Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs
|
|
- Norman Reeves
- 5 years ago
- Views:
Transcription
1 Acta Mathematica Sinica, English Series Oct., 016, Vol. 3, No. 10, pp Published online: September 15, 016 DOI: /s Acta Mathematica Sinica, English Series Springer-Verlag Berlin Heidelberg & The Editorial Office of AMS 016 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs Yu Tao MA School of Mathematical Sciences & Lab. Math. Com. Sys., Beijing Normal University, Beijing , P.R.China mayt@bnu.edu.cn Ran WANG School of Mathematics and Statistics, Wuhan University, Wuhan 43007, P. R. China and School of Mathematical Sciences, University of Science and Technology of China, Hefei 3006, P.R.China wangran@ustc.edu.cn Li Ming WU Institute of Applied Math., Chinese Academy of Sciences, Beijing , P. R. China and Laboratoire de Math. CNRS-UMR 660, Université Blaise Pascal, Aubière, France Li-Ming.Wu@math.univ-bpclermont.fr Abstract In this paper, we study some functional inequalities (such as Poincaré inequality, logarithmic Sobolev inequality, generalized Cheeger isoperimetric inequality, transportation-information inequality and transportation-entropy inequality) for reversible nearest-neighbor Markov processes on connected finite graphs by means of (random) path method. We provide estimates of the involved constants. Keywords Graph, log-sobolev inequality, isoperimetry, transport inequality MR(010) Subject Classification 60E15, 05C81, 39B7 1 Introduction Let G =(V,E) be a finite connected graph with vertex set V andorientededgessete, which is a symmetric subset of V \{(x, x) :x V }. If (x, y) E, wecallthatx, y are adjacent, denoted by x y. For any x V and any function f : V R, consider the operator Lf(x) = q(x, y)(f(y) f(x)), (1.1) y V where q(x, y) is the jump rate from x to y, which is non-negative and q(x, y) > 0 if and only if x y. Received May 18, 015, accepted April 6, 016 Supported by NSFC (Grant Nos , , and ) and 985 Projects and the Fundamental Research Funds for the Central Universities
2 1 Ma Y. T. et al. Let (X t ) be the Markov process generated by L, defined on (Ω, (F t ) t 0, (P x ) x V ). We always assume the reversibility condition, i.e., there is some probability measure μ satisfying the detailed balance condition: Q(x, y) :=μ(x)q(x, y) =μ(y)q(y, x), (x, y) E. (1.) Equivalently, the operator L is self-adjoint on L (μ), that is, f, Lg μ = Lf,g μ = 1 (f(x) f(y)) (g(x) g(y)) Q(x, y) x,y = 1 D e fd e gq(e) =:E(f,g), where D e f := f(y) f(x) fore =(x, y) E. When q(x, y) =1/d x with d x the degree of x (the number of neighbors y x), L becomes the Laplacian Δ on the graph. In that case μ(x) =d x / E and Q(e) =1/ E. Define the variance of f with respect to (w.r.t. for short) μ Var μ (f) :=μ((f μ(f)) ), and the entropy of f w.r.t. μ Ent μ (f ):=μ(f log f ) μ(f )logμ(f ). We say that μ satisfies a Poincaré inequality if there exists a constant λ>0 such that for all f L (μ), Var μ (f) λe(f,f), (1.3) μ satisfies a log-sobolev inequality if there exists a constant α>0 such that for all f L (μ), Ent μ (f ) αe(f,f). (1.4) The optimal constants λ and α in (1.3) and (1.4) are called respectively the Poincaré constant and the log-sobolev constant of μ, which are denoted by c P and c LS respectively. It is well known that c P c LS, see [5]. The Poincaré inequality and logarithmic Sobolev inequality play a crucial role in the analysis of the behaviour of the process. To study of the Poincaré constant, Jerrum and Sinclair [19] introduced the path combinatoric method in theoretic computer science, which is further developed by Diaconis and Stroock [13], Fill [15], Sinclair [9], Chen [7], and so on. The logarithmic Sobolev inequality in the discrete setting was also studied by many authors, such as Diaconis and Saloff-Coste [1], Roberto [4], Lee and Yau [], Chen [8], Chen and Sheu [6], Chen et al. [5], and so on. The reader is referred to the books of Saloff-Coste [7] and Chen [9] for further information. The main purpose of this paper is to study the logarithmic Sobolev inequality, the generalized Cheeger isoperimetric inequality and the transport inequality. The remainder of this paper is organized as follows: in the next section, we focus on the logarithmic Sobolev inequality, and the third section is devoted to the transportation-information inequality and the generalized Cheeger isoperimetric inequality. In the last section, some examples are discussed and the estimates of involved constants are given.
