Performance of stochastic clocks in the Alternate Ticks Game

Performance of stochastic clocks in the Alternate Ticks Game


In standard quantum theory, time is not an observable. It enters as a parameter in the Schrödinger equation, but there is no measurement operator associated to it. Nevertheless, one may take an operational viewpoint and regard time as the information one can read from clocks. The Alternate Ticks Game, introduced in [arXiv:1506.01373], is a completely operational means to quantify the accuracy of time scales generated by clocks. The idea is to count the number of ticks that two copies of a clock can produce until they run out of synchronisation. Here we investigate the performance of stochastic clocks in this game. These are clocks which are classical in the sense that they do not exploit quantum coherence. Our results support earlier conjectures that their accuracy grows linearly in the size of the clockwork, measured in terms of the dimension of the associated Hilbert space. In particular, we derive explicit bounds on the accuracy of a natural class of stochastic clocks, the stochastic ladder clocks.

Time enters as a parameter in the quantum-mechanical equations of motion. Treating time in this way is convenient in many cases, but it also bears conceptual problems. These become apparent if one tries to reconcile quantum mechanics with other physical theories. Indeed, one talks about the “problem of time” when describing obstacles that arise in attempts to quantise general relativity DeWitt (); Kuchar (); Isham (). The treatment of time as a parameter is also problematic from a thermodynamic point of view ThermodynamicsOfTime (). An alternative could be to represent time in terms of an operator, analogously to the quantum-mechanical position or momentum operators, but this turned out to be impossible in general Pauli (); PauliTwo (); BuschTimeOperator (); PashbyThesis ().

These problems may be avoided by an operational approach to time. According to this approach, time is what one reads from a clock. In other words, time scales are generated by clocks, which are modelled as physical systems. The approach has a long tradition and certainly played a key role in the development of relativity theory EinsteinClock (). It is therefore to be expected that it can also teach us something about quantum mechanics and its relation to other physical theories, as well as about cosmology. For example, the proposal to describe time as correlations between a clock and other systems, and extensions thereof, PageWootters (); Wootters (); Mott (); Briggs (); Brout (); GiovannettiQuantumTime (); ChiaraVlatko () certainly fits into this operational picture. The operational approach has also inspired work in quantum information theory. An example is the question whether clock synchronisation schemes that use quantum communication have advantages over classical ones PreskillClockSynchronisation (); JozsaClockSynchronisation (); Eddington (). Another one, related to quantum thermodynamics, is whether measuring time has a thermodynamical cost PauliThesis (); MischaRalph (); ThermodynamicQClock (); InflationUniverse ().

Clocks, regarded as actual physical systems, are obviously subject to physical constraints, which may limit their accuracy. One of these constraints is that clocks have a finite size. Taking a quantum-information perspective, it is natural to quantify size in terms of the dimension  of the Hilbert space associated to the clockwork. This is made precise by the framework proposed in ClockModel (), where clocks are modelled as general quantum systems that emit time information, the ticks, to their environment.

The accuracy of such tick-emitting clocks can be quantified in a purely operational manner in terms of the Alternate Ticks Game (AT Game) ClockModel (). In this game, the aim is to set up two clocks in such a way that their ticks occur in an alternating order for as long as possible. The game stops as soon as one of the clocks emits two ticks in a row without a tick by the other clock in between. The score, , of the game is the expected number of ticks emitted by each clock until this happens. The score achieved by the best strategy is then a measure for how well the two clocks can be synchronised. To turn this into a measure for the accuracy of a clock, one simply plays the AT Game with two copies of the clock.

Here we focus on a particular type of clocks, called stochastic clocks. These are, in some sense, the “most classical” clocks within the framework of ClockModel (), in the sense that their internal state is assumed to decohere quickly (i.e., much faster than the time scale on which the clock operates). As we will see, stochastic clocks exhibit some simple properties which make them particularly convenient to investigate. Specifically, they can be modelled as a system with perfectly distinguishable and, in this sense, classical states. Furthermore, the sequence of states that a stochastic clock admits can be represented in terms of a Markov chain.

Our main results are lower and upper bounds on the accuracy of stochastic clocks, measured in terms of the expected score  in the AT Game that is achieved by the best strategy (Theorem 1). The bounds depend on the size  of the clockwork. For stochastic clocks, corresponds to the number of classical states that the clockwork can admit. The bounds may be evaluated for specific clock constructions, such as stochastic ladder clocks. We find that, for this type of clocks, the accuracy  grows linearly in  (Theorem 2).

