The last part of this lecture will take place on Monday, May 6 at 3 PM in Bendheim Classroom 103. The full scribe notes for this lecture will be posted sometime after that date.
The next two lectures by Rene Carmona will be on games on random graphs.
Many thanks to Patrick Rebeschini for scribing these lectures!
In the following we discuss some results from the paper “Connectivity and equilibrium in random games” by Daskalakis, Dimakis, and Mossel. We define a random game on a random graph and we characterize the graphs that are likely to exhibit Nash equilibria for this game. We show that if the random graph is drawn from the Erdös-Rényi distribution, then in the high connectivity regime the law of the number of pure Nash equilibria converges toward a Poisson distribution, asymptotically, as the size of the graph is increased.
Let be a simple (that is, undirected and with no self-edges) graph, and for each denote by the set of neighbors of , that is, . We think of each vertex in as a player in the game that we are about to introduce. At the same time, we think of each edge as a strategic interaction between players and .
Definition (Game on a graph). For each let represent the set of strategies for player , assumed to be a finite set. We naturally extend this definition to include families of players: for each , let be the set of strategies for each player in . For each , denote by the reward function for player . A game is a collection .
The above definition describes a game that is static, in the sense that the game is played only once, and local, in the sense that the reward function of each player depends only on its own strategy and on the strategy of the players in its neighbors. We now introduce the notion of pure Nash equilibrium.
Definition (Pure Nash equilibrium). We say that is a pure Nash equilibrium (PNE) if for each we have
A pure Nash equilibrium represents a state where no player can be better off by changing his own strategy if he is the only one who is allowed to do so. In order to investigate the existence of a pure Nash equilibrium it suffices to study the best response function defined below.
Definition (Best response function). Given a reward function for player , we define the best response function for as
Clearly, is a pure Nash equilibrium if and only if for each . We now define the type of random games that we will be interested in; in order to do so, we need to specify the set of strategies and the reward function for each player.
Definition (Random game on a fixed graph). For a graph and an atomless probability measure on , let be the associated random game defined as follows:
- for each ;
- is a collection of independent identically distributed random variables with distribution .
Remark. For each game the family is a collection of independent random variables that are uniformly distributed in , and for each , we have almost surely. In fact, note that if and only if and this event has probability since the two random variables appearing on both sides of the inequality sign are independent with the same law and is atomless. As far as the analysis of the existence of pure Nash equilibria is concerned, we could take the present notion of best response functions as the definition of our random game on a fix graph. In fact, note that the choice of in does not play a role in our analysis, and we would obtain the same results by choosing different (atomless) distributions for sampling (independently) the reward function of each player.
Denote by the distribution of a Erdös-Rényi random graph with vertices where each edge is present independently with probability . We now introduce the notion of a random game on a random graph.
Definition (Random game on a ramon graph). For each , and each probability measure on , do the following:
- choose a graph from ;
- choose a random game from for the graph .
Henceforth, given a random variable let represent its distribution. Given two measures and on a measurable space, define the total variation distance between and as
where the supremum is taken over measurable functions such that the supremum norm is less than or equal to .
We are now ready to state the main theorem that we will prove in the following (Theorem 1.9 in Daskalakis, Dimakis, and Mossel).
Theorem 1 (High connectivity regime). Let be the number of pure Nash equilibria in the random game on random graph defined above. Let define the high-connectivity regime as
where satisfies the following two properties:
Then, we have
where denotes the conditional probability given the graph and is a Poisson random variable with mean . In particular,
which shows that in this regime a pure Nash equilibrium exists with probability converging to as the size of the network increases.
Remark. Using the terminology of statistical mechanics, the first result in Theorem 1 represents a quenched–type result since it involves the conditional distribution of a system (i.e., the game) given its environment (i.e., the graph). On the other hand, the second result represents an annealed–type result, where the unconditional probability is considered.