3 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 13 Logarithmic Sobolev Inequality.1 Length Functions, Random Paths Apathγ xy from x to y is a family of edges {e 1,...,e n },wheree k =(x k 1,x k ) E, such that x 0 = x, x n = y. It is said to have no circle if all x k,k =0,...,n, are different. A positive function w : E (0, + ) defined on the edge set E is called length function, ifw(x, y) =w(y, x) for any e =(x, y) E. Given the length function w, thew-length of a path γ xy from x to y is defined by γ xy w := w(e), e γ xy and the distance associated with w is ρ w (x, y) :=min γ xy w. γ xy When w 1, ρ w =: ρ 1 is the natural graph distance on V. Diaconis and Stroock [13] showed that the Poincaré constant c P satisfies that c P max 1 γxy (e) γ xy 1/Q μ(x)μ(y) (.1) for any collection of paths {γ xy : x, y V }, where γ xy 1/Q is the length γ xy w with w(e) = 1/Q(e), a quite natural distance associated with the Markov process. Furthermore, by using the length functions, the estimate (.1) can be improved to be 1 c P max 1 γxy (e) γ xy w μ(x)μ(y), (.) Q(e)w(e) which is sharp for birth-death processes (see Kahale [0] or Chen [7]). Now for any x, y V different, let γ xy be a random (maybe deterministic) path without circle from x to y. By convention, we set γ xx = and denote by E γ the expectation w.r.t. {γ xy : x, y V }.. Logarithmic Sobolev Inequality Theorem.1 For any length function w and any edge e, let L w,e (x) :=E γ 1 γxy (e) γ xy w μ(y). y V (.3) The logarithmic Sobolev constant c LS is bounded by c LS inf 1 ( Entμ (L w,e )+μ(l w,e )log(e +1) ), w Q(e)w(e) (.4) where inf w is taken over all length functions w on E and e is the Euler constant. The upper bound in (.4) gives us a very practical criterion for the logarithmic Sobolev inequality and the estimate above is based on the following weighted Poincaré inequality, which is a slight generalization of (.). Lemma. (Weighted Poincaré inequality) Let ϕ be a nonnegative function on V. Then for any length function w, (f(x) μ(f)) ϕ(x)μ(x) c(ϕ, w)e(f,f), f : V R, (.5) x V
4 14 Ma Y. T. et al. where c(ϕ, w) :=max =max Q(e)w(e) Eγ Q(e)w(e) 1 γxy (e) γ xy w ϕ(x)μ(x)μ(y) L w,e (x)ϕ(x)μ(x). x V When ϕ 1, our constant c(ϕ, w) is the twice of the quantity on the right-hand side of (.). Proof For any fixed realization of random path {γ xy : x, y V }, (f(x) μ(f)) ϕ(x)μ(x) x V = ( (f(x) f(y))μ(y)) ϕ(x)μ(x) x V y V = ( μ(y) ) D e f ϕ(x)μ(x) x V y V e γ xy ( ) D e f ϕ(x)μ(x)μ(y) e γ xy ( )( ) 1 w(e) w(e) (D ef) ϕ(x)μ(x)μ(y) e γ xy e γ xy = 1 Q(e)(D e f) 1 γxy (e) γ xy w ϕ(x)μ(x)μ(y), Q(e)w(e) where the Cauchy Schwarz inequality is applied twice. Taking the expectation E γ w.r.t. the randomness of γ, we get the desired result. Now recall two important lemmas: the first one is due to Rothaus [6] and the second is given by Barthe Roberto []. Lemma.3 For any real