Numerical results ClockModel (); ChrisThesis () suggest that general quantum clocks can achieve accuracies  that exceed this linear bound. That quantum coherence can indeed be exploited to build more accurate clocks has recently also been shown analytically for very large dimensions RPaper (), although with respect to a different measure of accuracy (see Section V for more details). It is therefore natural to conjecture that genuinely quantum clocks can outperform the best stochastic ones in the AT Game. The results presented here may be regarded as a stepping stone towards proving this conjecture.

I The General Clock Model

In order to facilitate comparison with other clock constructions, we will describe stochastic clocks, which are the main subject of this paper, within the general framework of quantum clocks introduced in ClockModel (). The idea underlying this general model is that a clock can be regarded as a physical system equipped with a mechanism that emits time information. To describe this mechanism, one considers two systems:

  • Clockwork (denoted ): This is the running (dynamical) part of the clock. It interacts with its environment, thereby outputting time information.

  • Tick registers (denoted ): These belong to the environment of the clockwork. Each tick register  is, in sequential order, brought in brief contact with the clockwork to record time information. After this interaction, it is separated from the clockwork, keeping a record of the clock time.

This idea is captured by the following definition.

Definition 1.

A quantum clock is defined by a pair , where is a density operator of a system , called clockwork, and is a completely positive trace preserving (CPTP) map from to a composite system , where is called tick register.

The map may be decomposed into a part corresponding to an internal evolution of the clockwork and a part that extracts time information from the clockwork to the tick registers. However, one can also always take the internal evolution to be a trivial map, i.e. , and incorporate the entire clock dynamics into the action of the measuring map . In the case of the stochastic clock (Definition 3 below), the clockwork consists of a finite number of “classical” states, and the evolution can be represented probabilistically, hence the label stochastic clock. Inspired by the Salecker-Wigner-Peres clock model Salecker1958 (); Peres (), we can picture a stochastic clock as a pointer moving on a circle, but with discretised dynamics. In other words, the clock’s evolution can be characterised by the probabilities that determine how likely it moves from one state to another. We will refer to these discrete movements as jumps.

Before proceeding to the formal definition of stochastic clocks, we first introduce a property for quantum clocks which captures the idea that the dynamics of any physically realistic clock must be continuous to a certain degree. The definition is also taken from ClockModel ().

Definition 2.

A quantum clock is called -continuous if the map restricted to is -close to the identity map , i.e.,


where is the diamond norm.

To fulfil this continuity condition for the clock, the total change of the clock state at every step has to be small enough. This means, in particular, that in any single application of the clock map, the occurrence of a tick must have a small probability. We will show below that a stochastic clock whose jump probabilities are upper bounded by is at least -continuous.

Ii Stochastic clocks

To define stochastic clocks we need to specify under what conditions such a clock produces a tick. We require that the tick registers output ticks (represented by in the two-dimensional tick register space) with a certain probability, whenever the clock system makes a jump that passes to or over the state from a non-zero state. Note that without loss of generality one can choose any other state or states on the circle for the tick states. For all other jumps the tick register would provide no-tick — events (represented by ). Note that one can think of these clocks as the reset clocks, since we will require that the clock starts over from the state if the tick occurs.

In contrast to a general quantum clock, stochastic clocks are easier to analyse. Indeed, even for moderately large dimensions  of the clockwork , a general dynamics can lead to internal states of the clock that do not admit a simple description.

To understand the formal definition below, it is convenient to think of random variables , for , which represent the position on the -dimensional clockwork after applications of the clock map . Imagine that the clock state can jump to any of the states of the clockwork, which we denote by , with a given probability. We can represent this using Markov chains where

Hence . This is a homogenous Markov chain, where the probability distribution does not depend on . We will now define mathematically a general stochastic reset clock.

Definition 3.

A stochastic reset clock is given by a pair , as in Def. 1, with and the map taking the form:

Note that any passage over state from a non-zero state is considered a tick, and hence after each detected tick the clock starts anew from the state . Without loss of generality one can take , and also choose any other state instead of as a tick state of the clock. Values represent a probability that clock jumps from the state to , and as mentioned above the probability distribution for a jump is the same from any state, i.e. . Importantly, and .

We can show that the above defined is a valid clock map as prescribed by Def. 1.