In order to prove Theorem 1 we need the following lemma on Poisson approximations. The lemma is adapted from the results of R. Arratia, L. Goldstein, and L. Gordon (“Two moments suffice for Poisson approximations: the Chen-Stein method”, Ann. Probab. 17, 9–25, 1989) and it shows how the total variation distance between the law of a sum of Bernoulli random variables and a Poisson distribution can be bounded by the first and second moments of the Bernoulli random variables. This result is a particular instance of the Stein’s method in probability theory.
Lemma (Arratia, Goldstein, and Gordon, 1989). Let be a collection of Bernoulli random variables with . For each let be such that is independent of . Define
where . Define and . If is a Poisson random variable with mean , then
Proof. We define the following operators that act on each function :
We point out that characterizes in the sense that if and only if is a Poisson random variable with mean ; is an example of Stein’s operator. First of all, we show that for each we have . In fact, if we have
and if we have
For each define and . The following properties hold:
In what follows, consider any given function such that . Define the function as for each , and let . From what was seen above we have and we get
The first term is bounded above by while the third term is equal to since is independent of . In order to bound the second term we want to rewrite each term as a telescoping sum. In what follow fix , label the elements of as and define
Noticing that , we have
and we get
Therefore, combining all together we get
To be continued…
The past three lectures were devoted to the giant component theorem:
Theorem Let be the connected component of that contains .
- If , then in probability.
- If , then in probability, for some .
- If , then in distribution.
We proved only the first (subcritical) and second (supercritical) cases: our presentation was largely inspired by the treatment of Janson, Luczak, and Rucinski and Durrett. We have omitted the critical case, however, as the last two lectures of the semester will be on another topic. The goal of this post is to provide some final remarks and references on the giant component theorem.
At first sight, the “double jump” in the giant component theorem looks quite shocking. In hindsight, however, this does not seem quite so miraculous, as it mirrors an elementary phenomenon that is covered in many introductory probability courses: given a (nice) random walk with initial condition , define the hitting time for some . Then there are three cases:
- If has negative drift, then . In fact, the random variable has a light (exponential) tail.
- If has positive drift, then .
- If has zero drift, then a.s. but . That is, the random variable has a heavy tail.
This “double jump” in the behavior of the hitting probabilities of a random walk is directly analogous to the behavior of the connected components of an Erdös-Rényi graph, and this was indeed the basic idea behind the proofs given in the previous lectures. Of course, it remains a bit of a miracle that the random walk approximation of the exploration process, which only holds for small times, is sufficiently powerful that it describes so completely the behavior of the random graph.
The critical case
In the subcritical case, the size of the largest component is of order because the hitting time of a random walk with negative drift has an exponential tail: that is, we proved
which goes to zero as for .
Similarly, we would expect that we can obtain the size of the largest component in the critical case if we understand the heavy tail behavior of the hitting time of a random walk with zero drift. This is in fact the case. Indeed, when there is zero drift, one can show that
The crude union bound argument used above now does not give the correct answer, but an only slightly better argument is needed. Indeed, note that
It turns out that in the critical case is not only bounded in probability, but in fact converges weakly to some limiting distribution. This distribution, and much more, is beautifully described by Aldous in terms of Brownian excursions. This is an interesting example of the application of stochastic analysis to discrete probability; unfortunately, we do not have the time to cover it.
In a different direction, it turns out that various additional phase transitions appear when we consider a finer scaling, for example, in the “critical window” . For an overview of the various transitions, see, for example, section 11.1 in Alon and Spencer.
Rather than considering the size of the largest component, one could ask when the entire Erdös-Rényi graph is connected. Note that when , the constant in the size of the giant component is always strictly positive, so the graph is not connected. Therefore, in order for the entire graph to be connected, we must let (that is, the edge probability must be superlinear). It turns out that the appropriate scaling for this question is , and another phase transition arises here.
Theorem. Let . If , then the Erdös-Rényi graph is connected with probability tending to as . If , the graph is connected with probability tending to as .