function f on V and any constant a R, Lemma.4 For any real function f on V, Ent μ (f ) Ent μ ( (f a) ) +μ ( (f a) ). Ent μ (f )+μ(f ) sup { μ(f ϕ): ϕ 0,μ(e ϕ ) e +1 }. Consequently, by Donsker Varadhan s variational formula (see [14]), we have μ(f ϕ) μ(f )logμ(e ϕ ) Ent μ (f ), ϕ : V R, sup { μ(f ϕ): ϕ 0,μ(e ϕ ) e +1 } Ent μ (f )+μ(f )log(e +1). (.6) Proof of Theorem.1 By Lemmas.3 and.4, we have Ent μ (f ( ) Ent μ (f μ(f)) ) +μ ( (f μ(f)) ) { } sup (f(x) μ(f)) ϕ(x)μ(x) : ϕ 0,μ(e ϕ ) e +1 x V
5 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 15 sup c(ϕ, w) E(f,f), ϕ 0,μ(e ϕ ) e +1 where the last inequality follows from (.5). Moreover by (.5) and (.6), we have sup c(ϕ, w) =max ϕ 0,μ(e ϕ ) e +1 max which implies (.4). The proof is complete. Q(e)w(e) Q(e)w(e) sup μ(l w,e ϕ) ϕ 0,μ(e ϕ ) e +1 ( Entμ (L w,e )+μ(l w,e )log(e +1) ), 3 Transportation Inequalities In this section, we shall establish the transportation-information inequality W 1 I and as a corollary, the transportation-entropy inequality W 1 H. For this purpose, let us introduce some notations. 3.1 Wasserstein Distance, Entropy and Information Given a metric ρ on V, the Lipschitzian norm of a function g is denoted by g Lip(ρ). Let M 1 (V ) be the space of all probability measures on V. For any ν, μ M 1 (V ), recall that (i) The Wasserstein distance W 1,ρ (ν, μ) associated with ρ is defined as W 1,ρ (ν, μ) =inf ρ(x, y)π(dx, dy), π V where π runs over all couplings of (ν, μ), i.e., probability measures on V such that π(a V )= ν(a) andπ(v A) =μ(a) for all Borel subsets A of V.Ifρ(x, y) =1 x y is the discrete metric, W 1,ρ (ν, μ) = 1 ν μ TV where ν TV =sup f 1 ν(f) is the total variation of a signed measure ν. (ii) The relative entropy of ν w.r.t. μ is given by ν(x) x V ν(x)log, if ν μ; H(ν μ) = μ(x) +, otherwise. (iii) Fisher Donsker Varadhan information of a probability ν = h μ w.r.t. μ is defined by I(ν μ) := 1 (h(x) h(y)) Q(x, y) = 1 (D e h) Q(e), where D e h = h(y) h(x) for the oriented edge e =(x, y) E. 3. Transportation-information Inequality Guillin et al. [17] introduced the following transportation-information inequality for the given metric ρ, W1,ρ(ν, μ) c G I(ν μ), ν M 1 (V ), (3.1) where c G is the best constant. In [17], it is proved that (3.1) is equivalent to the following Gaussian concentration inequality: for all probabilities ν μ and ρ-lipschitzian function g on
6 16 Ma Y. T. et al. V, P ν ( 1 t t 0 ) g(x s )ds > μ(g)+r dν dμ L { exp tr c G g Lip(ρ) }, t, r > 0. (3.) Here (X t ) is the Markov process generated by L, defined on some probability space (Ω, F, P) with initial distribution ν. So c G is also called the Gaussian concentration constant for (X t ) (w.r.t. the metric ρ). The reader is referred to the book of Villani [30] for optimal transport, transport inequalities and related bibliographies. Theorem 3.1 The