Lemma 1.

The map from Def. 3 is a completely positive trace preserving map.


See Appendix. ∎

One can think of the simplest stochastic clock model, which is described by a toss of a coin at every step. We will call this the stochastic ladder clock. This clock was first studied in ChrisThesis () (notice the usage of a similar clock in ThermodynamicQClock () for thermodynamical considerations, and in RPaper (), which is further discussed in the discussion section).

Definition 4.

A stochastic ladder clock is a clock defined by Def. 3 that can jump only to the next state with the jump probability and stay in the current state with the probability . Hence it is defined by:


independent of and .

We will next show that a stochastic clock can be made -continuous, for arbitrary , by choosing its probability distribution such that the total probability for a clock to move from its current state is sufficiently small.

To obtain the diamond norm needed for continuity calculation, we will use the mathematical framework of semidefinite programming, as applied to the channel distance in JohnWatrous ().

For a quantum channel , it holds that if and only if


where we take isomorphic to and is a so-called Choi-Jamiołkowski state,

In our case .

For our purpose it is enough to find a good upper bound for the channel distance, as the continuity holds with this upper bound as . We will use the fact that any dual feasible operator can be used to compute an upper bound on the optimal value of the dual problem 3.

Note that the values will determine critically the possible values of for -continuity. We will now show how exactly relates to the probability distribution of the jump of the clock.

Lemma 2.

The stochastic clock , with and of Def. 3, is -continuous iff .


See Appendix. ∎

Note that the statement of the lemma is rather intuitive. Indeed, a clock that moves from its current state with a large probability has a dynamics that does not approximate well the identity map.

Iii Performance of the stochastic clocks in the Alternate Ticks Game

As defined in ClockModel (), the Alternate Ticks (AT) Game involves two collaborating players, and , each equipped with a quantum clock as defined in Def. 1. The players can agree on a common strategy beforehand, but are not allowed to communicate once the game begins, nor to correlate their clocks prior to the start of the game. They are asked to provide ticks with their clocks in an alternating order — e.g. first from , then from , then again from , and so on. The goal of the players is to maximise the joint number of ticks respecting the posed alternate ticks condition.

We will now restrict to the case when clock starts from one of the basis states . We describe the number of jumps (applications of the map ) needed for a clock to produce a tick after the tick by a random variable . Note that all are independent, identically distributed (iid), since we consider reset clocks — after the tick they always start anew from the state and move with the same probability distribution. We will see that in the circular board picture, where the pieces move on the circle in one direction, the AT Game can be lost only if one player’s peace overtakes the other for at least positions. This is however not sufficient as the other player can catch up with this fallout. We comment on this in more details below.

We will assume that clocks can only move forward, but note that moving forward for steps is equivalent to moving backward for one step, since we can describe the dynamics on a circle. Hence we are still dealing with the most general case. To be able to analyse this further using probability theory, we will next define classical description of the stochastic clocks and the game dynamics.

Definition 5.

Let be a -dimensional stochastic clock, with , for some . We call the triple its classical description where for , and the random variable denotes the number of states for which the clock has moved forward (has jumped over) after applications of the map .

Note that the tick happens after steps. Now to quantify the success in the AT Game we need to look at the random variable describing the distance on the circular board between the players A and B. Suppose , hence the player A is in front of the player B on the board.

Definition 6.

The classical game description after applications of , , is defined by the random variable


where . We also introduce the random variables .

We now derive boundary cases for losing the game.

Lemma 3.

For the AT Game played with the stochastic clocks of dimension to be halted, it is necessary that one player is at least steps ahead of the other, i.e. or . A sufficient criterion for halting is that one of the players is steps in front of the other, i.e. or .


See Appendix. ∎

The expected number of ticks in the AT Game is hence lower bounded by the number of ticks until one player is exactly steps in front of the other, and upper bounded by the expected number of ticks until one is exactly steps in front of the other.

Assume that each clock can move up to states in one jump. Then the distance between the positions of the clocks and can change for any value between in one jump, i.e. . Note that . We are interested in the minimal number of steps before the random variable reaches one of the boundaries (one player being one or two circles in front of the other). This will lead to a higher-order differential equation, in the general case of order . We will assume player was in front of the player at the start of the game, and .