To get some intuition, consider the probability that a vertex is isolated (that is, disconnected from every other vertex):
Thus for , we have
In particular, if , then there must exist an isolated vertex with positive probability as , in which case the graph is not connected (in fact, it is not hard to show that the variance of the number of isolated components is of the same order as its mean, so that the probability that the graph is connected tends to zero). Somewhat miraculously, it turns out that when there are no isolated vertices, then the graph must already be connected, so that we do indeed obtain the sharp transition described in the Theorem above. For a proof of this fact (by a clever combinatorial argument) see, for example, the lecture notes by van der Hofstad. Alternatively, one can use a random walk argument entirely in the spirit of the proofs in the previous lectures to prove that the random graph is connected for : by running simultaneous exploration processes from different vertices as we did in the proof of the supercritical case, one can show that all connected components must intersect when and thus the entire graph must be connected. See section 2.8 in Durrett for such an argument.
Let us begin with a brief recap from the previous lecture. We consider the Erdös-Rényi random graph in the supercritical case . Recall that denotes the connected component of the graph that contains the vertex . Our goal is to prove the existence of the giant component with size , while the remaining components have size .
Fix sufficiently large (to be chosen in the proof), and define the set
of vertices contained in “large” components. The proof consists of two parts:
- Part 1:
- Part 2: in probability.
Part 1 states that all the sufficiently large components must intersect, forming the giant component. Part 2 counts the number of vertices in the giant component. Part 2 was proved in the previous lecture. The goal of this lecture is to prove Part 1, which completes the proof of the giant component.
As in the previous lectures, the central idea in the study of the giant component is the exploration process , where
We have seen that , where is a random walk with increments
When , we have . Thus is approximately a random walk with positive drift. The intuitive idea behind the proof of Part 1 is as follows. Initially, the random walk can hit rapidly, in which case the component is small. However, if the random walk drifts away from zero, then with high probability it will never hit zero, in which case the component must keep growing until the random walk approximation is no longer accurate. Thus there do not exist any components of intermediate size: each component is either very small () or very large (we will show , but the precise exponent is not important).
We now want to argue that any pair of large components must necessarily intersect. Consider two disjoint sets and of vertices of size . As each edge is present in the graph with probability , the probability that there is no edge between and is
We therefore expect that any pair of large components must intersect with high probability. The problem with this argument is that we assumed that the sets and are nonrandom, while the random sets themselves depend on the edge structure of the random graph (so the events and are highly correlated). To actually implement this idea, we therefore need a little bit more sophisticated approach.
To make the proof work, we revisit more carefully our earlier random walk argument. The process has positive drift as . Thus the process is still approximately a random walk with positive drift! Applying the above intuition, either dies rapidly (the component is small), or grows linearly in as is illustrated in the following figure:
This means that the exploration process for a component of size will not only grow large () with high probability, but that the exploration process will also possess a large number of active vertices (. To prove that all large components intersect, we will run different exploration processes simultaneously starting from different vertices. We will show that if two of these processes reach a large number of active vertices then there must be an edge between them with high probability, and thus the corresponding components must coincide. This resolves the dependence problem in our naive argument, as the edges between the sets of active vertices have not yet been explored and are therefore independent of the history of the exploration process.
The component size dichotomy
We now begin the proof in earnest. We will first show the dichotomy between large and small components: either the component size is , or the number of active vertices grows linearly up to time . To be precise, we consider the following event:
Our goal is to show that is large.
Define the stopping time
We can write
Now suppose and . Then , as exploration process is alive at time and stays alive until time . We can therefore write
To bound the probabilities inside the sum, we compare to a suitable random walk.
The random walk argument
To bound the probability that , we must introduce a comparison random walk that lies beneath . We use the same construction as was used in the previous lecture. Let
where , are i.i.d. random variables independent of , (the same used in the exploration process), and is the set of the first components of (if , then and thus is undefined; then we simply add variables ).
As in the previous lecture, we have:
- is a random walk with increments.
- whenever and .
Now suppose that and . Then
We therefore obtain for
Thus computing reduces to compute the tail probability of a random walk (or, in less fancy terms, a sum of i.i.d. random variables). That is something we know how to do.
Lemma (Chernoff bound). Let . Then
Proof. Let . Then
The result follows by optimizing over .
