Types of Amplifiers Common source, input pairs, are transconductance

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Presentation transcript:

Types of Amplifiers Common source, input pairs, are transconductance Most whole CMOS op amps are transconductance Common gate can be viewed as current amplifier Current mirrors are current amplifier Common drain or source follower is voltage amplifier Can cascade two or more basic one to get new types

Single transistor amplifiers, building blocks Rin = Rout = Rin = Rout = Rin = Rout =

Analysis of amplifiers DC analysis Find DC operating points, i.e., quiescent point, or Q point Finding the quiescent voltages VXXQ’s at various nodes Finding IXXQ’s through various branches Large signal static analysis Plot of output versus input (transfer curve) Large signal gain Output and input swing limits Small signal static and AC analysis DC gain A0, AC gain A(s) Input resistance/impedance, output resistance/impedance Small signal dynamic analysis Bandwidth, overshoot, settling Noise Power supply rejection Large signal dynamic analysis Slew rate Nonlinearity

Simple Inverting Amplifiers

Common source with diode load vOUT VDD |VTP| M1/2 sat vodP VGS-VTN M1 cutoff M2 sat vodN M1 tiode M2 sat vIN VDD VTN ID = ½bP(VDD-vOUT -|VTP|)2(1+lP(VDD-vOUT)) = ½bN(vIN-VTN)2(1+lNvOUT)

Large signal limits Absolute limits: None for v_in v_out: v_out at Vin=VDD to VDD-VTP To have all transistors in saturation: Vin range: Vout range:

Small Signal Characteristics Inverter with diode connection load Small Signal Characteristics

High gain inverters

Current source load or push-pull Refer to book for large signal analysis Must match quiescent currents in PMOS and NMOS transistors Wider output swing, especially push-pull Much higher gain (at DC), but much lower -3dB frequency (vs diode load) About the same GB Very power dependent

Small signal High gain! Especially at low power.

Dependence of Gain upon Bias Current ID ID + - Vg Vo+D + - Vg Vo

Use sufficient gm/Id Use sufficient L Use sufficient Vds-Ex

3 ways to increase A0: larger L, sufficient VDS, and small current density. But: Larger L reduces fT, slows down operation. VDS freedom is limited: in the 2nd stage VDS range is larger but must meet Vo swing requirement; 1st stage VDS range is quite small. Small current density also leads to slow operation.

Key to analysis by hand: Use level 1 or 3 model equations Use KCL/KVL

Transfer function of a system input u output y System zeros poles

For stability All closed loop poles must have negative real parts But open loop poles do not need to be stable Feedback changes the location of the poles Location of zeros cannot be changed by feedback Right half plane zeros do not cause instability by themselves But they have very negative impact on phase margin, making stabilization more difficult

Nodal analysis Identify nontrivial nodes Write a KCL at each node Solve for TF from input to output

Frequency Response of CMOS Inverters Only one non trivial node KCL: YtotVout(s)=Iinj Ytot =gds1+gds2+sCgd1 +sCBD1+sCL+sCBD2 +sCGD2 =go+sCL’ Iinj=-gm1vin+sCGD1vin

CMOS Inverters Let x=vin Still only one non trivial node KCL: YtotVout(s)=Iinj Same Ytot =gds1+gds2+sCgd1 +sCBD1+sCL+sCBD2 +sCGD2 =go+sCL’ But Iinj=-gm1vin+sCGD1vin –gm2vin+sCGD2vin

Input output transfer function When s=jw0, A(0)  When w∞, A(s)

Unity gain frequency of Loop gain Ab =-3dB frequency of closed loop =b*GB gain |A0 | =gm/go Acl=1/b 0 dB BW: |p1|= g0/CL’ gain BW product =|A0p1| =GB =gm/CL’ |z1| =gm/Cgd =GB*CL’/Cgd

Feedback changed pole location, but does not change zero location. Unity gain feedback A(s) Closed-loop zero: z1 Feedback changed pole location, but does not change zero location.

If a step input is given, the output response is By the final value theorem: By the initial value theorem:

Right half plane zero causes initial reverse transient, whose size depends on main pole/zero ratio. -1 Final settling determined by A0  need high gain Settling speed determined by A0p1=GB=UGF,  need high gain bandwidth product

Gain bandwidth product C’L = Ctotal = CGD1+ CGD2+ CBD1+ CBD2+ CL If fixed VEB used, W, ID, gm increase in proportion; GB initially increases but saturates near C’L=2CL.

Gain bandwidth product: ID bias

For small CL GB0 W1

At max GB sizing Use large current density Use small L Use NMOS for larger m Use smallest drain area Use larger VD Large Cox: thin oxide and high K Small gate drain overlap DL, small side wall capacitance density

Max GB and slew rate

NOISE IN MOS INVERTERS

To minimize: L2 >>L1 en1 small

For thermal noise