Denote with a random variable counting the number of ticks, a random variable counting number of jumps between two ticks, and with expected number of jumps until the game is lost for initial distance between the clock states . Note that and are independent random variables. Then the following holds:

where is the expected number of alternate ticks. In general, for the expected number of jumps until the end of the game (number of applications of the map ), we have:


where is the maximal number of states for which the positions of A and B can differ in one jump, and denotes the probability that the difference between positions of players and on the circle changed for exactly in one jump. We can have maximum which is the case that one clock jumps for steps and the other stays where it was.
Note that the value of will be important in determining -continuity of a clock, since the bigger possible we have, the less possibilities we have for small . In other words, the probability for the clock to move for many states in the same jump has to remain low for an -continuous clock with small .

iii.1 Identical clocks in the Alternate Ticks Game

If the two clocks are identical, the probability to change the distance between A and B for or states in one step will be the same. This means that variable changes for or for with the same probability, leading to . Note also that

Hence our recurrence relation becomes:


Solving this relation (done in details in Appendix) and inputing optimal , we obtain:


and we know that the expected number of ticks . Note that for for we have a clock described completely by the identity map, that will not produce a tick. Hence for this clock and it can produce zero expected alternate ticks. Note also that by the definition of the diamond norm . Clock with will be described in the next section.

We can then show the following Theorem.

Theorem 1.

Suppose that the AT Game is played between two identical -continuous -dimensional stochastic clocks, with . Then the expected number of alternate ticks is bounded by

where is the furthest state the clock can jump to from the state with probability , and is the probability for the clock to jump from state to .


See Appendix. ∎

We can see from the above result that for small, we have a greater linear upper bound on the number of ticks, and for approaching we have a very bad constant bound. This suggest that the ladder clock is one of the best stochastic clocks one can build, since .
To maximise lower bound one needs to be small, which again is minimised for a ladder clock (where ) with small .

iii.2 Perfect stochastic clocks

We will now introduce a clock that we will call the perfect clock. When the AT Game is played with two perfect clocks, it always produces infinite number of ticks. However, the perfect clock is not -continuous for , i.e., it is not a physical clock (see ClockModel ()).

Definition 7.

A perfect stochastic clock is a clock that always produces a tick after exactly the same number of applications of the map .

Again note that this clock is not -continuous for since , and that if two identical perfect clocks play the AT Game then . Hence from Eq. 7 the expected number of ticks is .

In the ladder clock model, this clock will always produce a tick after steps, where is the dimension of the clockwork system. Since we have taken that , the tick is produced after exactly steps. Hence for the perfect stochastic ladder clock.

In the Appendix we show that the following bunds hold if this clock was to play the AT Game with any stochastic ladder clock:


Then gives a bound on the number of alternate ticks, which will be very bad for small , as expected. If the perfect ladder clock plays against the perfect clock we have and they can play the AT Game forever.

Iv Bounds on the expected number of alternate ticks for ladder clocks

For any clockwork dimension , we will derive a tight lower and upper bound on the expected number of alternate ticks generated in the AT Game with two identical ladder clocks.

The lower bound obtained also provides us with the minimum average number of alternate ticks achievable with the best possible quantum clocks within the given mathematical framework. It is an open question whether it is possible to achieve a stronger-than-linear relationship, but current numerical results - e.g. ClockModel (); ChrisThesis () and work on different clock accuracy definitions RPaper () confirm such a superiority of well-defined quantum to any classical clocks for certain measures used.

Remember from Eq. 4, that for the ladder clock and . One can easily deduce that the possible change in distance between two players in one step takes values: , with when either both A and B stand still or both make a step, when A makes a step and B stands still and when B makes a step and A stands still.
The connection to the Gambler’s ruin problem can be seen easily ProbabilityTheory (). Consider scenario where at each round gambler wins with probability , loses with probability or has a draw with a casino with the probability .
The following result can easily be deduced from our calculations in Sec. III.

Theorem 2.

Consider the AT Game played with two identical -dimensional stochastic ladder clocks with a step probability . Assume that an optimal strategy is applied. Then the expected number of alternate ticks produced on each side is lower and upper bounded by functions asymptotically linear in the dimension of the clockwork space, given by




Note that the expected number of steps in the random walk until one of the boundaries is reached, is also the number of times the map will be applied on both sides A and B. For the ladder clock we have where are iid random variables denoting the number of applications of the map to go from position to .