Note that . We therefore have by the Chernoff bound
for all (here depends only on and ). In particular, we have
provided is sufficiently large. Thus we can estimate
which goes to zero as provided that is chosen sufficiently large. In particular, the component size dichotomy follows: choosing any , we obtain
Remark: Unlike in the proof of Part 2 in the previous lecture, here we do need to choose sufficiently large for the proof to work. If is too small, then the random walk cannot move sufficiently far away from zero to ensure that it will never return. In particular, even in the supercritical case, the second largest component has size of order .
Large components must intersect
To complete the proof, it remains to show that all large components must intersect. To do this, we will run several exploration processes at once starting from different vertices. If the sets of active vertices of two of these processes grow large, then there must be an edge between them with high probability, and thus the corresponding components intersect. Let us make this argument precise.
In the following, we denote by the exploration process started at . For each such process, we define the corresponding set that we have investigated above:
We have shown above that, provided , we have
We can therefore estimate
Now note that by time , the exploration process has only explored edges where (or ), and similarly for . It follows that
In particular, if are disjoint subsets of vertices, then
On the other hand, implies that must be disjoint at every time . Thus if , there can be no edges between vertices in and at any time (if such an edge exists, then the vertices connected by this edge will eventually be explored by both exploration processes, and then the sets of removed vertices will no longer be disjoint). Therefore,
Thus we finally obtain
and the proof of the giant component theorem is complete.
Many thanks to Quentin Berthet for scribing this lecture!
Consider the Erdös-Rényi graph model , and denote as usual by the connected component of the graph that contains the vertex . In the last lecture, we focused mostly on the subcritical case , where we showed that . Today we will begin developing the supercritical case , where for a suitable constant . In particular, our aim for this and next lecture is to prove the following theorem.
Theorem. Let . Then
where is the smallest positive solution of the equation . Moreover, there is a such that all but one of the components have size with probability tending to as .
Beginning of the proof. Define the set
The proof of the Theorem consists of two main parts:
- Part 1: .
- Part 2: in probability.
Part 1 states that all “large” components of the graph must intersect, forming one giant component. Some intuition for why this is the case was given at the end of the previous lecture. Part 2 computes the size of this giant component. In this lecture, we will concentrate on proving Part 2, and we will find out where the mysterious constant comes from. In the next lecture, we will prove Part 1, and we will develop a detailed understanding of why all large components must intersect.
Before we proceed, let us complete the proof of the Theorem assuming Parts 1 and 2 have been proved. First, note that with probability tending to one, the set is itself a connected component. Indeed, if and then must lie in disjoint connected components by the definition of . On the other hand, with probability tending to one, all must lie in the same connected component by Part 1. Therefore, with probability tending to one, the set forms a single connected component of the graph. By Part 2, the size of this component is , while by the definition of , all other components have size . This completes the proof.
The remainder of this lecture is devoted to proving Part 2 above. We will first prove that the claim holds on average, and then prove concentration around the average. More precisely, we will show:
Together, these two claims evidently prove Part 2.
Mean size of the giant component
We begin by writing out the mean size of the giant component:
where we note that does not depend on the vertex by the symmetry of the Erdös-Rényi model. Therefore, to prove convergence of the mean size of the giant component, it suffices to prove that
This is what we will now set out to accomplish.
In the previous lecture we defined exploration process . We showed that
and that for
where is an arbitrary nonanticipating choice, say, (recall that denotes the adjacency matrix of the random graph). As are i.i.d. and as edges emanating from the set of unexplored vertices have not yet appeared in previous steps, the process is “almost” a random walk: it fails to be a random walk as we only add Bernoulli variables in each iteration, rather than a constant number. In the last lecture, we noted that we can estimate from above by a genuine random walk by adding some fictitious vertices. To be precise, we define
where are i.i.d. independent of the (if , then and thus is undefined; in this case, we simply add all variables ). In the present lecture, we also need to bound from below. To this end, we introduce another process as follows:
where is the set consisting of the first elements of in increasing order of the vertices (if , we add variables ). The idea behind these processes is that is engineered, by including “fictitious” vertices, to always add i.i.d. Bernoulli variables in every iteration, while is engineered, by including “fictitious” vertices when is small and omitting vertices when is large, to always add i.i.d. Bernoulli variables in every iteration. The following facts are immediate:
- is a random walk with i.i.d. increments.
