ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems. Today MOS MOS. Capacitor. Idea

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Transcription:

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 9: September 26, 2011 MOS Model Today MOS Structure Basic Idea Semiconductor Physics Metals, insulators Silicon lattice Band Gaps Doping 1 2 MOS Metal Oxide Semiconductor 3 MOS Metal gate Oxide insulator separating gate from channel Ideally: no conduction from gate to channel Semiconductor between source and drain See why input capacitive? gate drain channel 4 src Capacitor gate drain channel Charge distribution and field? src Idea gate drain channel Semiconductor can behave as metal or insulator Voltage on gate creates an electrical field Field pulls (repels) charge from channel Causing semiconductor to switch conduction Hence Field-Effect Transistor src 5 6 1

Source/Drain Contacts Fabrication Contacts: Conductors metalic Connect to metal wires that connect Start with Silicon wafer Dope Grow Oxide (SiO 2 ) Deposit Metal Mask/Etch to define where features go 7 http://www.youtube.com/watch?v=35jwsqxku74 Cartoon fab seq.: t=2min 4min 8 Dimensions Channel Length (L) Channel Width (W) Oxide Thickness (T ox ) Semiconductor Physics Process named by minimum length 45nm L=45nm 9 10 Conduction Why metal conduct? Metal conducts Insulator does not conduct Semiconductor can act as either (periodic table) 11 http://chemistry.about.com/od/imagesclipartstructures/ig/science-pictures/periodic-table-of-the-elements.htm 12 2

Conduction Electrons move Must be able to remove electron from atom or molecule Atomic States Quantized Energy Levels Must have enough energy to change level (state) 13 14 Thermal Energy Silicon Atom Except at absolute 0 There is always free energy How many valence electrons? Causes electrons to hop around.when enough energy to change states Energy gap between states determines energy required 15 16 Silicon Silicon-Silicon Bonding 4 valence electrons Inner shells filled Can form covalent bonds with 4 other silicon atoms Only outer shells contribute to chemical interactions 17 18 3

Silicon Lattice Forms into crystal lattice Silicon Lattice Cartoon two-dimensional view http://www.webelements.com/silicon/crystal_structure.html 19 20 Outer Orbital? Energy? What happens to outer shell in Silicon lattice? What does this say about energy to move electron? 21 22 State View State View Conduction Band all states empty Energy Energy Valance Band all states filled Valance Band all states filled 23 24 4

Band Gap and Conduction Doping Insulator 8ev Metal OR Add impurities to Silicon Lattice Replace a Si atom at a lattice site with another Semiconductor 1.1ev 25 26 Doping Doping with P Add impurities to Silicon Lattice Replace a Si atom at a lattice site with another E.g. add a Group 15 element E.g. P (Phosphorus) How many valence electrons? 27 28 Doping with P End up with extra electrons Donor electrons Not tightly bound to atom Low energy to displace Easy for these electrons to move 29 Doped Band Gaps Addition of donor electrons makes more metallic Easier to conduct 0.045ev 1.1ev Semiconductor E D 30 5

Localized Electron Conduction Electron is localized Won t go far if no low energy states nearby Increase doping concentration Fraction of P s to Si s Decreases energy to conduct 31 32 Electron Conduction Capacitor Charge Remember capacitor charge + + 33 34 MOS Field? MOS Field Effect What does capacitor field do to the doped semiconductor channel? Vgs=0 No field = + + + Vgs>0 Conducts Vcap>0 35 Charge on capacitor Attract or repel charge in channel Change the donors in the channel Modulates conduction + + Positive Attracts carriers Enables conduction Negative? Repel carriers Disable conduction 36 6

Group 13 What happens if we replace Si atoms with group 13 atom instead? E.g. B (Boron) Valance band electrons? 37 Doping with B End up with electron vacancies -- Holes Acceptor electron sites Easy for electrons to shift into these sites Low energy to displace Easy for the electrons to move Movement of an electron best viewed as movement of hole 38 Hole Conduction Doped Band Gaps Addition of acceptor sites makes more metallic Easier to conduct Semiconductor 0.045ev 1.1ev E E A v 39 40 Field Effect? Effect of postivive field on Acceptordoped Silicon? Field Effect? Effect of negative field on Acceptordoped Silicon? Vgs=0 No field + Vcap>0 Vgs=0 No field + Vcap<0 Vgs>0 No conduction Vgs<0 Conduction 41 +++++ 42 7

Donor doping Excess electrons MOSFETs Negative or N-type material NFET Acceptor doping Excess holes Positive or P-type material PFET 43 Admin Intel Fabrication Talk Wednesday (28 th ) at 4pm (Raisler) HW3 Largely based on Wed. lecture Should be able to do SPICE parts now Will want to read text 3.3.2 44 MOSFET Semiconductor can act like metal or insulator Use field to modulate conduction state of semiconductor + + 45 8