professor jri lee - 國立臺灣大學cc.ee.ntu.edu.tw/~jrilee/course/commic08/commic_03.pdflimiting...

21
Limiting Amplifiers Professor Jri Lee 台大電子所 李致毅教授 Electrical Engineering Department National Taiwan University

Upload: others

Post on 03-Feb-2021

1 views

Category:

Documents


0 download

TRANSCRIPT

  • Limiting Amplifiers

    Professor Jri Lee台大電子所 李致毅教授

    Electrical Engineering DepartmentNational Taiwan University

  • Outline

    IntroductionDesign ChallengesLoss of Signal DetectionBroadband TechniquesCase Study

  • General Considerations

    Requirement

    Broad Bandwidth ( 0.7 Data Rate)Low Noise (300 ~ 400 µVrms)Small Offset VoltageWell-Behaved Response to Large Signals

    High Gain (40~60dB)≥ ×

  • Challenges of Noise

    Example: OC-192 Receiver (Data Rate 10Gb/s)≈

    For TIA output noise = 1 mVrms and LA contributes 10% of noise ⇒ LA input noise = 330 µVrmsFor a bandwidth of 10 GHz ⇒ Vn,LA < 3 nV/ Hz

  • Offset Due to Mismatches

    Random asymmetries (e.g., device mismatches) in LA result in finite offset.Offset degrades sensitivity and causes pulse-width distortion, necessitating cancellation technique.Offset may totally destroy the output in high-gain systems (Why?).

  • Offset Cancellation Technique

    outos,1mFoutos,inos, ][ VARGVV =−

    1mF

    inos,

    inos,1mF

    outos, 1

    RGV

    VRAG

    AV

    +=

    FF1mF

    FF1m

    in

    out1

    )(1RsCRAG

    RsCRAGVV

    +++

    =

    Offset cancellation introduces one zero and one pole.Lower corner defined by standards, usually very low.

  • First Order Realization of Gain Stages

    12BW

    1

    1/n0tot

    Lout0

    −=

    =

    ω

    ωCR

    Cascading identical amplifying stages.Trade bandwidth with gain since the latter increases in a way faster than the former decreases.

  • Optimization of Stage Numbers

    For a given technology, the gain-bandwidth product is relatively constant.

    totopt

    1/n1/ntot

    tot

    ln2

    12GBWBW

    AnA

    =⇒

    −=⇒

    For Atot = 50 dB, nopt = 11

    However, noise and power issues limit the number of stage to 5.

  • Large Swing Effect

    Small-signal gain-bandwidth analysis is pessimistic!

    The last few stages switch with large input.The speed of a cascade of stages is limited by only that of one stage.

  • AM/PM Conversion

    3in3in1out VVI αα +=

    )sin(343))sin(

    43()( 2

    3m331

    3m3m11out θθ ωαωαα +−++= tVAtVVAtV

    Noise on input signal amplitudes translates to variations of output zero crossings, i.e., jitter.

  • Broadband Technique (I): Inductive Peaking

    ζω

    ωζωζω

    222 n

    2nn

    2n

    Dmin

    out

    +++

    −=ss

    sRgVV

    LD3dB 2

    1.79CR

    =− 21/=ζLD

    3dB 21

    CRf

    π=−

    for

    Most Efficient method; no extra power consumption.Area consuming (although has been moderated in advanced technology).

  • Broadband Technique (II): Miller Capacitor Cancellation

    1Dmeff1,

    GDDmeffGD,

    )(1)(1CRgCCRgC

    −=

    +=

    GDGDDm

    Dm1 1

    1 CCRgRgC ≈

    −+

    =⇒

    Mismatch or process variation matters.Efficient only for high gain.Button-plate parasitics degrade the performance.

  • Broadband Technique (III): Cherry-Hooper Amplifiers

    Increase the bandwidth significantly in a cost of minor gain loss.Voltage headroom might be an issue in low supply technologies.

    m2

    m1Fm1

    in

    outggRg

    VV

    −=

    Y

    m2Yp,

    X

    m2Xp,

    CgCg

    ω

    ω

  • Broadband Techniques (IV): Voltage-Current Feedback

    Voltage-current (shunt-shunt) feedback can be further applied to multiple stages.Watch level shifting in BJT.

    Double Triple

  • Broadband Techniques (V): f DoublerT

    Din2in1mout )( RVVgV −=

    Double IR drop, voltage headroom issue.Parasitics on tail current sources degrade the performance.Still quite useful in output buffer designs.

  • Broadband Technique (VI): Capacitive Degeneration

    DL

    D

    smss

    ssm

    in

    out1

    21

    )(1RsC

    RRgsCR

    sCRgVV

    +++

    +=

    If RSCS = RDCL, bandwidth increases by a factor of (1+gmRS/2) whereas gain decreases by the same amount.

  • Broadband Technique (VII): Distributed Amplification

    vlfnZgA T0Lmv 2

    π≈=

    Voltage gain is proportional to physical length l.With ideal T-lines, distributed amplifiers would achieve infinite gain with infinite bandwidth!

  • Modified Distributed Amplifiers

    Cascade and segmented structure helps to improve the performance.

  • Realization of Monolithic Transmission Lines

    mm-wave techniques become practical in deep-submicron CMOS.T-lines are lossy but still useful.

  • Challenges of Distributed Amplifiers

    Transmission Line Loss.Output resistance of transistors. Miller capacitance.Propagation velocity mismatches.Routing difficulties in differential realization.PVT variations.

    ⇒ Nevertheless, T-line based distributed amplifiers still provide promising applications.

  • Case Study

    [Galal et al., 2003]