transportation-information inequality (3.1) holds with c G K := inf K(w), (3.3) w where the infimum is taken over all length functions w and the geometric constant K(w) is given by K(w) =max 1 Q(e)w(e) E γ 1 γxy (e)ρ (x, y) γ xy w μ(x)μ(y). (3.4) Remark 3. When ρ(x, y) = 1 x y (the discrete metric), K coincides with the quantity in (.). By Guillin et al. [17, Theorem 3.1], the transportation-information inequality w.r.t. thediscretemetricandthepoincaré inequality are equivalent: c P 8 c G c P. If we apply this result together with (.), we obtain only c G K. Since c P = K for birthdeath processes (see [7, 0]), we get c G K/8. In other words, our estimate of c G is of correct order. Proof of Theorem 3.1 For each probability measure ν = h μ, by Kantorovich Robinstein s identity (see [30]) and the Cauchy Schwarz inequality, W 1,ρ (ν, μ) = sup g(x) ( h (x) 1 ) μ(x) g Lip(ρ) 1 x V = 1 sup (g(x) g(y)) ( h (x) h (y) ) μ(x)μ(y) g Lip(ρ) 1 1 (g(x) g(y)) (h(x) h(y)) μ(x)μ(y) sup g Lip(ρ) 1 (h(x)+h(y)) μ(x)μ(y) x,y ρ (x, y)(h(x) h(y)) μ(x)μ(y). For any fixed random path {γ xy = γ xy (ω) :x, y V } and the length function w, wehaveby the Cauchy Schwarz inequality, ρ (x, y)(h(x) h(y)) μ(x)μ(y) x,y
7 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 17 = ( ) ρ (x, y) D e h μ(x)μ(y) x,y e γ x,y ( )( ρ (x, y)μ(x)μ(y) (D e h) 1 ) w(e) w(e) x,y e γ xy e γ xy = (D e h) 1 Q(e) 1 γx,y (e)ρ (x, y) γ xy w μ(x)μ(y). Q(e)w(e) Taking first the expectation E γ and then the maximum of the last term over all oriented edges e, wegetc G K(w). The proof is complete. Corollary 3.3 Assume that there exists some constant M>0such that 1 ρ (x, y)q(x, y) M. (3.5) sup x V y x Then the following transportation-entropy inequality holds W 1,ρ(ν, μ) KMH(ν μ), ν M 1 (V ), (3.6) or equivalently for any Lipschitzian function g, ( λ e λ(g μ(g)) MK dμ exp 4 Proof g Lip(ρ) ), λ R. (3.7) The transportation-entropy inequality (3.6) follows from the transportation information inequality (3.3) under the condition (3.5), by Guillin et al. [18, Theorem 4.]. The equivalence between (3.6) and the Gaussian concentration (3.7) is the famous Bobkov Götze s characterization in [4]. Corollary 3.4 For the Laplacian L =Δon the connected graph G =(V,E), we have, for the graph metric ρ 1, c G K d bd 3, E where d =max x V d x, D is the diameter of G and Proof b =max {ρ 1 -shortest paths γ : e γ}. (3.8) e Choose γ xy distributed uniformly on all shortest paths from x to y and w =1,wesee that K is bounded from above by (noting that Q(e) =1/ E and μ(x) =d x / E ) max ( ) E Eγ 1 γxy (e)ρ 1 (x, y) 3 d d bd 3. E E The proof is complete. 3.3 Generalized Cheeger Isoperimetric Inequality Consider the following generalized Cheeger isoperimetric inequality W 1,ρ (fμ,μ) c I D e f Q(e), ν = fμ M 1 (V ), (3.9) where c I is the best constant, called as Cheeger constant w.r.t. the metric ρ.
