Clock and Data Recovery for Serial Digital Communication
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1 Clock and Data Recovery for Serial Digital Communication Rick Walker Hewlett-Packard Company Palo Alto, California
2 Basic Idea Serial data transmission sends binary bits of track information drifting tx as clock a series and prop of optical delay or variation electrical + identify pulses: bits The transmission channel (coax, radio, fiber) generally distorts the signal in various ways: From this signal we must recover both clock and data 5
3 Eye diagram Use a precise clock to chop the received data into periods Overlay each of the periods onto one plot symbol cell } X Y X jitter Y amplitude distribution at Y-Y 7
4 Eye diagram construction random data TX RX link synth scope trigger 6
5 Definition of Jitter unit interval -3T -2T -T 0 T 2T 3T 4T Impulses spaced equally in time (jitter free signal) time -3T -2T -T 0 T 2T 3T 4T Impulses spaced irregularly in time (jittered signal) Errors treated as discrete samples of continuous time jitter After Trischitta and Varma: Jitter in Digital Transmission Systems 20
6 Analytic Treatment of Jitter Perfect Clock: xt () = Acosω c t Jittered Clock: xt () = Acos[ ω c t + φ() t ] φ() t is then treated as a continuous time signal After Behzad Razavi: Monolithic Phase-Locked Loops, ISSCC96 Tutorial 29
7 Data Recovery with simple PLL Jittered Data Signal D Q Retimed Data PLL Phase Detector Low-pass Loop Filter Voltage Controlled Oscillator 28
8 Model of Loop Phase Detector Loop Filter VCO K 1 φ K v -- s β + 1 ( sτ) Warning: Extra Integration in loop makes for tricky design! See Floyd M. Gardner, Phaselock Techniques, John Wiley and Sons, for good introduction to PLL theory 30
9 Loop Frequency Response a (input data jitter) K φ β + 1 ( sτ) K v s b c (vco phase noise) 80dB 40dB 0dB c/a open loop gain c/b -40dB -80dB 1k 10k 100k 1M 10M 100M 1G 10G 31
10 Jitter Measurements SONET has most complete set of jitter measurement standards, but the techniques are useful and relevant for datacom applications also. Jitter Tolerance Jitter Transfer Jitter Generation 46
11 Jitter Tolerance Test Setup laser transmitter optical receiver data generator xamp + limiter decision circuit bit error rate tester FM modulated clock optical attenuator retiming circuit sine wave generator At each frequency, the sinewave modulation amplitude is increased until the BER penalty is equal to that caused by 1dB optical attentuation After Trischitta and Varma: Jitter in Digital Transmission Systems 47
12 SONET Jitter Tolerance Mask 15 UI 1.5 UI acceptable range 0.15 UI f 0 f 1 f 2 f 3 f t Data Rate f 0 [Hz] f 1 [Hz] f 2 [Hz] f 3 [khz] f t [khz] 155 Mb Mb Gb Gb??? from SONET SPEC: TA-NWT Issue 6, Sept. 1990, fig
13 Jitter Transfer Measurement data generator decision circuit clock Phase detector Signal Generator D.U.T. retiming circuit Phase modulator ϕ [TrV89] [RaO91] IN OUT network analyzer 49
14 Jitter Transfer Analysis clock amplitude sideband Θ resultant Assuming small angles (i.e.: only one dominant sideband on recovered clock): Jitter pp( rads) = 2 Θ 2 V sideband atan V clock Jitter transfer is defined as the jitter at the clock output divided by the jitter at the D.U.T input, plotted as a function of jitter frequency.??
