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Floating-Gate Devices / Circuits
Prof. Paul Hasler Georgia Institute of Technology
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Channel Current Dependence on Gate Voltage
0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 10 -11 -10 -9 -8 -7 -6 Gate voltage (V) Drain current (A) k = Io = fA In linear scale, we have a quadratic dependence In log-scale, we have an exponential dependence return
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Basic Scaling Rules for MOSFETs
Early effect increases (Early voltage) decreases with length --- to keep the same margin from punchthrough as the previous generation, the doping must increase doping 1 / L2 (keeps constant field) To keep sufficiently high k (subthreshold slope),we must decrease the oxide thickness. This slope determines the ratio of on-current to off-current. (as supplies go down, we need a higher slope) oxide thickness 1 /L
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Scaling of MOS Parameters
Relationship between Substrate Doping and Oxide Thickness - square relationship keeps a constant coupling into the surface potential by keeping the gate and depletion capacitances the same Relationship between Oxide Thickness and Gate Length At this 4nm oxide thickness boundary: - the drawn gate length is 160nm - the substrate doping is 1018 cm-3 - a 1V barrier produces a one-sided depletion width of 40nm
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Effect of Velocity Saturation
VT A 76 nm MOSFET
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Maximum Operating Frequencies
fT = frequency where gain is unity at a given current
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DIBL in PFETs in 2mm Process
1 2 3 4 5 6 7 10 -1 -9 -8 -7 -6 Drain Current (A) Drain Voltage (V) Gate Voltage = 0V L = 1.25 m m L = 1.50 m m L = 1.75 m m V d g Gate voltage = 0
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DIBL in PFETs in 2mm Process
1 1.5 2 2.5 3 3.5 4 4.5 10 -11 -10 -9 -8 -7 -6 -5 V d g Drain current (A) I = I0 e e Vd / V0 kVg / UT V0 = 450mV; k = .422 Drain voltage
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Impact Ionization The mean rate of an impact-ionization
collision is highly energy dependant Impact Current is proportional to source current
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Overview of Floating-Gate Devices
Information Storage Floating-Gate Transistor Modifying Floating-Gate Charge UV photo-injection Electron tunneling Hot-electron injection
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Floating-Gate Charge Modification
Decrease Floating-Gate charge by hot-electron injection Increase Floating-Gate charge by electron-tunneling
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Electron Tunneling Increasing the applied voltage decreases the effective barrier width The range of tunneling currents span many orders of magnitude.
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How do we measure these currents?
V1 Measurement scheme used to characterize floating-gate devices Cf C2 V2 C3 Vout V3 Vref V4 Used in memory cells --Epots [Harrison, et. al.] C4
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Scaling Theory for Electron Tunneling
Tunneling Curve (Theory) for 5nm oxides 3 3.5 4 4.5 10 -18 -17 -16 -15 -14 -13 -12 Oxide Voltage Oxide Current (A) Itun = Itun0 e -Eo/Eox = Itun0 e - toxEo/Vox 108mV Itun = 0.2 e -(125V)/Vox
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Tunneling in normal FET operation
1 2 3 4 5 6 7 8 9 10 -70 -60 -50 -40 -30 -20 -10 Oxide thickness (nm) Oxide current at equilibrium 10 20 10 15 10 10 1 year Hold time on 1fF capacitor 10 5 1 hour 10 10 -5 10 -10 1 1.5 2 2.5 3 3.5 4 4.5 5 Oxide thickness (nm) To store a value (10 years), minimum oxide = 35nm Tunneling occurs normally in MOSFET operation
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Electron Transport in a Hot-Electron Injecting nFET
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Electron Transport in a Hot-Electron Injecting nFET
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Electron Transport in a Hot-Electron Injecting nFET
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Measurements and Modeling of Hot-Electron Injection
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pFET Hot-Electron Injection
The injected electrons are generated by hole impact ionizations. Vinj = 430mV Injection current is proportional to source current, and is an exponential function of Fdc.
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Circuit Model of Injection
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A 0.25mm Floating-Gate MOSFET
UT/k = 35mV, Ith = 10uA (minimum size) tox = 5nm, NA = 5 x 10 17 Injection pFET: efficiency at 3.3V Vinj = 90mV at 3.3V Iinj = (Is/ Iso) e -DVd/Vinj 0.6 Tunneling: Vx = 108 mV 0.32 -DVfg/Vx Iinj = 2.1 x (Is/ Iso) e
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Summary of Scaling FG Devices
Near future: Very good floating-gate devices, and “classical” theory holds reasonably well (down to L = 100nm, ~2006) Long term: We have many possibilities (at 50nm and below) - Storage by thicker oxide FETs - Basic FETs will tunnel / inject in normal operation
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