- is a random walk with i.i.d. increments.
- for all .
- for all on the event .
To see the last property, note that the exploration process can only explore as many vertices as are present in the connected component , so that for all ; therefore, in this situation only the second possibility in the definition of occurs, and it is obvious by construction that then (nonetheless, the first possibility in the definition must be included to ensure that is a random walk).
We now define the hitting times
Then we evidently have
(Note how we cleverly chose the random walk precisely so that whenever ). We have therefore reduced the problem of computing to computing the hitting probabilities of random walks. Now we are in business, as this is something we know how to do using martingales!
The hitting time computation
Let us take a moment to gather some intuition. The random walks and have increments distributed as and , respectively. As , both increment distributions converge to a distribution, so we expect that where is the first hitting time of the Poisson random walk. On the other hand, as , we expect that . The problem then reduces to computing the probability that a Poisson random walk ever hits the origin. This computation can be done explicitly, and this is precisely where the mysterious constant comes from!
We now proceed to make this intuition precise. First, we show that the probability can indeed be replaced by , as one might expect.
Lemma. as .
Proof. We need to show that
Note that as when ,
We can evidently write
Choosing , we obtain for . Therefore,
This completes the proof.
By the above Lemma, and a trivial upper bound, we obtain
To complete computation of the mean size of the giant component, it therefore remains to show that and converge to . In fact, we can compute these quantities exactly.
Lemma. Let . Then
where is the smallest positive solution of .
Proof. Recall the martingale used in last lecture:
Suppose that and . Then
The first equality holds since if then and , while if then and . The second equality holds by dominated convergence since , and the third equality is by the optional stopping theorem.
Now suppose we can find such that as . Then we have
by dominated convergence. Thus, evidently, it suffices to find with the requisite properties. Now note that as , , and for , we evidently must have
We can find such by inspecting the following illustration:
Evidently the requisite assumptions are satisfied when is the smallest root of the equation (but not for the larger root at !)
Remark. Note that the supercritical case is essential here. If then the equation for has no solutions , and the argument in the proof does not work. In fact, when , we have .
By an immediate adaptation of the proof of the previous lemma, we obtain
where is the smallest positive solution of . Letting , we see that
where is the smallest solution of the equation (which is precisely the probability that the Poisson random walk hits zero, by the identical proof to the lemma above). We have therefore proved
Variance of the giant component size
To complete the proof of Part 2 of the giant component theorem, it remains to show that
To this end, let us consider
To estimate the terms in this sum, we condition on one of the components:
To proceed, note that the event can be written as
In particular, the event is independent of the edges for . Therefore, for , the conditional law of given coincides with the (unconditional) law of , the conncted component containing in the induced subgraph on the vertices :
As this quantity only depends on by the symmetry of the Erdös-Rényi model, we can evidently write
for , . In particular, we obtain
Now note that, by its definition, is distributed precisely as the component containing vertex in the random graph model. We can therefore show, repeating exactly the proof of the mean size of the giant component above, that
We have therefore shown that
which evidently implies
This is what we set out to prove.
Remark. It should be noted that the proof of Part 2 did not depend on the value of , or even on the rate, in the definition of the set : any sequence that grows sublinearly to infinity would have given the same result. This suggests that all but a vanishing fraction of vertices are contained in connected components of order or . We find out only in the next lecture why the rate (for sufficiently large!) is important: only sufficiently large connected components are guaranteed to intersect, while there might (and do) exist components of order that are disjoint from the giant component. If we do not exclude the latter, we will not be able to prove Part 1.
Many thanks to Weichen Wang for scribing this lecture!
Consider the Erdös-Rényi graph model . In previous lectures, we focused on the “high complexity regime”, i.e., as goes to infinity, is fixed. We discussed topics such as clique numbers and chromatic numbers. From now on, we shall consider the “low complexity regime”, where as goes to infinity, for a fixed constant . As before, let be the adjacency matrix of . Then are i.i.d. Bernoulli random variables with success probability .