15 Jitter Transfer Specification P[dB] slope = -20 db/decade acceptable range f c Data Rate f c [khz] P[dB] 155 Mb Mb Gb This specification is intended to control jitter peaking in long repeater chains 50
16 Some Signal Degradation Mechanisms Multiplex Jitter AC Coupling Optical Pulse Dispersion Skin Loss Random Noise E+O Crosstalk Intersymbol Interference 8
17 Multiplex Jitter bit stuffing events high speed data sub-rate data phase error [in UI] time Multiplex jitter is not a problem on the high rate channel itself - it only occurs on non-synchronous, lower speed tributaries that have been sent over the high-speed channel (e.g.: DS3 over SONET OC-48). 9
18 Voltage and Time aberrations caused by AC-coupling t V V t t=0 t=t 1 AC coupled pulses droop as P V V t t V RC Jitter is introduced by finite slope of pulse rise/fall time: t r t 1 t = ( 2RC) 10
19 Jitter Generation decision circuit computer retiming circuit spectrum analyzer S.U.T. recovered clock 51
20 Jitter Generation (cont.) 1) Measure Jitter Sidebands around Clock Jitter pp( rads) = 2 Θ 2 V sideband atan V clock 2) Multiply Jitter components by Filter Mask 3) RMS sum total noise voltages over band 4) Convert RMS noise voltage to RMS jitter clock amplitude sideband Θ resultant OC-48 (2.488 Gb/s SONET) specifies 12 khz hipass filter, and maximum 0.01 UI RMS integrated jitter. 52
21 Decision Circuit Quantizes amplitude at precise sample instant Typically uses positive feedback to resolve small input signals A master/slave D-flip-flop carefully optimized for input sensitivity and clock phase margin is a common choice Latches input data on rising edge of clock signal simplified schematic symbol: D Q clock 39
22 Code Disparity Disparity is defined as N high - N low in past transmitted signal encoded data signal signal disparity In an unbalanced code the disparity can grow without limit. e.g.: 4B5B code of FDDI In a balanced code, the disparity is limited to a finite worst case value. e.g.: 8B10B of FibreChannel After Tom Hornak: Interface Electronics for Fiber Optic Computer Links, (see bibliography for full citation) 16
23 Filter Method Examples d dt X 2 bandpass filter NRZ Data Input non-linear element delay e.g.: SAW filter bandpass filter LC tank Recovered Clock Output (this last circuit can be thought of as an NRZ-RZ converter) 25
24 Spectrum of NRZ data variations due to DC balance strategy power in db sin( 2πfT) π ft missing clock frequency f = 0 1 2T 1 T 3 2T 2 T 22
25 NRZ and RZ signalling NRZ = non return to zero data RZ = return to zero data neither clock nor data frequency in spectrum data frequency clock frequency clock,butno data frequency in spectrum T NRZ signalling is almost universally used. 21
26 A detailed look at the spectrum of differentiated NRZ missing clock frequency power in db ± k f = 0 f c 2 f c A k 2π f c sin ± 2 k ± Θ k k 23
27 Reconstructing the Clock Start with symmetric sideband pairs about f c /2: A k 2π f c sin ± 2 k ± Θ k k Mix data signal with itself (e.g.: square law): 1 sinαsinβ = -- 2 cos( α β) cos( α+ β) All the symmetric sidebands mix pairwise to coherently create a carrier frequency component: direct implementation of this principle is Filter Method 24
28 Example Bipolar Decision Circuit master latch slave latch gnd data in clock in Vbias data out -5V many clever optimizations are possible 40
29 Summary of Filter Method Jittered NRZ Data Signal D Q Retimed Data d dt X 2 bandpass filter/limiter Pro: Very simple to implement Can be built with microwave tinkertoys using coax to very high frequencies Con: Temperature and frequency variation of filter group delay makes sampling time difficult to control Narrow pulses imply high f T Hi-Q filter difficult to integrate 26
30 Example MOS Decision Circuit master latch data in clock slave latch clock decision circuits can be implemented in NMOS technology up to Gb/s speeds 41
31 Decision Threshold Generation To minimize bit-error rate, the decision threshold X-X must centered in the signal swing. Two common ways of automatically generating threshold voltage are: Peak detection of signal extremes, limited run-length required Signal positive peak detector negative peak detector Decision Threshold Decision threshold = signal average, balanced signal required Signal Low-Pass Filter Decision Threshold After Tom Hornak: Interface Electronics for Fiber Optic Computer Links, (see bibliography for full citation) 15
