Clock and Data Recovery/Structures and types of CDRs/The jitter tolerance function

Three magnitude functions of jitter tolerance for the three main loop models in the case of phase-aligner architectures.
For each the lateral eye opening is the same, as is the same the length of the elastic buffer (=phase adder).
The two important 2nd order PLLs are plotted as well, in the under-damped but significant condition of ζ = 0.5.
The natural frequency is 500 KHz (ωn= 3.14 e6 rad/sec) and is the same for each of the three loops (yellow marker).

The jitter tolerance of an equipment Edit

In digital networks it is established practice (see for instance some of the ITU-T Recommendations G7xx [1]) to specify (e.g. [1], [2]), and to characterise by measurement [3], the jitter that can be tolerated at the input ports of an equipment.

At any frequency of interest, a sinusoidal input jitter is added to the phase of an otherwise flawless incoming signal, and the jitter amplitude is increased as much as the equipment can tolerate. Beyond that limit, the received data stream is not regenerated perfectly and error bits or slips begin to appear. The same procedure is repeated at different jitter frequencies, to cover all the frequency band of interest for the jitter tolerance and the results are interpolated to obtain a continuous curve.

The boundary of the area (in the plane of jitter frequencies and magnitudes) where the CDR operates without bit errors is then called the curve of jitter tolerance of that equipment.

The errors can either be generated by sampling the received pulses too far from the optimum point, or by slips. In both cases, the tolerance limit has been exceeded.

  • Slips can either come from exceeding the range of the phase comparator, or by exceeding the range of an elastic buffer. The slip is a catastrophic event in terms of BER because, after its occurrence, 50% (statistically) of the regenerated bits are seen as errors and 50% (statistically) are seen as fictitiously correct. The BER is as high as it can ever be (until the framing circuits are able to get in sync again).
  • Error-ed bits. The CDR under test extracts the clock directly from the pulses of the received signal, and then uses it to regenerate the pulses received. The tolerance limit will be reached when the clock that samples the incoming pulses is too far (too early or too late) from the optimum point (the point of “maximum eye opening”, that approximately coincides with the central point between transitions). Such distance from the central sampling point, beyond which errors begin to occur, is called lateral eye opening ΦLEO. Error-ed bits will give evidence that the tolerance limit has been exceeded (even if they only pop up sparsely in small bursts at the moments of peak amplitude of the jitter sinusoidal oscillation).


  1. The jitter tolerance curve always has a "low-pass" shape. The tracking ability of an equipment is best at low frequencies and is low at high frequencies.
  2. At high frequencies, where no more tracking takes place, the equipment can only tolerate the jitter that does not bring the sampling instant to the eye corners. With zero jitter, the sampling point is offset from the central point by the steady state error, if the steady state error is non zero. If the steady state error is zero, the sampling point is in the eye center.
    The tolerance at high frequencies is just a horizontal asymptote, and the asymptote value indicates, for the equipment port under measurement, the difference:
    ΦLEO - steady state error
    where the steady state error is the possible error corresponding to an offset of the frequency of the incoming pulses from the free-running frequency of the local oscillator.
    Such error is \tfrac{\omega_p - \omega_{fr}}{G} [rad] in a slave system of type 1, and is 0 [rad] in a phase aligner system or in any type 2 system.
  3. Towards the lowest frequencies the measured tolerance curve also is asymptotic, but the slope of the asymptote depends on the PLL architecture:
    1. 0 dB/decade, i.e. horizontal, This indicated that an elastic buffer is present to absorb some large low frequency jitter. The horizontal asymptote indicates that the jitter compensation is finite. (The length of the buffer is approximately twice the magnitude of the tolerance represented by the horizontal asymptote).
    2. - 20 dB/decade. This indicated that the receiver is a slave (the local oscillator can follow an infinite phase accumulation, as long as its frequency can track the incoming pulse frequency). The - 20 dB/decade slope tells that the PLL is a type 1 loop.
    3. - 40 dB/decade. This indicated that the receiver is a slave (the local oscillator can follow an infinite phase accumulation, as long as its frequency can track the incoming pulse frequency). The - 20 dB/decade slope tells that the PLL is a type 2 loop.
  4. The tolerance curve sometimes looks like the slope of terraced rice field, with more than one flat section after the first left slope. This indicates that more than one CDR is present along the regeneration path between the injection of the test signal, and that some of them operate at different bit rates.

