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Kristin Ackerson, Virginia Tech EE Spring 2002 3 The diode is the simplest and most fundamental nonlinear circuit element. Just like resistor, it has.

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Presentation on theme: "Kristin Ackerson, Virginia Tech EE Spring 2002 3 The diode is the simplest and most fundamental nonlinear circuit element. Just like resistor, it has."— Presentation transcript:

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2 Kristin Ackerson, Virginia Tech EE Spring 2002

3 3 The diode is the simplest and most fundamental nonlinear circuit element. Just like resistor, it has two terminals. Unlike resistor, it has a nonlinear current-voltage characteristics. Its use in rectifiers is the most common application. Introduction

4 SJTU Zhou Lingling4 The most important region, which is called pn junction, is the boundary between n-type and p-type semiconductor. Physical Structure

5 SJTU Zhou Lingling5 (a) diode circuit symbol; (b) i– v characteristic; (c) equivalent circuit in the reverse direction; (d) equivalent circuit in the forward direction. Symbol and Characteristic for the Ideal Diode

6 What Are Diodes Made Out Of? Silicon (Si) and Germanium (Ge) are the two most common single elements that are used to make Diodes. A compound that is commonly used is Gallium Arsenide (GaAs), especially in the case of LEDs because of it’s large bandgap. Silicon and Germanium are both group 4 elements, meaning they have 4 valence electrons. Their structure allows them to grow in a shape called the diamond lattice. Gallium is a group 3 element while Arsenide is a group 5 element. When put together as a compound, GaAs creates a zincblend lattice structure. The concept of majority carrier and minority carrier is important in semiconductor devices. Majority carrier is the carrier type in a doped semiconductor with the highest concentration. Minority carrier is the carrier type with the lowest concentration.

7 7 Conducting in one direction and not in the other is the I-V characteristic of the diode. The arrowlike circuit symbol shows the direction of conducting current. Forward biasing voltage makes it turn on. Reverse biasing voltage makes it turn off. Characteristics

8 Forward Bias hole diffusion electron diffusion pn hole drift electron drift +- Applied potential lowers the potential barrier, I diffusion > I drift Mobile carriers drift through the dep. region into neutral regions become excess minority carriers and diffuse towards terminals

9 Forward Bias p n0 n p0 -W 1 W 2 0 p n ( W 2 ) n-regionp-region L p diffusion Typically avoided in Digital ICs x W n Metal contact to n-region -W p Metal contact to p-region p (x) n n (x) p minority carrier concentration

10 Reverse Bias hole diffusion electron diffusion pn hole drift electron drift -+ Applied potential increases the potential barrier Diffusion current is reduced Diode works in the reverse bias with a very small drift current

11 Reverse Bias x n p0 -W 1 W 2 0 n-region p-region p n0 diffusion The Dominant Operation Mode -W p Metal contact to p-region W n Metal contact to n-region n p0

12 12 The pn junction under open-circuit condition I-V characteristic of pn junction  Terminal characteristic of junction diode.  Physical operation of diode. Junction capacitance P-N junction

13 13 Usually the pn junction is asymmetric, there are p + n and pn +. The superscript “+” denotes the region is more heavily doped than the other region. pn Junction Under Open-Circuit Condition

14 14 Fig (a) shows the pn junction with no applied voltage (open- circuited terminals). Fig.(b) shows the potential distribution along an axis perpendicular to the junction. pn Junction Under Open-Circuit Condition

15 15 The procedure of forming pn the dynamic equilibrium of drift and diffusion movements for carriers in the silicon. In detail, there are 4 steps: a) Diffusion b) Space charge region c) Drift d) Equilibrium Procedure of Forming pn Junction

16 16 diffusion  Both the majority carriers diffuse across the boundary between p-type and n-type semiconductor.  The direction of diffusion current is from p side to n side. Procedure of Forming pn Junction

17 17 Space charge region  Majority carriers recombining with minority carriers results in the disappearance of majority carriers.  Bound charges, which will no longer be neutralized by majority carriers are uncovered.  There is a region close to the junction that is depleted of majority carriers and contains uncovered bound charges.  This region is called carrier-depletion region or space charge region. Procedure of Forming pn Junction

18 18 Drift  Electric field is established across the space charge region.  Direction of electronic field is from n side to p side.  It helps minority carriers drift through the junction. The direction of drift current is from n side to p side.  It acts as a barrier for majority carriers to diffusion. Procedure of Forming pn Junction

19 19 Equilibrium  Two opposite currents across the junction is equal in magnitude.  No net current flows across the pn junction.  Equilibrium conduction is maintained by the barrier voltage. Procedure of Forming pn Junction

20 Thank You


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