32 Quantized Feedback AC-Coupled Transmission Link TX H( ω) RX Feedback voltage models missing DC information 1 H( ω) D Q Output Data (models ideal TX waveform) clock 11
33 Phasor Diagram Graph of relative phase between clock and data Each complete rotation is 1 unit interval of phase slip Rotations/second = frequency error (in Hz) 0 Plot of data transitions versus VCO clock phase Data at 1/2, or VCO at 2x, the proper frequency look locked. This puts a limit on VCO tolerance to prevent false locking. = missing transitions = actual transitions 43
34 Example Lock Detector 0 [FP15.5] ideal data eye noisy data eye 180 clock a,b data D Q D Q Raw out-of lock indication 44
35 Aided Acquistion Tricky task due to Nyquist sampling constraints caused by stuttering data transitions Input Data PD loop filter 1 VCO FD loop filter 2 Still subject to false lock if VCO range is too wide After Behzad Razavi: Monolithic Phase-Locked Loops, ISSCC96 Tutorial 42
36 Phase Detectors Phase detectors generate a DC component proportional to deviation of the sampling point from center of bit-cell Phase detectors are: Continuous Binary Quantized Binary quantized phase detectors are also called Bangbang phase detectors After Tom Hornak: Interface Electronics for Fiber Optic Computer Links, (see bibliography for full citation) 32
37 Training Loops retimed data Data bang-bang drive Input PDET select charge pump VCO Clock Reference Clock 2.488GHz/256 FDET dlock dtrans flock State Machine LOS Clock/256 1/256 divider An increasingly common technique is to provide a reference clock to the CDR circuit. This allows the VCO process-variation to be dynamically trimmed out, avoiding false locking problems. (Figure from paper FP15.5, 1997 ISSCC) 45
38 Coding for Desirable Properties DC balance, low disparity Bounded run length High Coding Efficiency Spectral Properties (decrease HF and/or DC component) Many Variations are Possible! Manchester [San82] mb/nb [Gri69][Rou76][WiF83] [YKI84] [Pet88] Scrambling [CCI90] CIMT [WHY91] 17
39 Simple 3B/4B code example 4B Output Data 3B Input Data Even Words Odd Words Maximum Runlength is 6 Coding Efficiency is 4/3 Sending Sync Sequence: SyncA(even), SyncA(odd), SyncB(even), SyncB(odd) allows the unambiguous alignment of 4-bit frame SyncA SyncB
40 Scrambling Uses a feedback shift register to randomize data - reversing process at receiver restores original data Data Input Scrambled Data Data Output XOR Shift Register n j 2 1 Clk 1 2 j n PRBS Generators Caveat: Only guarantees balance and runlength under very specific data conditions! After Tom Hornak: Interface Electronics for Fiber Optic Computer Links, (see bibliography for full citation) 19
41 VCO alternatives LC Oscillator Multivibrator Ring Oscillator Speed Technology Dependent 1-10 s of GHz, CMOS 1-2 GHz Phase Noise Good Poor Integration Poor (L, Varactor) Excellent Tunability Narrow/Slow Wide/Fast Stability Good Poor (needs acquisition aid) Other Multi-Phase Clocks [Cor79, Ena87, Wal89, DeV91,Lam93, WKG94] After Todd Weigandt, B. Kim, P.Gray, Timing Jitter Analysis for High-Frequency CMOS Ring Oscillators, March 10,
42 Multivibrator VCO I tune Capacitor is alternately charged and discharged by constant current Tuned by varying I tune in current source Diode clamps keep output voltage constant independent of frequency Relies on non-linear switching for oscillation behavior, and so is limited to moderate frequencies. Frequency = I tune CV be After Alan B. Grebene, Analog Integrated Circuit Design, Van Nostrand Reinhold, 1972, pp
43 Example Ring Oscillator VCO Output Tune Input 1 Input 2 [SyA86] [EnA87] [Wal89] Input 1 Output Input 2 Input 1 Tune Input 2 Output 38
44 Loop Filters may be analog (integrator) or digital (up-down counter) should have provision for holding value constant (tristating) under long run-length conditions [Den88] [Dev91] [LaW91] [WuW92] V OUT UP DOWN V OUT 0 0 tristate UP DOWN 0 1 ramp DOWN 1 0 ramp UP 1 1 tristate 35
45 Skin Loss Nearly all cables can be modeled by the Skin Loss Equation with various k factors: T( f) = 10 ( k) f. 1.0 linear amplitude k=.0001 k= k=.001 R3 R2 R1 L3 Ring 3 Ring 2 Ring1 L k freq (log scale) [YFW82] 10G Three-element equivalent circuit of a conductor with skin loss 12
46 Skin Loss Equalization at Transmitter boost the first pulse after every transition Error at sampling pt. usable signal See Paper: FP15.1, 1997 ISSCC before after 14
