The Enhancement-type MOSFET only operates in the enhancement mode. VGS is always positive As VGS increases, ID increases But if VGS is kept constant and VDS is increased, then ID saturates (IDSS) The saturation level, VDSsat is reached. 44

Enhancement-Type MOSFET Construction To determine ID given VGS: where VT = threshold voltage or voltage at which the MOSFET turns on. k = constant found in the specification sheet. k can also be determined by using values at a specific point and the formula: VDSsat can also be calculated: 45

p-Channel Enhancement-Type MOSFETs The p-channel Enhancement-type MOSFET is similar to the nchannel except that the voltage polarities and current directions are reversed. 46

Symbols 47

Specification Sheet 48

MOSFET Handling p MOSFETs are very static sensitive. Because of the very thin Si. O 2 layer between the external terminals and the layers of the device, any small electrical discharge can stablish an unwanted conduction. Protection: • Always transport in a static sensitive bag • Always wear a static strap when handling MOSFETS • Apply voltage limiting devices between the Gate and Source, such as back-to-back Zeners to limit any transient voltage. 49

VMOS – Vertical MOSFET increases the surface area of the device. Advantage: • This allows the device to handle higher currents by providing it more surface area to dissipate the heat. • VMOSs also have faster switching times. 50

CMOS – Complementary MOSFET p-channel and n-channel MOSFET on the same substrate. Advantage: Useful in logic circuit designs Higher input impedance Faster switching speeds Lower operating power levels 51

Summary Table 52