8 18 Ma Y. T. et al. Define the geometric constant κ Theorem 3.5 Proof V }, κ := max It holds that 1 Q(e) Eγ c I κ. 1 γxy (e)ρ(x, y)μ(x)μ(y). (3.10) By Kantorovich Robinstein s identity, we have, for any fixed random path {γ xy : x, y W 1,ρ (fμ,μ)= sup g(x)(f(x) 1)μ(x) g Lip(ρ) 1 x V = 1 sup (g(x) g(y)) (f(x) f(y)) μ(x)μ(y) g Lip(ρ) 1 1 ρ(x, y) D e f μ(x)μ(y) e:e γ xy = 1 1 D e f Q(e) 1 γxy (e)ρ(x, y)μ(x)μ(y). Q(e) Taking the expectation E γ, we obtain the desired result. Corollary 3.6 (Weighted L 1 -Poincaré inequality) for any function f on V, V Given a positive function ϕ on V, we have, f μ(f) ϕdμ κ D e f Q(e), (3.11) where κ is given by (3.10) with ρ(x, y) =1 x y (ϕ(x)+ϕ(y)),x,y V. Proof Considering (f c 1 )/c if necessary, we assume without loss of generality that f>0 and μ(f) = 1. In that case, for the metric ρ(x, y) =1 x y (ϕ(x)+ϕ(y)), it is known that W 1,ρ (fμ,μ)= ϕ(ν μ) TV = f 1 ϕdμ. By Theorem 3.5, we get (3.11). The proof is complete. Remark 3.7 Taking ϕ 1 and considering the corresponding geometric constant κ, (3.11) is equivalent to (by Bobkov and Houdré [3, Theorem 1.1]) μ(a)μ(a c ) κ Q(e), A V, where e A A := {e =(x, y) E : x A, y A c } is the boundary of A. Thus(3.11) implies the standard Cheeger inequality μ(a) κ Q(e), A V such that μ(a) 1/, e A which has an equivalent functional version as: for every function f on V, f(x) med μ (f) μ(x) κ D e f Q(e), (3.1) x V
9 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 19 where med μ (f) is the median of f under μ. The Cheeger inequality (3.1) with the geometric constant κ is due to Diaconis and Stroock [13], whose idea goes back to Jerrum and Sinclair [19]. Thus, Corollary 3.6 slightly improves theirs in this particular case. The Cheeger isoperimetric inequality for general jump processes is studied by Chen and Wang [10]. Remark 3.8 If G =(V,E) is a tree, i.e., there is only one path without circle from x to y for any two different vertices x, y, then the geometric constant κ becomes optimal for two types of metrics: (a) ρ(x, y) =1 x y (ϕ(x)+ϕ(y)) (then the constant κ in the weighted L 1 -Poincaré inequality above is optimal in the case of trees); (b) ρ(x, y) =ρ w (x, y), the distance induced by some length function w. The optimality of κ for those two types of metrics in the case of trees is established by Liu Ma Wu [3], in a completely different way. The usual Cheeger inequality exhibits the relationship between the isoperimetry and the Poincaré inequality (see [1, 19, 1]). Now we present the relationship between the generalized Cheeger isoperimetric inequality and the Gaussian concentration. Corollary 3.9 Assume that y:y x q(x, y) B for all x V.Then c G κ B. Proof This is due to [18]. But for the self-completeness, we still present its proof. By the generalized Cheeger isoperimetric inequality in Theorem 3.5 and the Cauchy Schwarz inequality, we have, for any probability measure ν = fμ, W 1,ρ (fμ,μ) κ μ(x)q(x, y) f(x) f(y) x y κ 1 I(ν μ) μ(x)q(x, y)( f(x)+ f(y)) x y κ I(ν μ) μ(x)q(x, y)f(x) x y κ I(ν μ) B μ(x)f(x) =κ BI(ν μ), x V where the desired result follows. Corollary 3.10 For the Laplacian L =Δon the connected graph G =(V,E), we have, for the graph metric ρ 1, κ d bd, E where d,d,b are given in Corollary 3.4. Proof Choosing γ xy distributed uniformly on all shortest paths from x to y and w =1,since
10 130 Ma Y. T. et al. Q(e) =1/ E and μ(x) =d x / E, the geometric constant κ is bounded from above by max ( ) d E Eγ 1 γxy (e)ρ 1 (x, y) d bd. E E The proof is complete. 4 Several Examples and Graphs with Symmetry 4.1 Several Examples Webeginwithababy-model. Example 4.1 (Complete graph) Let G =(V,E) be a complete graph with n different vertices, i.e., for any different x, y V,(x, y) E (n of course). Consider the Laplacian L =Δand the graph metric ρ 1 which is now ρ 1 (x, y) =1 x y. Hence μ is the uniform distribution on V and Q(e) =1/ E =1/[n(n 1)]. In such case the Dirichlet form is given by E(f,f) = 1 (D e f) Q(e) = n n 1 Var μ(f), where Var μ (f) =μ(f ) μ(f) is the variance of f w.r.t. μ. Soc P = n 1 n. In this example, we take γ xy = {(x, y)} as random path and the length function w 1. For the logarithmic Sobolev constant c LS, notice that for any fixed edge e =(x 0,y 0 ), e γ xy if and only if x = x 0 and y = y 0 ;andl w,e (x) =1 x=x0 /n. Thus by Theorem.1, c LS E ( Ent μ (L w,e )+μ(l w,e )log(e +1) ) [ 1 = n(n 1) n log 1 n 1 n log 1 n + 1 ] n log(e +1) ( = 1 n) 1 [log n +log(e +1) ]. (4.1) Comparing with the optimal logarithmic Sobolev constant c LS = n 1 n log(n 1) for complete graph (see [1, Corollary A.5]), the estimate (4.1) has the correct order log n. Now we turn to bound the Gaussian concentration constant c G by the geometric quantity K in (3.4), w.r.t. the graph metric ρ 1.Wehave K = max (x,y) E 1 μ(x)μ(y) = E Q(x, y) n = n 1 n. Then by Theorem 3.1, for any μ-probability density f, W1,ρ 1 (fμ,μ)= 1 ( ) f 1 dμ n 1 4 n E( f, f) = Var μ ( f). V But by [17, Theorem 3.1], the corresponding optimal constant c G = n 1 n. Consequently, we have K = n 1 n = c G K.
