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**UNIT 4 BASIC CIRCUIT DESIGN CONCEPTS**

(Pucknell p: )

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**Each of layers have their own characteristics like capacitance and resistances**

Concepts such as sheet resistance Rs and a standard unit capacitance □Cg Also delay associated with wiring, with inverters and with other circuitry may be evaluated in terms of a delay unit τ .

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sheet resistance Rs Consider a uniform slab of conduction material of resistivity ρ,of width W, thickness t, length between faces L Consider the resistance between two opposite faces RAB= ρL/A Ω Where area of the slab A=Wt. RAB= ρL/Wt Ω

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**Now, consider the case in witch L=W, that is a square of resistive material, then**

RAB= ρ/t =Rs Where Rs =ohm per square or sheet resistance The table of values for a 5µm technology is listed below.5µm technology means minimum line width is 5µm and λ= 2.5µm.

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**CAPACITANCE ESTIMATION**

Area capacitances of layers Standard unit of capacitance □Cg Some area capacitance calculations

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**Area capacitances of layers**

There are many layers and thus forms parallel plat capacitance effect Dielectric thickness , we can calculate area capacitance as follows: C=εo ε ins A farads D D= thickness of the dioxide in cm A = area of the plate in cm2 εo = permittivity of free space-8.854x10-14f/cm ε ins = relative permitivity of sio2=4.0

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**Typical values of area capacitance are set out in table for 5µm technology**

Value in pF*10-4/µm2(relative values in brackets) Gate to channel 4 (1.0) Diffusion 1 (.25) Poly to sub 0.4 (.1) M1 to sub 0.3 (0.075) M2 to sub 0.2 (0.05) M2 to M1 0.4 (0.1) M2 to poly 0.3 (0.075) Relative value = specified value / gate to channel value for that technology

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**Standard unit of capacitance □Cg**

The unit □Cg is defined as gate-to-channel capacitance of a MOS transistor having W=L=feature size □Cg was evaluated for any MOS, for example 5µm MOS circuits: Area/standard square = 5µm X 5µm = ? Capacitance value (from table) = 4 X 10-4 pF/µm2 Thus , standard value □Cg = 25µm2 X 4 X 10-4 pF/µm2 = ?

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**Some area capacitance calculations**

W=3λ area capacitance calculated by relative to that of a standard gate Consider the area in metal 1 Capacitance to substrate = relative area X relative C value =1.125 □Cg Consider the same area in polysilicon = ? Consider the same area in n-type diffusion = ?

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**Total capacitance CT=Cm+Cp+Cg =7.20 □Cg**

3 λ 4λ Metal 1λ 2 λ Diffusion 2 λ Polysilicon Total capacitance CT=Cm+Cp+Cg =7.20 □Cg

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**Total capacitance CT=Cm+Cp+Cg = Total capacitance CT=Cm+Cp+Cg = 7 □Cg**

Metal 1 |< λ > I <- 4 λ -> I < λ > I 3 λ 4λ 1λ 2 λ Diffusion 2 λ Polysilicon Total capacitance CT=Cm+Cp+Cg = Total capacitance CT=Cm+Cp+Cg = 7 □Cg

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DELAY τ The concept of sheet resistance and standard unit capacitance can be used to calculate the delay consider that a one feature size poly is charged by one feature size diffusion then the delay is Time constant τ =[1 Rs (n channel) X 1 □Cg ] For 5µm technology τ = 0.1 nsec

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**τ is not much differ from transit time τsd τsd = L2 / µn Vds**

Assume that Vds varies with Cg from oV to 63% of Vdd in period τ , then calculate τsd τsd =0.13 nsec

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**INVERTER DELAYS Consider 4:1 ratio nMOS inverter**

The delay associated with the inverter will depend on whether it is being turned off or on Consider pair of cascaded inverters then over delay will be Td= (1 + Z p.u / Z p.d) τ

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**Considering CMOS inverters , then equal size pull-up p-transistor and pull-down n-transistor**

Then Rs will asymmetry Gate capacitance is double because the input is connected to the common poly, putting both the gate capacitance in parallel..

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DELAY τ The concept of sheet resistance and standard unit capacitance can be used to calculate the delay consider that a one feature size poly is charged by one feature size diffusion then the delay is Time constant τ =[1 Rs (n channel) X 1 □Cg ] For 5µm technology τ = 0.1 nsec

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**τ is not much differ from transit time τsd τsd = L2 / µn Vds**

Assume that Vds varies with Cg from oV to 63% of Vdd in period τ , then calculate τsd τsd =0.13 nsec

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**INVERTER DELAYS Consider 4:1 ratio nMOS inverter**

The delay associated with the inverter will depend on whether it is being turned off or on Consider pair of cascaded inverters then over delay will be Td= (1 + Z p.u / Z p.d) τ

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**Considering CMOS inverters , then equal size pull-up p-transistor and pull-down n-transistor**

Then Rs will asymmetry Gate capacitance is double because the input is connected to the common poly, putting both the gate capacitance in parallel..