Theorem 1 Let be the connected component of that contains .
- If , then in probability.
- If , then in probability, for some .
- If , then in distribution.
In the following lectures, we will aim to prove at least parts 1 and 2.
The exploration process
How to study ? We will explore by starting an “exploration process” at that moves around until all its sites have been visited. This walk will be constructed so that it hits each site once. So, the time it takes to explore all of is exactly . As a consequence, studying reduces to studying a hitting time of a certain random walk, and to the latter we can apply martingale theory.
At each time , we maintain three sets of vertices:
Below is an illustration of how these sets are updated on a simple example.
- At , initialize , and . Namely, only is active, all the vertices other than are unexplored, and no vertices have been removed.
- At , update , and . Namely, all neighbors of are moved from the unexplored set to the active set, and itself is removed.
- At , pick some and update , and . Namely, all unexplored neighbors of are moved into the active set, and itself is removed.
- At time , we pick some vertex from the current active set , activate all unexplored neighbors of and remove itself.
This is a sort of local search along the connected component : much like playing a game of Minesweeper! At each , the choice of can be made arbitrarily (e.g., selecting the vertex with the smallest index or randomly selecting a vertex in ). The only requirement is that it is nonanticipating (only depending on the edges visited up to time ). For example, we cannot pick the vertex in which has the largest number of unexplored neighbors, as this choice relies on unexplored edges.
A formal description of the “exploration process”:
- Initialize , and .
- For , we set
where is a nonanticipating but otherwise arbitrary choice.
This process stops when there are no more active vertices. It hits each vertex in once and only once. At each time , we remove one vertex in . So the stopping time is exactly equal to the size of :
So, we only need to study the stopping time .
Recall that indicates whether there is an edge between vertices and , and . By construction,
Now, let’s do a thought experiment (wrong, but intuitive). Let’s forget for the moment that some sites were previously visited, and assume that in each step all neighbors of are unvisited still (note that when is really large and is relatively small, this assumption makes sense). Then is the sum of independent ) variables, which has a distribution. This binomial variable is independent of the past because it only depends on unexplored edges; in addition, its distribution does not depend on . Therefore, would be a random walk with increment distribution . Then, studying boils down to studying first time a Poisson random walk hits zero! Of course, we cannot really ignore previously visited sites, but this rough intuition nonetheless captures the right idea as and will serve as a guiding principle for the proof.
A comparison random walk
The reason that is not a random walk is that there are only edges (not ) to explore at time . We can artificially create a random walk by adding “fictitious” points at each time as follows.
Let be i.i.d. for , , which are independent of . Define
(When , then and thus is undefined; in this case, we simply add all variables .)
Note that is the sum of edges from to . Since we have not explored yet, those edges are independent of all edges explored up to time (here we use that is nonanticipating). We therefore see that is indeed a random walk with increment
Moreover, since all are nonnegative,
as long as . It follows that is dominated by the genuine random walk , that is,
We can now obtain bounds on by analyzing hitting times of the random walk .
The subcritical case
Define the first time the comparison walk hits zero as
Since for , it is obvious that
Now we study . The intuition is that as , is a random walk with negative drift in the subcritical case . Thus , and in fact the hitting time has nice tails!
Lemma 2 Let and . Then for any positive integer ,
We will prove this lemma below. Using the lemma, we immediately obtain:
Corollary 3 If , then for any
Proof. Applying the Lemma 2 and the union bound,
This corollary proves part 1 of Theorem 1. In fact, it turns out that the constant is tight: by using the second moment method, one can prove a matching lower bound on (see, for example, the lecture notes by van der Hofstad), which implies that in fact in probability. The proof is not much more difficult, but we prefer to move on to the supercritical case.