11 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 131 For the generalized Cheeger isoperimetric inequality in Theorem 3.5 w.r.t. ρ 1,wehave or equivalently, x V c I κ = K n 1 n f(x) μ(f) μ(x) n 1 n D e f Q(e). This inequality becomes equality for the indicator function 1 A. Hence c I = κ, i.e., our generalized Cheeger isoperimetric inequality in Theorem 3.5 is optimal in this example. Example 4. (Star) Consider a star G =(V,E) with a central vertex v 0 and n outside vertices {v i : i = 1,...,n} connecting only with v 0. For the Laplacian L = Δ, we have μ(v 0 )= 1,μ(v k)= 1 1 n, 1 k n and Q(e) = n for every edge e. Itisknownthatc P =1(c.f. [13]). Taking the length function w 1 in (.4), we obtain by calculus ( 3 c LS 1 ) log[n(e +1)]. n Applying the logarithmic Sobolev inequality to f =1 vk, 1 k n, we get c LS log(n)/. Clearly, for large n, we have the correct order log n. For the geometric constants K and κ associated with the graph distance ρ 1,takingγ xy as the unique path from x to y without circle, we have Considering f(v) =n1 [v=v1 ], we have K 9 4 n and κ = 3 1 n. W 1 (fμ,μ)= 3 1 n, D e f Q(e) =, c I = κ = 3 1 n, i.e., the geometric quantity κ as an upper bound of c I is optimal. Example 4.3 (Trees) Consider the full binary tree of depth d. For d 1, such a tree has d+1 1 vertices, d+1 edges and the maximum degree is 3. Consider the Markov chain arising from nearest neighbor random walk on this tree. The longest path is of length d and the value of b defined in (3.8) is ( d 1) d. By Corollary 3.4, we have K 18 d d 3. For κ w.r.t. the graph distance ρ 1, by (3.10), Theorem 4.1 and Corollary 7.1 in [3], κ =(d 3) d +3 9 d d 1, which shows that Corollary 3.10 offers a good upper bound. 4. Graphs with Symmetry In this section, we shall consider various graphs with symmetry. See Chung [11] for examples and properties of symmetric graphs. For a graph G =(V,E), an automorphism f : V V is
12 13 Ma Y. T. et al. one-to-one mapping which preserves edges, i.e., for any x, y V,wehave(x, y) E if and only if (f(x),f(y)) E. For any oriented edge e =(x, y) E, consider the opposite oriented edge e := (y, x) and the non-oriented edge e 0 := {x, y}. PutE 0 := {e 0 : e E}, the set of all non-oriented edges Edge-transitive Graph A graph G is called edge-transitive if for any two non-oriented edges {x, y} and {x,y },there is an automorphism f such that {f(x),f(y)} = {x,y }. Corollary 4.4 Assume that G is edge-transitive. For the Laplacian L =Δand the graph metric ρ 1, we have c I κ E [ ρ 1(X, Y ) ] and c G κ (E[ρ 1(X, Y )]), where the law of (X, Y ) is μ μ and μ is the uniform measure on V. Proof We consider a random (ordered) pair of vertices (X, Y ), chosen according to μ μ. Now given (X, Y ), we choose randomly a shortest path γ XY between X and Y (uniformly chosen over all possible shortest paths from X to Y ). Notice that for w 1, ρ = ρ 1, 1 h(e) := E γ 1 γxy (e)ρ(x, y)μ(x)μ(y) = E Eρ 1 (X, Y )1 