a stabilization technique for phase-locked frequency synthesizers tai-cheng lee and behzad razavi...

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A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003 Vladimir Ivanov October 23, 2007

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Page 1: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

A Stabilization Technique forPhase-Locked Frequency SynthesizersTai-Cheng Lee and Behzad RazaviIEEE Journal of Solid-State Circuits, Vol. 38, June 2003

Vladimir IvanovOctober 23, 2007

Page 2: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Outline

Integer-N PLL frequency synthesizer Conventional architecture Two proposals Delay network Synthesizer design Simulations Experimental results Performance Summary

Page 3: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Integer-N PLL frequency synthesizer

Phase-frequency Detector (PFD) compares phases and sends voltage pulses to CP

Charge Pump (CP) converts the voltage pulses into current pulses

Loop filter converts current pulses into a voltage level

Voltage-controlled Oscillator (VCO) produces frequency proportional to its control input

Page 4: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Conventional architecture

R1 provides the stabilizing zero

C2 lowers the ripple on Vcont

C1 determines the settling time

Tight tradeoff: settling time vs. ripple on Vcont

Goal: relax this tradeoff

Page 5: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Overview To avoid overdamped settling, C2 ~ C1/10

Therefore, C1 has to be large Idea: stabilize by creating a zero without the

resistor Thus, C1 both defines the switching speed and

suppresses the ripples Approach: create a zero through a discrete-time

delay Achieves both fast settling and small ripple Obviates the resistor in the loop filter => digital CMOS “Amplifies” the value of the loop filter capacitor

=> saves die area Two proposals: delay before and delay after CP2

Page 6: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Proposal 1: delay before CP2

CP1 drives C1 directly

CP2 injects charge in C1 after time ΔT Transfer function: Zero: To have ωz low enough and desired loop

behavior, ΔT ~ 500 ns

Page 7: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Proposal 1: delay before CP2

Problems with Proposal 11. The delay line has to:

provide very large ΔT and accommodate a wide range of

UP and DN pulsewidths

2. ΔT varies with process and temperature; therefore, the damping factor (and thus the stability) may be affected because

Proposal 2: place the delay line after CP2

Page 8: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Proposal 2: delay after CP2

If loop settling time >> 1/fREF and C2>>C1: C2 value “amplified” by 1/(1-)

ωz achieved without resistors damping factor much less depended on process

and temperature

Page 9: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Delay network

Page 10: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Synthesizer design

Page 11: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Comparison with conventional architecture

Loop filters: type A (delay-sampled) andtype B (conventional)

Gain: about 10 dB lower sidebands

Page 12: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Simulations Simulation takes very long time due to:

Very different time scales Large number of devices

Two models to speed up the design: Linear discrete-time model (in Matlab):

to compute optimal CP current, C1 and Cs

Transistor-level model: to study the nonidealities of PFD, CP, and VCO1. Time contraction: fREF scaled up by 100;

C2 and M scaled down by 1002. Divider realized as a simple behavioral

model with ideal devices

Page 13: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Experimental results

Page 14: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Experimental results

Page 15: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Performance

Page 16: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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Summary

Proposed PLL stabilization technique by creating a zero in the open-loop TF which: Relaxes the tradeoff between the settling

time and ripple on the VCO control voltage

Makes the resistor in the loop filter unnecessary

“Amplifies” the loop filter capacitor, saving die area

Page 17: A Stabilization Technique for Phase-Locked Frequency Synthesizers Tai-Cheng Lee and Behzad Razavi IEEE Journal of Solid-State Circuits, Vol. 38, June 2003

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VCO design

Inductors: 180μm x 180μm ~ 14 nH with Q = 4 (100 fF)

Varactors: 160 fF with tuning range ~ 12%

VCO phase noise: -120 dBc/Hz at 1 MHz