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Lecture 1b - Review. Kishore C Acharya. Building Semiconductor Devices. To build semiconductor devices # of carriers present in the semiconductor must be increased by adding impurities from Group III and Group V elements from periodic table Typical impurities Group III: Boron
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Lecture 1b - Review Kishore C Acharya
Building Semiconductor Devices • To build semiconductor devices # of carriers present in the semiconductor must be increased by adding impurities from Group III and Group V elements from periodic table • Typical impurities • Group III: Boron • Group V: Phosphorous
Increasing Carrier concentration by Doping • np = ni2 • n- elrctron concentration, p- hole concentration • ni = Intrinsic carrier concentration=1010/cc for silicon • For N type semi conductor • n = Nd donor concentration [1014 to 1018 /cc] – majority carrier • p = ni2 /Nd – minority carrier • For P type semi conductor • p = Na acceptor concentration [1014 to 1018 /cc] – majority carrier • n = ni2 /Na – minority carrier
Energy Levels of Silicon Ec = Edge of conduction band Ev = Edge of Valence band Efp = Fermi Level for P type Efn = Fermi Level for N type Eg = Energy gap kT = 0.025 eV at T = 300º K Ln(10) = 2.3
Fermi Level Calculation Example For Silicon ni = 1010 /cc For P type Semiconductor let Na = 1014 /cc Efp = Ec + Eg/2 + kT Ln(ni/Na) At t = 27º C, T = 300º K Efp = -4.05 - .55 + 0.025 Ln(1010 / 1014) = -4.83 eV
Fermi Level Calculation Example For Silicon ni = 1010 /cc For N type Semiconductor let Nd = 1016 /cc Efn = Ec + Eg/2 + kT Ln(Nd/ni) At t = 27º C, T = 300º K Efn = -4.05 - .55 + 0.025 Ln(1016 / 1010) = -4.25 eV
MOS Diode Structure Vint = (Efm – Efs)/q, Vint =0 once thermodynamic equilibrium is achieved Vint readjust the charge distribution so that Efm = Efs , where Efm and Efs are the Fermi Level of metal and semiconductor respectively
Metal Selection • Typical • Aluminum (Al), Ef = -4.1 eV • N+ poly silicon, Ef = -3.95 eV • Newer Material • For N type: Select Efn = -.411 0.2 eV • titanium, tantalum, zirconium, and hafnium • For P type: Select Efp = - 5.2 0.2 eV • platinum, palladium, nickel, cobalt, and ruthenium
Ideal MOS Diode( Efm = Efp) Vdiode = 0 Difficult to find Matching Metal so that Efm = Efp
Real MOS Diode Real MOS Diode Efm Efp Vint = Efm – Efs generates fields that readjusts charge distribution so that Vint = 0 After Equilibrium Efm = Efp Since Efm went down, it is similar to applying a positive Voltage to the metal side. Electrons accumulated at the surface and the band on the semiconductor side became curved
For Conduction Vs > 0 & Vgs Vt a negative threshold voltage about –1v This gate voltage is necessary to create a P channel under the oxide layer
For conduction Vd < 0 and Vgs Vt a positive threshold voltage about 1v This gate voltage is necessary to create a N channel under the oxide layer
Minimum Size MOS Transistor Channel Active Region Bulk or Substrate Is called the technology parameter = L/2. All sizes are integer multiple of
Condition for Conduction • Bulk must be reverse biased • Direct connection (P to Gnd, N to Vdd) • Connect bulk to one active which becomes source and proper source connection will reverse bias bulk • Channel must be created under the oxide layer • Apply a gate voltage of proper polarity exceeding a threshold • Circuit must be connected so that current flow is consistent with carrier flow
Quantitative criteria for conduction • For NMOSFET • Vds = Vd – Vs > 0 • Vgs = Vg – Vs Vtn (Vtn > 0, Typical 1V) • Vbs = Vb – Vs 0 • For PMOSFET • Vds = Vd – Vs < 0 • Vgs = Vg –Vs < Vtp (Vtp < 0, Typical –1 V) • Vbs = Vb – Vs 0
Source/Drain Source/Drain Gate Bulk (P) Bulk (N) Drsain/Source Drsain/Source Circuit Symbol Channel (N) Channel (P) Gate NMOSFET Bulk is P Channel is N Leakage current (P to N) Bulk to Channel PMOSFET Bulk is N Channel is P Leakage current (P to N) Channel to Bulk