Remark. It might seem somewhat surprising that the result we obtain is so sharp, considering that we have blindly replaced by the larger quantity . However, in going from to we do not lose as much as one might think at first sight. When is large and is relatively small, the excess term in the definition of is zero with high probability, as most vertices are unexplored and the Bernoulli success probability of the is very small. With a bit of work, one can show that and will actually stick together for times with probability going to one as . Thus, in the subcritical case where the random walk only lives for time steps, nothing is lost in going from to , and our rough intuition that should behave like a random walk as is vindicated.
To wrap up the subcritical case, it remains to prove the lemma.
Proof of Lemma 2. By the Markov inequality,
It remains to bound , which is a standard exercise in martingale theory.
where are i.i.d. Define the moment generating function , and let
Since and is independent of ,
where we have used . So is a martingale.
In the case and ,
The inequality is by Fatou’s lemma and the second equality is by the optional stopping theorem. To see the first equality, note that if , then and as , while if , then for all and . Thus .
Next, we compute . Recall that . It has the same distribution as the sum of i.i.d. variables. For , we have . Therefore,
where the last inequality is because for any . Now, by setting , we obtain that . Thus we have shown .
The supercritical case
The goal of the following lectures is to prove part 2 of Theorem 1. More precisely, we will prove:
Theorem 4 Let . Then
in probability, where is the smallest positive solution of the equation . Moreover, there is such that all but one of the components have size , with probability tending to as .
This theorem says that with probability tending to , there is a unique giant component whose size is , and all other components are small with size .
Here we provide some vague intuition for this theorem. When , the random walk satisfies , i.e., has positive drift. Then ! In fact, the further away it starts from , the smaller the probability it will ever hit . Consider the two situations:
- dies quickly: this implies that the component is small.
- lives long: then it must live very long, as once it gets far away from , the probability of returning is very small. This implies that the component must be very large (if we pretend that ).
Of course, is not (obviously eventually hits ). But the intuition explains that there cannot be components of intermediate size: given any vertex , either is small (), or it must get very large (, say). In fact, we will find that all components of size must grow all the way to . However, any pair of large components must intersect with high probability, as there are many potential edges between them! Therefore, all vertices with should be in the same giant component. We then show that the number of such vertices is with high probability.
Many thanks to Tracy Ke for scribing this lecture!
Just a reminder that next week (March 21) is Spring Break, while the week after (March 28) there will be no lecture due to the ORFE/PACM colloquium of Elchanan Mossel.
The next Stochastic Analysis Seminar lecture will be on April 4. We will start fresh with a new topic: the study of the giant component of an Erdös-Rényi graph.
Let be set of integers that represent colors. A vertex coloring of a graph is an assignment of a color to each vertex . Furthermore a vertex coloring is said to be proper if for all . The chromatic number of a graph is the smallest number of colors needed for a proper vertex coloring to exist. In this lecture, any coloring is a proper vertex coloring. All logs are in base .
Theorem [Bollobas, 1988]
The chromatic number of a random graph satisfies
1. Basic properties
In this section, we begin by reviewing some basic properties of the chromatic number, and in particular how it relates to independent sets. Recall that an independent set of a graph is a set of vertices such that . Independent sets are sometimes called stable sets. Denote by the complement graph of where iff . If is an independent set of , then it is a clique in . The largest independent set in is called independence number of and denoted by .
Proposition For any graph with independence number , clique number and chromatic number the following holds
2. Chromatic, clique and independence numbers
Our goal is to study the chromatic number of a random graph . It actually builds upon the clique number that we studied during last lecture. Indeed, we will use the following observation: if then so does the complement graph of . It implies that the independence number has the same distribution as the clique number . We know from last lecture that . Therefore, it follows from the above proposition that
Our main theorem suggests that this simple bound is, in fact, tight. Proving this requires a stronger lower bound on clique of a random graph.
Define and let be a subset of vertices and observe that induced subgraph restricted to vertices in has distribution .
That is: every vertex subgraph contains an independent set of size .
Consider now the following coloring procedure to produce a proper coloring. Pull out independent sets of size one by one and give each a distinct color. According to the definition of , as long as there are at least vertices, this is possible. If there are less than vertices left, give each a distinct color.