Note that and hence , leading to

Now we are left with calculating . But this is also the expected number of steps until random walk is ended for variable . Again call for game starting in . Then we obtain the following recurrence relation:

with .
Absorbing boundaries are for the lower bound, and for the upper bound on the game (see Lemma 3). The general solution of this recurrence relation is

Inserting boundary conditions, and maximising over , to obtain the optimal starting conditions of the game (the corresponding z is which is as expected - it is the best strategy to start with diametrically opposite states of the two identical clocks), we obtain bounds from Eq. 9. ∎

Figure 1: Expected number of the alternate ticks of the two identical stochastic ladder clocks. The blue line represents an asymptotic lower bound and the red line an asymptotic upper bound. The orange data points are results from numerical simulations with the step parameter , averaged over iterations.

In Fig. 1 we show numerical results for the performance of the stochastic ladder clock in the AT Game. Note that the numerics confirms our derived analytical bounds.

V Discussion and Conclusions

This work is motivated by the principle that time, rather than just being an external parameter in the equations of motion, should be defined operationally as the quantity we can read off a clock. The principle entails that measures for the accuracy of clocks must not depend on an external time parameter, either. Indeed, having access to such a parameter would be akin to using a perfectly accurate clock as a reference. Conversely, the score  achievable in the AT Game, which we considered here, is defined without any reference to parametric time. Note that this operational viewpoint is also imposed on us when we talk about the accuracy of the best available clocks, e.g., atomic clocks AtomicClocks (); Wineland (); WinelandFrequencyStandards (). Since there do not exist more accurate clocks, we have no reference to test against — but we can of course still count how many ticks two such clocks emit until they run out of synchronisation.

The performance of a clock in the AT Game is sometimes difficult to determine analytically. One may thus try to approximate it by measures with more mathematical structure. One such possible measure is the so-called -value, defined as , where is the expected length of the time interval between two ticks and its standard deviation. The drawback of this measure is that it uses the parametric time explicitly. Intuitively, one may think of it as a measure for how many ticks it takes until the standard deviation in the (parametric) time of a tick is equally large as the average time interval between two ticks. This interpretation suggests that the -value of a clock can related to the AT Game score . In work simultaneous to this one RPaper (), further evidence for the close interrelation between and is provided. In particular, it has been shown that is upper bounded by a function linear in the size  for stochastic clocks and that it equals for the first tick of stochastic ladder clocks.

The precise relation between the AT Game performance  and the -value for general clocks is however unknown. Given the above considerations, a natural conjecture would be that they depend linearly on each other. This would have interesting consequences. In RPaper (), a construction of a quantum clock has been presented whose -value grows almost quadratically in its size , when . If the conjecture was true, this would imply that quantum clocks can outperform the best stochastic clocks in the AT Game.

We also note that the operational accuracy measure based on the AT Game that we employed here may be generalised in various directions. For example, one could consider a variant of the AT Game with more than two players and strengthen the condition of alternating ticks accordingly. Another possibility is to consider non-binary tick registers and demand that the emitted ticks all contain a different number. It would also be interesting to investigate scenarios that include relativistic effects, like the ones described in e.g. CaslavEsteban (); LockFuentes (). Another, possibly quite far-reaching, project would be to apply the operational approach taken here to the correlations framework of PageWootters (); Wootters (); Mott (); Briggs (); Brout (); GiovannettiQuantumTime (); ChiaraVlatko (). In particular, the clock systems employed within the latter may be replaced by finite-size clocks as considered here (see PanticMasterThesis () for some initial steps in this direction).


The authors thank Ralph Silva for insightful discussions. We acknowledge support from the Swiss National Science Foundation (SNSF) via the National Centre of Competence in Research QSIT and project No. .

Appendix A Proof of Lemma 1

The map of Def. 3 is a completely positive trace preserving map.


By Choi’s theorem ChoiCompletelyPositive (), it is enough to show that there is a Kraus representation for the map . Define:

It can easily be seen that these operators are linear operators from to . Also



Hence they represent Kraus operators and we can easily see that

is indeed a CPTP map.

Appendix B Proof of Lemma 2

The stochastic clock , with and of Def. 3, is -continuous iff .