γxy (e) Q(e)w(e) satisfies h(e) =h( e )fore E (that is true on any graph). Then h canberegardedasalength function on E 0. Now by the edge-transitivity, h(e) does not depend on e, so we get by averaging over all edges e, Therefore h(e) = 1 E E E [ρ 1 (X, Y )1 γxy (e)] = E [ ρ 1(X, Y ) ]. κ max h(e) =E [ ρ 1(X, Y ) ]. Since y:y x q(x, y) 1 for all x V,wehavec G κ by Corollary 3.9. The proof is complete. Remark 4.5 From the result above, we may wonder whether on edge transitive graphs the correct order in diameter D of c G is D 4, and that of c I is D, which is indeed true. For example, for the Laplacian on the circle Z p := Z/pZ, c P is of order D. Taking the eigenfunction h corresponding to λ 1 =1/c P with h Lip(ρ1 ) =1,weseethatVar μ (h) isoforderd,too. By the central limit theorem, 1 t h(x s )ds t converges weakly to the normal law N(0,σ (h)), where the limit variance is 0 σ (h) = ( Δ) 1 h, h μ =c P Var μ (h),
13 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 133 which is of order D 4. But from the Gaussian concentration inequality, we always have c G σ (h). In other words, c G is at least of order D 4. We leave to the reader for verifying that the correct order of c I is D. Example 4.6 (Circle Z p ) Let p Z and consider the integers mod p as p points around a circle. For x and y in Z p,chooseγ xy as the shorter of the two paths from x to y. Forthismodel μ(x) =1/p (x Z p ),Q(e) =1/(p) for any edge e. Itiswellknownthatc P =(1 cos π p ) 1, which is also the logarithmic Sobolev constant c LS when p is even (c.f. [6]). Taking the length function w 1 in (.4), we obtain by careful calculation, log(3(e +1)) (p +1)(p +), p is even; c LS 1 log(3(e +1)) (p +1)(p +)(1+3/p), p is odd, (4.) 1 ( 5 log(3(e +1)) 1 cos π ) 1. p This, together with c LS c P =(1 cos π p ) 1, offers a two sided estimate for c LS with factor 5 log(3(e +1)). Since the circle Z p is edge transitive, by Corollary 4.4, we have c I κ p 1 + o(p ); c G κ p4 1 + o(p4 ). For this model, Sammer and Tetali [8] proved that the best constant in the transportationentropy inequality (3.6) is p 48 + o(p ). Then by Corollary 3.3, we have p o(p4 ) c G p4 1 + o(p4 ). Thus the correct order of c G is p 4, as mentioned in Remark Vertex-transitive Graph A graph G is vertex-transitive if for any two vertices u and v, there is an automorphism f such that f(u) =v. The automorphism group defines an equivalent relation on the edges of G. Two undirected edges e 0 1, e 0 are equivalent if and only if there is an automorphism mapping e 0 1 to e 0. We can consider equivalent classes of undirected edges, denoted by E 0 1,...,E 0 s. The index of G is defined as index(g) =max i E 0 E 0 i. Clearly E 0 i V,i =1,...,s, 1 index(g) d, where d = d x for any x V, the degree of the graph G. See[11]. For any edge e such that e 0 Ei 0, i =1,...,s, E μ μ [ ] 1 ρ 1 (X, Y )1 [e γxy ] = Ei 0 E μ μ [ ] ρ 1 (X, Y )1 [e γxy ] e:e 0 Ei 0 index(g) E μ μ [ ρ E 1(X, Y ) ].
