1 / 15

Lecture #21

Lecture #21. ANNOUNCEMENTS No coffee hour today  Quiz #3 on Friday (March 9) Material of HW #5 & #6 (Lectures 13-17) Closed book, no calculators; 3 pages of notes allowed OUTLINE pn Junctions: transient response: turn-on Summary of important pn-diode concepts pn diode applications

corinna
Télécharger la présentation

Lecture #21

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Lecture #21 ANNOUNCEMENTS • No coffee hour today • Quiz #3 on Friday (March 9) • Material of HW #5 & #6 (Lectures 13-17) • Closed book, no calculators; 3 pages of notes allowed OUTLINE • pn Junctions: • transient response: turn-on • Summary of important pn-diode concepts • pn diode applications Reading: Chapters 8 & 9 EE130 Lecture 21, Slide 1

  2. Turn-On Transient • Again, consider a p+n diode (Qp >> Qn): i(t) Dpn(x) t vA(t) x xn t For t > 0: EE130 Lecture 21, Slide 2

  3. By separation of variables and integration, we have • If we assume that the build-up of stored charge occurs quasi-statically so that then EE130 Lecture 21, Slide 3

  4. If tp is large, then the time required to turn on the diode is approximately DQ/IF EE130 Lecture 21, Slide 4

  5. Summary of Important Concepts • Under forward bias, minority carriers are injected into the quasi-neutral regions of the diode • Current flowing across junction is comprised of hole and electron components • In order for one of these components to be dominant, the junction must be asymmetrically doped EE130 Lecture 21, Slide 5

  6. Summary of Important Concepts (cont.) • The ideal diode equation stipulates the relationship between JN(-xp) and JP(xn) • If holes are forced to flow across a forward-biased junction, then electrons must also be injected across the junction EE130 Lecture 21, Slide 6

  7. Summary of Important Concepts (cont.) • Under reverse bias, minority carriers are collected into the quasi-neutral regions of the diode • Minority carriers within a diffusion length of the depletion region will diffuse into the depletion region and then be swept across the junction by the electric field. • Current flowing in a reverse-biased diode depends on the rate at which minority carriers are supplied in the quasi-neutral regions EE130 Lecture 21, Slide 7

  8. Varactor Diodes • Voltage-controlled capacitor • Used in oscillators and detectors (e.g. FM demodulation circuits in your radios) • Response changes by tailoring doping profile: EE130 Lecture 21, Slide 8

  9. Tunnel Diodes • Degenerately doped such that EFp < Ev and EFn > Ec • Can achieve negative differential resistance • useful in high-speed circuits and perhaps static memories EE130 Lecture 21, Slide 9

  10. Tunnel Diodes (cont.) EE130 Lecture 21, Slide 10

  11. Optoelectronic Diodes EE130 Lecture 21, Slide 11

  12. EE130 Lecture 21, Slide 12

  13. p-i-n Photodiodes • W  Wi-region, so most carriers are generated in the depletion region faster response time (~10 GHz operation) • Operate near avalanche to amplify signal EE130 Lecture 21, Slide 13

  14. Light Emitting Diodes (LEDs) • LEDs are typically made of compound semiconductors (direct bandgap) EE130 Lecture 21, Slide 14

  15. Organic LEDs • Some organic materials exhibit semiconducting properties • OLEDs are attractive for low-cost, high-quality flat-panel displays EE130 Lecture 21, Slide 15

More Related