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**INVERTER DELAYS Estimation of CMOS inverter delay Rise time estimation Fall time estimation**

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**INVERTER DELAYS Consider 4:1 ratio nMOS inverter**

The delay associated with the inverter will depend on whether it is being turned off or on Consider pair of cascaded inverters then overall delay will be Td= (1 + Z p.u / Z p.d) τ

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**Considering CMOS inverters , then equal size pull-up p-transistor and pull-down n-transistor**

Then Rs will asymmetry Gate capacitance is double because the input is connected to the common poly, putting both the gate capacitance in parallel.

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**Estimation of CMOS inverter delay**

The inverter either charges or discharges the load capacitance CL. Raise-time and fall-time estimations obtained by following analysis

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Rise time estimation In this condition p-device stays in saturation for entire charging period of the load capacitance CL the p device is in saturation current given by Idsp=ßp(Vgs-|Vtp|)2 / (1)

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**The above current charges the capacitance and it has a constant value**

The above current charges the capacitance and it has a constant value. The output is the drop across the capacitance, given by Vout =Idsp x t /CL (2) Let t= τr ,Vout=Vdd, Vtp=0.2Vdd and Vgs=Vdd We have τr = 3CL /ßpVdd

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Fall time estimation Similar reasoning can be applied to the discharge of CL through the n- transistor Making similar assumptions we may write for fall-time : τf = 3CL /ßnVdd

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**Summary of CMOS fall time and rise factors**

Final expression we may deduce that: τr / τf = ßn / ßp Raise time is slower by factor of 2.5 when both ‘n’ and ‘p’ are in same size In order to achive symmetrical operation need to make Wp=2.5 Wn The factors which affect rise-time and fall-time as follows: τr and τf are proportional to 1/Vdd τr and τf are proportional to CL τr =2.5 τf for equal n and p transistor geometries

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**Driving large capacitance loads. Super buffers. BiCMOS driver**

Driving large capacitance loads Super buffers BiCMOS driver Cascaded inverters as drivers

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**The problem of driving large capacitive loads arises when signals must travel outside the chip.**

Usually it so happens that the capacitance outside the chip are higher. To reduce the delay these loads must be driven by low resistance.

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Super buffers Consider Vin=1 Inverter formed by T1 and T2 is turned on and thus the gate of T3 is pulled down to 0V but T4 is turned on and the output is pulled down Consider Vin=0,then the gate of T3 is allowed to rise quickly to Vdd,T4 is turned off. T3 is made to conduct with Vdd on its gate,i.e twice the average voltage that applied to gate Super buffers are better solution for large capacitance load delay problems

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BiCMOS driver VDD R Vout 1 Vin CL GND

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BiCMOS driver High current drive capabilities for small areas in silicon Working of bipolar transistor depends on two main timing components: Tin the time required to charge the base of the transistor which is large TL the time take to charge output load capacitor which is less

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Delay T CMOS BiCMOS Tin CL(crit) Load Capacitance CL Critical value of load capacitance CL(crit) below which the BiCMOS driver is slower than a comparable CMOS driver

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**Cascaded inverters as drivers**

N cascaded inverters, each one of which is larger than the preceding by a width factor f . Now both f and N can be complementary. If f for each stage is large the number of stages N reduces but delay per stage increases. Therefore it becomes essential to optimize. 4: f2 4: f 4:1 CL 1:1 1: f 1: f2 GND

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**Fix N and find the minimum value of f.**

For nMOS inverters Delay per stage = fτ for ↑Vin or = 4fτ for ↓Vin The delay for a nMOS pair is 5 fτ

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**For N=even Td=2.5 Neτ for nmos, Td=3.5 Neτ for cmos For N=odd**

Transition from 0 to 1 Transition from1 to 0 nMOS Td=[2.5(N-1)+1] eτ Td=[2.5(N-1)+4]eτ CMOS Td=[3.59N-1)+2]eτ Td=[3.5(N-1)+5]eτ

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**Propagation delay wiring capacitances Choice of layer**

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Propagation delay Cascaded pass transistors: delay introduced when the logic signals have to pass through a chain of pass transistors The transistors could pose a RC product delay Ex: the response at node V2 is given by C dV2/dt =(I1-I2)= [(V1-V2)(V2-V3)]/R

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**Lump all the R and C we have**

Rtotal=nrRs ….eq-1 Ctotal=ncﾛCg ….eq-2 Where r=relative resistance/section in terms of Rs c=relative capacitance/section in terms ofﾛCg Overall delay τd for n sections is given by τd = n2rc Long wires may be a problem with slowly rising signals

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wiring capacitances Fringing field: is due to parallel fine metal lines running across the chip for power connection. Total wire capacitance Cw=Carea+Cff Interlayer capacitance: is due to different layers cross silicon area Peripheral capacitance: is due to junction of two devices (regions) Total diffusion capacitance Ctotal = Carea + Cperi

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Choice of layer Vdd and Vss lines must be distributed on metal lines due to low Rs value Long lengths of poly must be avoided because they have large Rs The resistance effects of the transistors are much larger, hence wiring effects due to voltage divider effects b/w wiring and transistor resistances Diffusion areas must be carefully handled because they have larger capacitance to substrate.

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Lecture 11: MOS Transistor

Lecture 11: MOS Transistor

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