First note that since we are considering that random variable denoting the position of a stochastic clock performs a homogenous Markov chain, we have that is a constant for all . We will now use semi-definite programming described above to obtain an upper bound on which will also determine possible values of from Def. 2.
As a first step we need to calculate Choi-Jamiołkowski state of which is, assuming to be a copy space of , . Note that


hence we have:


Now we need to find a dual feasible map such that both and are positive maps on . Let

from which it follows


Now let . Then to show and are positive we need to show that for any and correspondingly for . Calculating,

Now, notice that and the sums can be written as:

since all of the terms are non-negative. Also

Further, we can see that


Hence is a diagonal matrix with elements on the main diagonal. We can hence deduce that without loss of generality. Since represents a bound for the we see that our stochastic clock is -continuous for all . Also, given an we can choose a probability distribution for our clock jumps to be such that and we know that our clock will be -continuous by Def. 2. ∎

Appendix C Proof of Lemma 3

Let Alice and Bob play the AT Game with two identical -dimensional stochastic clocks A and B and suppose the game has ended after applications of map . Then either A or B has to be at least states ahead at moment .


Let and be the classical dynamical descriptions of the clocks and let be the classical game description. Assume that it is possible for the AT Game to end without any of the clocks being time ahead.

First, consider two special cases: 1) The game ends before B ticks for the first time: In this case, and , and therefore , i.e. A is states ahead. 2) The game ends before A ticks for the first time: Here, and , and therefore , i.e. B is states ahead.

Next, assume that each clock has ticked at least once. Let be the times at which clocks A and B produce their last alternate tick, respectively. Now, if A produces the final (non-alternate) tick that ends the game at moment , then and . Remind yourself that a clock generates its th tick at the moment corresponding to the smallest for which . Since A produced the first tick by convention and the last tick by assumption, we know that and for some alternate ticks. Solving one of the equations for and plugging it into the other one yields: and thus . But by definition, this means that A is states ahead.

Similarly, if B produces the final tick that ends the game, then and . But following an analogous argument as above, we find , so that and B is at least states ahead. ∎

Let Alice and Bob play the AT Game with identical -dimensional stochastic clocks A and B of dimension and suppose that one of the clocks is times ahead (at least steps ahead) at some moment . Then there exists , for which the Alternate Ticks Game has ended.


Let again and be the classical dynamical descriptions of the clocks and let be their classical game description. Notice that for a given classical dynamical description for a stochastic clock, for any moment , we have seen that the number of alternate ticks is given by .

Now, assume first, that A is times ahead at moment . Then , i.e. . From the above equation, it follows that A has produced at least two more ticks than B. But by the pigeon hole principle, this immediately implies that at least two ticks of A must have occurred non-alternately, i.e. without B ticking in between. Therefore, the game must have ended at some earlier moment .

Similarly, notice that if B is times ahead at some moment , it holds that , so that , i.e. B ticked more often than A. By definition, A must have produced the first tick (otherwise the game has already ended and we are done). But that again means that B must have ticked times more than A after the first alternate tick. By the pigeon hole principle two ticks by B must have violated the alternating order and the game ended at some . ∎

Appendix D Proof of Theorem 1

Assume that the AT Game is played between two identical stochastic clocks. Then following bounds hold on the number of alternate ticks:


We can consider homogenous equation from Eq. 6 (which excludes the constant term on the RHS). One can notice that will be the solution. Namely inserting to the homogenous part of Eq. 6, we obtain:


Note that this is the case because of the symmetry of the particular problem. Hence we are left to find a particular solution. After considering a quadratic function in , we obtain following solution:

Hence the total solution is .
We can now impose boundary conditions (recall: for the lower bound, and for the upper bound on the game). For the lower bound we have


This leads to


For the upper bound we obtain




Now recall that , where is the number of ticks and for initial distance between clock states . We will have maximised for as expected for identical clocks (they start from opposite states on the circle). Note that is not trivial to calculate as it depends on the probability distribution of the particular clock.
Inputing , we have:


Now write . We can restrict to the case when clock can not jump more than places in one step. This is the same as the maximum number of place differences players can achieve in one step. Note also that the average number of steps each clock needs until the tick is reached is then lower bounded by , . Hence, expected number of ticks can be upper bounded as follows (note that by assumption):


using , , and . Note that is a constant for any and same for both clocks. We can see from the above result that for small, we have a better linear bound on the number of ticks, and for approaching we have a very bad constant bound. This suggest that the ‘ladder’ clock is one of the best stochastic clocks one can build.

Note also that the average number of steps until the tick of one clock, is upper bounded by , where is also a constant in . Hence we have: