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PN Junction Reverse Breakdown-Introduction to Microelectronic Circuits-Lecture 20 Slides-Electrical Engineering, Slides of Microelectronic Circuits

This course is taught in University of California, covers the fundamental circuit concepts and analysis techniques in the context of digital electronic circuits. Transient analysis of CMOS logic gates; basic integrated-circuit technology and layout are also included. PN Junction Reverse Breakdown, PN Junction, Reverse, Breakdown, Circuit Analysis, Nonlinear Element, Load Line, Analysis Method, Perfect, Rectifier Model, PN, Diode, Large Signal, Diode Model, Analyze, Circuits, Zener Diode, Light E

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2011/2012

Uploaded on 02/27/2012

elmut
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Download PN Junction Reverse Breakdown-Introduction to Microelectronic Circuits-Lecture 20 Slides-Electrical Engineering and more Slides Microelectronic Circuits in PDF only on Docsity! 1 Lecture 20, Slide 1EECS40, Fall 2003 Prof. King Lecture #20 OUTLINE • The pn junction (cont’d) – reverse breakdown • Load line analysis method • Diode models • Diode applications Reference Reading • Rabaey et al. (finish Chapter 3.2) • Howe & Sodini – Chapter 6.4.1 - 6.4.2 • Schwarz and Oldham (finish Chapter 13.2) Lecture 20, Slide 2EECS40, Fall 2003 Prof. King pn-Junction Reverse Breakdown • As the reverse bias voltage increases, the peak electric field in the depletion region increases. When the electric field exceeds a critical value (Ecrit ≅ 2x105 V/cm), the reverse current shows a dramatic increase: ID (A) VD (V) reverse (leakage) current forward current breakdown voltage VBD 2 Lecture 20, Slide 3EECS40, Fall 2003 Prof. King Circuit Analysis with a Nonlinear Element Since the pn junction is a nonlinear circuit element, its presence complicates circuit analysis. (Node and loop equations become transcendental.) VTh + − + V – RTh I Lecture 20, Slide 4EECS40, Fall 2003 Prof. King Load Line Analysis Method 1. Graph the I-V relationships for the non-linear element and for the rest of the circuit 2. The operating point of the circuit is found from the intersection of these two curves. VTh + − + V – RTh I I V The I-V characteristic of all of the circuit except the non-linear element is called the load line VTh VTh/RTh operating point 5 Lecture 20, Slide 9EECS40, Fall 2003 Prof. King Application Example #2 (using the Perfect Rectifier model) vs(t) + − + vR(t) – vs(t) t RC vR(t) t Lecture 20, Slide 10EECS40, Fall 2003 Prof. King integrated circuit A Zener diode is designed to operate in the breakdown mode. Zener Diode ID (A) VD (V) reverse (leakage) current forward current breakdown voltage R VBD = 15V VBD + vs(t) – t + vo(t) – Example: 6 Lecture 20, Slide 11EECS40, Fall 2003 Prof. King Light Emitting Diode (LED) • LEDs are made of compound semiconductor materials – Carriers diffuse across a forward-biased junction and recombine in the quasi-neutral regions optical emission Lecture 20, Slide 12EECS40, Fall 2003 Prof. King Diode Logic • Diodes can be used to perform logic functions: AND gate output voltage is high only if both A and B are high A B R Vcc C OR gate output voltage is high if either (or both) A and B are high A B R C Inputs A and B vary between 0 Volts (“low”) and Vcc (“high”) Between what voltage levels does C vary?
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