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Introduction Semiconductors are materials whose electrical properties lie between Conductors and Insulators. Ex : Silicon and Germanium.

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Presentation on theme: "Introduction Semiconductors are materials whose electrical properties lie between Conductors and Insulators. Ex : Silicon and Germanium."— Presentation transcript:

1 Introduction Semiconductors are materials whose electrical properties lie between Conductors and Insulators. Ex : Silicon and Germanium

2 Semiconductors: ability to change from conductor to insulator Can either allow current or prohibit current to flow

3 What are P-type and N-type ? Semiconductors are classified in to P-type and N-type semiconductor P-type: A P-type material is one in which holes are majority carriers i.e. they are positively charged materials (++++) N-type: A N-type material is one in which electrons are majority charge carriers i.e. they are negatively charged materials (-----)

4 Electronic devices created by bringing together a p-type and n-type region within the same semiconductor lattice. Used for rectifiers, LED etc

5 Diodes and Bias Diode: simple P-N junction. Forward Bias: allows current to flow from P to N. Reverse Bias: no current allowed to flow from N to P.

6 It is represented by the following symbol, where the arrow indicates the direction of positive current flow.

7 Characteristics of Diode Diode always conducts in one direction. Diodes always conduct current when “Forward Biased” ( Zero resistance) Diodes do not conduct when Reverse Biased (Infinite resistance)

8 Rectification Converting ac to dc is accomplished by the process of rectification. Two processes are used: –Half-wave rectification; –Full-wave rectification.

9 Half-wave Rectification Simplest process used to convert ac to dc. A diode is used to clip the input signal excursions of one polarity to zero.

10 Full Wave Rectifier

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12 Transistors Useful as a switch, but also as an amplifier Essential part of many technological advances

13 A Brief History Guglielmo Marconi invents radio in 1895 Problem: For long distance travel, signal must be amplified Lee De Forest improves on Fleming’s original vacuum tube to amplify signals Made use of third electrode Too bulky for most applications

14 The Transistor is Born Bell Labs (1947): Bardeen, Brattain, and Shockley Originally made of germanium Current transistors made of doped silicon

15 How Transistors Work Doping: adding small amounts of other elements to create additional protons or electrons P-Type: dopants lack a fourth valence electron (Boron, Aluminum) N-Type: dopants have an additional (5 th ) valence electron (Phosphorus, Arsenic) Importance: Current only flows from P to N

16 3 adjacent regions of doped Si ( each connected to a lead ): –Base. (thin layer,less doped). –Collector. –Emitter. 2 types of BJT: –npn. –pnp. Most common: npn (focus on it). Bipolar Junction Transistor (BJT) npn bipolar junction transistor pnp bipolar junction transistor Developed by Shockley (1949)

17 1 thin layer of p-type, sandwiched between 2 layers of n-type. N-type of emitter: more heavily doped than collector. With V C >V B >V E : –Base-Emitter junction forward biased, Base-Collector reverse biased. –Electrons diffuse from Emitter to Base (from n to p). –There’s a depletion layer on the Base-Collector junction  no flow of e - allowed. –BUT the Base is thin and Emitter region is n + (heavily doped)  electrons have enough momentum to cross the Base into the Collector. –The small base current I B controls a large current I C BJT npn Transistor

18 Basis of digital logic circuits Input to transistor gate can be analog or digital Building blocks for TTL – Transistor Transistor Logic BJT as Switch 2

19 BJT as Amplifier

20 (4.20) Logic Functions Using CMOS A B p p n n out input 0input 1 two input NAND - if both inputs 1, both p-channel are off, both n-channel are on, out is negative; otherwise at least one p-channel is on and one n- channel off, and out is positive

21 Types of Transistors


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