47 Skin Loss Equalization at Receiver transmission (linear scale) k pure skin loss freq (log) 3dB boost equalized 10G 2x improvement in maximum usable bit-rate [WWS92] 13
48 Agenda Overview of Serial Data Communications Signal Degradation Mechanisms Data Coding Techniques Clock Recovery Methods Components Used in Clock/Data Recovery Jitter Measurements 2
49 Diversity of CDR applications Clock and Data Recovery (CDR) applications span the range from ultra-high-volume, low cost datacom applications to very high precision, long-haul telecom applications Many different trade-offs are made to tailor each circuit to the target application area 1.25Gb/s Gigabit Ethernet Transceiver <$10 in volume (datacom application) 1cm 2.488Gb/s SONET CDR ~$500 (telecom application) 3
50 Q-Factor in resonant circuits Voltage envelope of ringing circuit falls to 1/sqrt(e) in Q radians /sqrt(e) Q/2*PI cycles Q also equals the center frequency of a filter divided by the full-width of the resonance measured at the half power points: F center / amplitude F center High-Q filter can be emulated by PLL with low loop B.W. 27
51 Bit Error Rate (BER) Testing Pseudo-Random-Bit-Sequence (PRBS) is used to simulate random data for transmission across the link PRBS pattern 2 N -1 Bits long contains all N-bit patterns Number of errored-bits divided by total bits = BER. Typical links are designed for BERs better than PRBS data generator TX link RX PRBS data receiver clock in synth clock in 4
52 Drawbacks of Simple PLL 1) timing pulses 2) transfer function (linear vs BB), 3) quadratic, BB 4) critical problem is the stuttering data??
53 Self-Correcting Phase Detector UP Data Clock DQ DQ DOWN Data See FA9.6, 1997 ISSCC [Hog85][Shi87] 1 = Data... 2= Clock (Early)... 3 = 1 retimed... 4 = Clock... 5 = 3 retimed... 6 = 1 xor 3 (UP)... 7 = 3xor 5 (DOWN) 33
54 Data Clock Binary Quantized Phase Detector NRZ data is sampled at each bit cell and near the transitions of each bit cell The sign of the transition sample is compared with the preceeding and following bit cell sample to deduce the phase error DQ DQ DQ DQ A B T ATB [Ale75][WHY91] [LaW91][ReG73] A T B Output tristate vco fast 0 1 0? vco slow vco slow 1 0 1? vco fast tristate 34
55 CDR Design Checklist 1) Eye Margin how much noise can be added to the input signal while maintaining target BER? (voltage margin) How far can clock phase alignment be varied while maintaining target BER? phase margin) how much does the static phase error vary versus frequency, temperature and process variation? Is input amplifier gain, noise and offset sufficient?
56 CDR Design Checklist (cont) 2) Jitter Characteristics what is the jitter generation? (VCO phase noise, etc) what is the jitter transfer function? (peaking and bandwidth)what is the jitter tracking tolerance versus frequency?
57 CDR Design Checklist (cont) 3) Pattern Dependency how do long runlengths affect system performance? is bandwidth sufficient for individual isolated bit pulses? are there other problematic data patterns? (resonances) does PLL bandwidth, jitter, and stability change versus transition density? 4) Acquisition Time what is the initial, power-on lock time? what is the phase-lock aquisition time when input source is changed?
58 CDR Design Checklist (cont) 5) How is precision achieved? are external capacitors, inductors needed? does the CDR need an external reference frequency? are laser-trimming or highly precise IC processes required? 6) Input/output impedance Is S11/S22 (input/output impedance) maintained across the frequency band? are reflection large enough to lead to eye closure and pattern dependency? is t >15 db return loss maintained across the band?
59 CDR Design Checklist (cont) 7) Power Supply does the CDR create power supply noise? how sensitive is the CDR to supply noise? Is the VCO self-modulated through its own supply noise? (can be deadly ) what is the total static power dissipation? what is the die temperature under worse case conditions?
60 CDR Design Checklist (cont) 8) False lock susceptibility can false lock occur? are false lock conditions be detected and eliminated? can the VCO run faster than the phase/frequency detector can operate? (another killer ) have all latchup/deadly embrace conditions been considered and eliminated?
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