The tolerance function, a simulation of the the tolerance curveEdit

In a feedback loop, like in a PLL for CDR use, the operation is linear, and the linear modeling remains valid, as long as all blocks in the loop operate within their linearity range.

Increasing the input signal amplitude, a point will be reached where one block reaches the limit of its range of linear operation.

Increasing further the input signal amplitude, the linear model loses its adherence to the real system and the actual operation deviates from the modeled behavior.

When investigating the effects of the timing variation of the input signal (the input jitter), the tolerance function (that can be derived using the border between linear operation and the most important hard non-linearities - see below) is of particular interest. It corresponds to the important characteristic of the CDR that is often a precise requirement, specified and measured as a function of the magnitude of the input sinusoidal jitter at different frequencies. The mathematical function can be very close to the measured curve, and can therefore represent a fundamental engineering tool.

Reaching with the signal level the onset on hard non-linearity inside an internal block often corresponds to the appearance of errored bits in the regenerated data stream. The input signal supplied the CDR has then exceeded the level of the CDR tolerance (such level is a function of the frequency of the input signal).

A mathematical derivation of such jitter tolerance function can be made finding out:

  1. the block in the loop that is first to reach its limit of non-linear operation and to generate errored bits or slips;
  2. the amplitude of the (phase) signal inside such block that reaches the limit of linear operation (such amplitude is a function of ω)
  3. the input signal amplitude (function of ω) that generates such internal signal amplitude.

In mathematical terms, defining as W(jω) the signal at a generic node of the CDR model that is , and as ± Φtol the deviation tolerated at that node,

the tolerance function is the locus, for every angular frequency ω, of the magnitude of the input signal X(jω) that produces a W(jω) that reaches, at one or both of its sinusoidal peaks, the tolerance level for that node:

Jitter tolerance = |X(jω)||W(jω)| = Φtol

is exactly the input (to the CDR) needed for the internal signal to touch the tolerance limit at least at its positive or negative sinusoidal peaks.

Different shortcomings may identify different tolerance functions. They are then combined into one considering, at every frequency, the lowest value among their values.

The function so obtained is called the jitter tolerance function.

In order to derive a tolerance function that simulates well the tolerance curve obtained by measurement, there are 3 (three) fundamental shortcomings of the linear model must be considered :

  • The limited range of the phase comparator
  • The pulse regeneration (= the eye corners and the steady state sampling offset)
  • The limited range of the (possible) elastic buffer.

The limited range of the phase comparatorEdit

The border of normal operation of a phase comparator is reached when the distance in phase between its two inputs exceeds a certain value.

It does not depend on the absolute value of either input, but on their difference only.

The phase comparator is built so that its range covers without discontinuity the period T of one line pulse, and the PLL is designed so that zero difference between the comparator inputs corresponds to the perfect lock of the loop:

Φmax = -T/2 , +T/2 ⇒ = -π , + π .

When Φmax is exceeded by the error signal x(t)-y(t), the phase comparator output falls into the next period of its characteristic and its output indicates to the PLL that the closest locking point is now the center of the nearby pulse.

If the transient is short enough the loop has no time to react, the error signal comes back quickly within range, and the output goes back to the original segment of the comparator characteristic. A large burst of errors have affected the CDR, but at the end there is no slip of the recovered clock

If instead the transient lasts long enough for the loop to react, then lock will be achieved at the center of the new segment of the comparator characteristic: a slip has occurred.

Mathematically such limit of linearity of the phase comparator characteristic defines one of the tolerance curves of the closed loop. Such tolerance can be modeled as the locus -for every frequency- of the magnitudes of sinusoidal input signals X(jω) such that :

|X(jω) - Y(jω)| = |Ε(jω)| = \Phimax =  \pi

But, in the particular case of the measurement of the tolerance curve, as well as in the derivation of the tolerance function, the range extremes of the phase comparator are never reached!

Its range may be exceeded during real operation, in particular during the early phase of a difficult acquisition of phase lock, but it will not be reached while finding the tolerance limit.

In fact, the range of error-less sampling corresponds a sub-range of the phase comparator range. Sampling errors do appear as a consequence of sinusoidal jitter when the lateral eye margin is reached, while the comparator range limit is always larger. The following figure helps identify the quantities involved and clarify the related concepts, and the following sub-paragraph addresses the loop tolerance associated with the sampling phase margin.

The pulse regeneration (= the eye corners and the steady state sampling offset)Edit

The pulse regeneration may not take place at the best instant because of a timing deviation.
There is margin against a bit error resulting from a misplaced sampling instant.
Looking at the eye diagram it is easy to identify the margin.

