Thiết kế VLSI - Bài 4 (HUST) Thầy Nguyễn Vũ Thắng

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goupee.vn goupee.com Design and Implementation of VLSI Systems Lecture04 MOSFET cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnMOS transistor theory goupee.com • Schedule for 4 lectures – Ideal (Shockley) Model – Non-ideal model – Inverter DC characteristics – SPICE cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vngate-oxide-body sandwich = capacitor goupee.com polysilicon gate Operating modes V < 0 silicon dioxide insulator g + • Accumulation - p-type body • Depletion • Inversion (a) 0 < V < V g t + depletion region - (b) • The charge accumulated is proportional to thecuu duong than cong . comV > V g t excess gate-channel + inversion region - depletion region voltage (Vgc-Vt) (c) fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnGate capacitance as a function of Vgsgoupee.com QuickTime™ and a decompressor are needed to see this picture. cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnThe MOS transistor has three regions of goupee.com operation • Cut off Vgs < Vt • Linear (resistor): Vgs > Vt & Vds < VSAT=Vgs-Vt Current prop to Vds NMOS transistor, 0.25um, Ld = 10um, W/L = 1.5, VDD = 2.5V, VT = 0.4V • Saturation: cuu duong than cong . com Vgs > Vt and Vds ≥ VSAT=Vgs-Vt Current is independent of Vds fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnHow to calculate the current value? goupee.com • MOS structure looks like parallel plate capacitor while operating in inversion – Gate – oxide – channel • Qchannel = CV • C = εoxWL/tox = CoxWL (where Cox=εox/tox) • V = Vgc – Vt = (Vgs – Vds/2) – Vt gate + V + g cuu duong than cong . comsource-Vgs Cg Vgd- drain V channel V s - + d n+ V n+ ds p-type body fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnCarrier velocity is a factor in determining thegoupee.com current • Charge is carried by electrons • Carrier velocity v proportional to lateral E-field between source and drain • v = μE μ called mobility • E = Vds/L • Time for carrier to cross channel: t = L / v cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnI=Q/t goupee.com • Now we know – How much charge Qchannel is in the channel – How much time t each carrier takes to cross Q I  channel ds t  W  V   C V V  ds 2 V ox L  gs t  ds   V V V V  gs cuu duong than cong . comt ds 2  ds   fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnIn linear mode (Vgs > Vt & Vds < Vgs-Vt) goupee.com Q I  channel ds t  W  V   C V V  ds 2 V ox L  gs t  ds Can be ignored for small Vds   V V V V  gs t ds 2  ds   cuu duong than cong . com ➢For a given Vgs, Ids is proportional (linear) to Vds fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnIn saturation mode (Vgs > Vt and Vds ≥ Vgsgoupee.com-Vt) Q I  channel ds t  W  V   C V V  ds 2 V ox L  gs t  ds   V V V V  gs t ds 2  ds   I   V V V V pinched off ds  gs t dsat 2  dsat     2  V Vcuu duong than cong . com 2 gs t ➢Now drain voltage no longer increases current fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnOperation modes summary goupee.com   0 V V cutoff  gs t I   Vcuu duong than cong . comV Vds V V V linear ds  gs t 2  ds ds dsat     2  V V V V saturation  2 gs t ds dsat fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vn goupee.com cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnTransistor capacitance goupee.com ▪ Gate capacitance: to body + to drain + to source ▪ Diffusion capacitance: source-body and drain-body capacitancescuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnGate capacitance as a function of Vgsgoupee.com QuickTime™ and a decompressor are needed to see this picture. cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vnSource/Drain diffusion capacitance goupee.com • Csb, Cdb • Undesirable, called parasitic capacitance Channel-stop implant NA1 • Capacitance depends on area and Side wall perimeter Source W N – Use small diffusion nodes D Bottom – Comparable to Cg – Varies with process xj Side wall Channel LS SubstrateN A cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vn goupee.com cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vn goupee.com cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vn goupee.com cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vn goupee.com cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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goupee.vn goupee.com cuu duong than cong . com fb.com/goupee.vn CuuDuongThanCong.com https://fb.com/tailieudientucntt

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