The above algorithm gives one possible way of coloring graph and thus the output number is an upper bound on the chromatic number . Let us now compute this upper bound. By definition of , we have
Therefore, we need to prove a bound on , uniformly in . This can be done using concentration properties of a suitable martingale.
3. Azuma-Hoeffding inequality
Martingales have useful concentration properties. Specifically the following lemma holds.
Lemma [Azuma-Hoeffding inequality.]
Let be a filtered space and let be a random variable on . Assume that the martingale is such that for all ,
Then for any positive integer and any , it holds,
Proof: We assume the following inequality due to Hoeffding. For any random variable such that a.s. and any , it holds
Now, using a Chernoff bound, we get for any ,
where . The above two displays yield that
The second part of the proof follows by applying the same argument to the martingale .
Consider the lexicographic ordering of and let be iid Bernoulli random variables with parameter indicating the presence of an edge in a graph . Define the –algebra . We are going to apply the Azuma-Hoeffding inequality to the (Doob) martingale where is maximal number of edge-disjoint –cliques in .
Note first that a.s., since adding/removing one edge can add/remove at most one edge disjoint –clique. Moreover, this inequality would not hold if we had chosen to be the number cliques of size (not necessarily disjoint). Indeed, adding or removing an edge can create or destroy many overlapping cliques.
It follows that,
It remains to show that is sufficiently large. Note first that , where is is the number of –cliques that do not share an edge with any other –clique of the graph.
4. A strong lower bound on the clique number
Fix positive integers and
and let denote the number of cliques in that do not share an edge with any other –clique of the graph. Then
for all . Here the asymptotic notation notations are as .
Proof: Define (for large enough) for some to be chosen later.
Moreover, note that for large enough,
so that where is the number of cliques in that do not share an edge with any other –clique of the graph . Let .
For any define the indicator:
Moreover for any set , let denote the number of –cliques in , other than itself, that share at least two vertices with . Observe that
We bound as follows
The following bound holds for all ,
Moreover, for , , it holds
To conclude the proof, observe that by Stirling, since ,
Let and observe that
We can therefore apply the previous proposition together with~(2), to get
5. Proof of the main theorem
we get for ,
Thus . Together with~(1), it yields
Which completes the proof of our theorem.
Lecture and scribing by Philippe Rigollet
In this lecture all logs are in base . We will prove the following.
Theorem For the centered and normalized clique number
That is, as , the clique number of the Erdös-Rényi graph is .
Proof: The proof is divided into two parts. First, we show that the clique number cannot be too big using a union bound. Then we show that the clique number cannot be too small using the second moment method. In the following, denotes an Erdös-Rényi graph .
For the first part one has
Thus, choosing , we obtain
for every , where we used that for large .
For the second part it is useful to introduce some notation. Define
In particular, iff . Thus we want to show that for one has . Using the trivial observation that implies , we get
where we have used Markov’s inequality. Note that by linearity of the expectation, . Furthermore, we can write
As are boolean random variables we have and thus
which tends to for (see the first part of the proof and use the inequality ). Thus it remains to show that the following quantity tends to :
First note that, by the independence of the edges, for with we have that and are independent, so that in the numerator of the above quantity one can restrict to with . Now by an elementary reasoning we have (with being an arbitrary subset of vertices)
Clearly one has
which shows that (1) can be rewritten as
Now note that since
Using one obtains that (2) is bounded from above by
As is a convex function and as , one has . Thus for large enough the exponent in the above display is bounded from above by , and for this latter is bounded by . Thus we proved that (2) is bounded from above by
which tends to as tends to infinity, concluding the proof.
Welcome to the stochastic analysis seminar blog! We are experimenting with this blog for the first time in the Spring 2013 semester. The intention is to post notes from the lectures here: we are grateful to several graduate students who have graciously volunteered to serve as scribes. In addition, any announcements or organizational matters will be posted to this blog. Information on previous semesters can be found here.
Time change: In order to avoid conflicts with a number of seminars, the stochastic analysis seminar will be held on Thursdays, 4:50–6:20, Bendheim Center 103 starting this week. That is, we start and end 20 minutes later than originally announced for the remainder of this semester.