The tolerance function due to the lateral closure of the eye diagram can be modeled by an equation like the one resulting from the comparator range, but using a tighter range limit, and taking also into consideration the possible sampling offset that exists in some cases.

The input jitter that is not tracked by the PLL leaves a residual (sinusoidal) error between input (that represents the eye center) and output (that represents the sampling instant).

Overall, the output y(t) is not able to track exactly the input x(t) because of two shortcomings:

  1. a d.c. offset (the steady state error) and
  2. its (sinusoidal) phase variation is not able to replicate exactly the input (sinusoidal) phase variation, and a (sinusoidal) error of the same frequency remains.

When the sinusoidal error adds to the steady state error the sampling may take place before the beginning transition or after the end transition of the pulse.

Just one, or a few, or a high density of errors are equally relevant in the identification of the tolerance limit. In other words, the limit is meant to have been reached when the sampling takes place in what could be a wrong instant, even if the irregular jitter of the beginning or of the end of the pulse do not necessary imply an error at every bit time, but with a lower frequency of occurrence. (It should be remarked that the "irregular jitter" of the transitions happens at random -due to line noise and I.I.- but to a large extent faster than the sinusoidal jitter of the tolerance measurement or simulation).

|X(jω)||X(jω)-Y(jω)| = Φleo = |X(jω)||Ε(jω)| = Φleo

where Φleo ≤ Φmax.

When the error signal instantaneously exceeds Φleo, error bits are generated in the CDR with a certain probability.

When the error signal exceeds Φmax and a slip consolidates, the BER remains very high as long as the framing circuits downstream of the CDR re-align (in a real transmission network) or as long as the sequence recognition circuits of the BER tester re-align (in a tolerance curve test set-up) .

The curves in the figure above can be seen as examples, with the exclusion of the flat asymptote towards low frequencies.
The tolerance due to the lateral eye closure decreases with increasing frequency and flattens out at high frequencies.
The clamping of the curves at low frequencies if present because the circuits described incorporate an elastic buffer (see section here below).

The limited range of the (possible) elastic bufferEdit

In general, a buffer may come in various forms, grouped here below in three categories of decreasing added delay:

  • Buffer memories used to store and forward large amounts of bits, like packets of a TCP/IP protocol.
    They are often organised by byte, and are written and read with clocks running at the byte rate.
    The memory is so deep -and the added delay is so large with respect to the bit period- that they easily absorb the timing jitter or the frequency mismatch between the write and the read clocks.
    These buffers could be located inside a single clock domain or at the border of two different domains.
  • Elastic buffers between clock domains.
    They are meant to absorb or at least to mitigate the effects of jitter, wander and drifts between the clocks of the two domains.
    Their depth is chosen to absorb the clocks drifts with as rare slips as possible. These elastic buffers are not as deep as a buffer memory but much deeper than a phase adder in a phase aligner (see below).
    As there is no prior knowledge of the drift sign, their end of range triggers a reset to the central point.
    They deal with serial transmissions and are essentially based on shift registers clocked with the incoming clock and read with the local clock.
    Their tolerance is studied using linear phase ramps.
  • Phase adders for Phase aligner CDRs.
    Only a clock domain is involved and there are no d.c. drifts between the incoming signal and the local clock.
    They are meant to absorb just the a.c. jitter that has been generated in a relatively short timing loop inside an equipment or in a downstream/upstream loop of an access network.
    Their tolerance is studied with sinusoidal jitter i.e. with Fourier transforms.
    The border of linear operation (= of the tolerance) of a phase adder is typically found when the algebraic sum of the phases of its two inputs reaches the minimum or the maximum value allowed for the output range of the adder.
    It does not depend on the value of either input, even though in practice such limits of tolerance are often reached when one input simply swings too wide.
    The mathematical model shall be:
Magnitude of [I1(jω) + I2(jω)] = |I1(jω) + I2(jω)| = Φmax
where +/- Φmax are the largest values that the adder can process linearly.
As there is no drift at all, but just alternating jitter, at the end-of-range the adder saturates (as explained below for the delay line implementation).
The model (of steady state condition), with |I1(jω) + I2(jω)| = 0 for the mid output point, is chosen because it matches the corresponding hypothesis that, if the initial delay was not the mid point, then a transient out-of-range with subsequent re-centering has occurred.
The phase adder of a PLL is a delay line
In PLLs the phase adder is implemented in the form of a delay line. The input of the delay line is one input of the adder, while the other input simply controls the amount of delay added to the signal that enters the delay line.
Such adders can tolerate an added delay between zero and the maximum length of the delay line, Dmax.
The delay can also be measured as a phase, in units of radians at the angular frequency of interest.
If a delay is known in seconds, then it can be be converted into radian
multiplying it by the angular clock frequency: [sec] * [rad * sec-1] = [rad].
The tolerance limit will be in such cases modeled as:
0 < added delay < Dmax.
When the tolerance extremes are exceeded, the delay lines simply saturates in the sense that it either does not add any delay or that it keeps on adding its maximum delay Dmax. In terms of signal phases, the output remains constant at its minimum or maximum value.
In the case of a phase phase lock loop incorporating the delay line, this means opening the loop until the input jitter changes its direction of variation. The delay range is frozen while the input jitter waveform insists in the same direction and until it starts getting back. At that moment the lock resumes, but the delay range is now translated towards the average value of the incoming jitter by the amount of the sidetracking.
This achieves some sort of translation of the delay range towards re-centering around the average value of the input the jitter. It is important to observe that this takes place in a discontinuous mode, because the loop keeps on re-locking into the center of the closest pulse in the delayed waveform presented to its phase comparator. This adds an imprecision of ± π to the positioning of the delay line with respect to the incoming signal, and consquently to the loop jitter tolerance.
The granularity of the delay line can be as coarse as about 1/3 of the line pulse period (π/2 - ε in theory), or as fine as fraction of one percent of such period. This granularity adds with the imprecision of the point above in reducing the resulting tolerance.
To model the phase tolerance curve associated to the delay line in the phase alignerthe following points are considered:
- Initial conditions. Sufficient re-centerings have occurred in the past, and presently the delay is centered with the inevitable imprecision of ± π
- A granularity of Φgran characterizes the delay line;
- total delay that the delay line can adjust is Dmax:
The tolerance limit imposed by the phase adder to the phase aligner is a fixed amount at all frequencies and is modeled as follows:
|X(jω)| < (Dmax/2 - π - Φgran)

The curves in the figure above can be seen as examples of tolerance of phase adders in the flat part at low frequencies..
Such clamping of the curves at low frequencies if present because the tolerance of the elastic buffer (present in the circuits of the figure) is independent from the jitter frequency and only depends on the length of the buffer. The tolerance due to the lateral eye closure further reduces the tolerance at mid and high frequencies and ultimately flattens out at very high frequencies (see section here above).


  • It should be emphasized that the jitter tolerance function is:
    • neither a transfer function (its output is not generated with input frequencies of unit amplitude)
    • nor a part of the mathematical model in the strict sense
      (because it depends on non-linearities for its definition, although it is computed within the boundary of the circuit linear operation, and
      because it may be different for different architectural variants belonging to the same model architecture. See the example of the 1st order type 1 phase aligner that has a different tolerance from the 1st order type 1 slave).
  • In the cases where the tolerance function is determined only by the maximum difference acceptable inside the phase comparator, the tolerance limit is a consequence of the one sided eye opening and not of the comparator range (that is larger).
Exceeding the comparator range (±π) generates slips (= very high BER) while exceeding the lateral eye opening only generates error bursts that can be rather short. But the lateral eye range is reached always before the comparator range is exceeded: the tolerance function (as well as the tolerance curve!) corresponds to the errors that occur at the eye corners. Phase comparator slips (and associated errors) do occur in a CDR, but beyond the limit of tolerance set by the lateral eye aperture.
Such high frequency jitter tolerance is visible (and is measurable) as the horizontal asymptote at the highest frequencies of jitter. From a certain frequency up, the PLL does not track at all, the jitter imposed to the input signal moves back and forward the signal transitions (already affected by I.I., noise etc.) and the sampling clock does not move.
The tolerance function derived from the eye opening in such case still replicates very well, in magnitude, characteristic asymptotes and corner frequencies the diagram that is obtained with an actual measurement.
  • Where more than one non-linearity define each a region of tolerance for a CDR, then the overall CDR tolerance will correspond to the intersection of those tolerance regions.


  1. ITU-T Rec. G.813 (03/2003) in particular Appendix II
  2. -G.825-2000.03-The control of jitter and wander within digital networks which are based on the synchronous digital hierarchy (SDH): 6.1 Jitter and wander tolerance for STM-N input ports
  3. Ransom Stephens, “Tektronics Jitter 360° Knowledge Series” from

Last modified on 5 April 2013, at 14:04