14 134 Ma Y. T. et al. For any two vertices y, y V, there is an automorphism such that f(y) =y. Since the stationary distribution μ 1/ E and ρ 1 (x, f(y)) = ρ 1 (f 1 (x),y) for any x V,wehave E μ [ ρ 1(X, y ) ] = E μ [ ρ 1(X, f(y)) ] = E μ [ ρ 1(f 1 (X),y) ] = E μ [ ρ 1(X, y) ]. Then for any fixed vertex v 0 V, E μ μ [ ρ 1(X, Y ) ] = E μ [ ρ 1(X, v 0 ) ]. Therefore, we have proved the following estimate of the Gaussian constant c G in (3.1). Corollary 4.7 Let Δ be the Laplacian operator on a vertex transitive graph G. For any fixed vertex v 0 V and the graph metric ρ 1, we have c I κ index(g)e μ [ρ 1(X, v 0 )] de μ [ρ 1(X, v 0 )] and where c G K κ, K index(g)e μ [ρ 4 1(X, v 0 )] de μ [ρ 4 1(X, v 0 )]. The proof of the bound on K is similar, omitted here Distance Transitive Graph AgraphG is distance transitive if for any two pairs of vertices {x, y} and {x,y } with ρ 1 (x, y) = ρ 1 (x,y ), there is an automorphism mapping x to x and y to y. The distance transitive graph is both edge-transitive and vertex-transitive. Then index(g) = 1. The estimate in Corollary 4.7 holds for distance transitive graphs, that is, for any fixed vertex v 0 V, c G ( E μ [ ρ 1(X, v 0 ) ]) and c I E μ [ ρ 1(X, v 0 ) ]. (4.3) Example 4.8 The vertex set V consists of all the subsets of k elements in {1,,..., n} (1 k n is fixed). Define a metric on V by d(x, y) =k x y. The edge set is given by {(x, y) V : d(x, y) =1}. This is a distance transitive graph. The Markov process generated by the Laplacian Δ on G is known as the Bernoulli Laplace diffusion model. See Lee and Yau [] for the estimate of the logarithmic Sobolev constant, Gao and Quastel [16] for the exponential decay rate of entropy. By (4.3), we have for the graph metric ρ 1 = d, c I κ and c G κ, where κ ( 1 min{k,n k} ( k n j k) j j=0 )( n k j ). Acknowledgements The authors are grateful to the anonymous referees for constructive comments and corrections.
15 Logarithmic Sobolev, Isoperimetry and Transport Inequalities on Graphs 135 References [1] Alon, N., Milman, V.: λ 1, isoperimetric inequalities for graphs, and superconcentrators. J. Combin. Theory, Ser. B., 38, (1985) [] Barthe, F., Roberto, C.: Sobolev inequalities for probability measures on the real line. Studia Math., 159(3): (003) [3] Bobkov, S., Houdré, C.: Some connections between isoperimetric and Sobolev-type inequalities. Mem. Amer. Math. Soc., 19, 1997 [4] Bobkov, S., Götze, F.: Exponential integrability and transportation cost related to logarithmic Sobolev inequalities. J. Funct. Anal., 163, 1 8 (1999) [5] Chen, G. Y., Liu, W.-W., Saloff-Coste, L.: The logarithmic Sobolev constant of some finite Markov chains. Ann. Fac. Sci. Toulouse Math., 17(6), (008) [6] Chen, G. Y., Sheu, Y. C.: On the log-sobolev constant for the simple random walk on the n-cycle: the even cases. J. Funct. Anal., 0, (003) [7] Chen, M. F.: Analytic proof of dual variational formula for the first eigenvalue in dimension one. Sci. China Ser. A, 4(8), (1999) [8] Chen, M. F.: Logarithmic Sobolev inequality for symmetric forms. Sci. China Ser. A, 43(6), (000) [9] Chen, M. F.: Eigenvalues, Inequalities and Ergodic Theory, Springer, London, 005 [10] Chen, M. F., Wang, F. Y.: Cheeger s inequalities for general symmetric forms and existence criteria for spectral gap. Ann. Probab., 8(1), (000) [11] Chung, F. R. K.: Spectral Graph Theory, CBMS Regional Conference Series in Mathematics, 9, Washington, American Mathematical Society, Providence, RI, 1997 [1] Diaconis, P., Saloff-Coste, L.: Logarithmic Sobolev inequalities for Markov chains. Ann. App. Probab., 6(3), (1996) [13] Diaconis, P., Stroock, D.: Geometric bounds for eigenvalues of Markov chains. Ann. App. Probab., 1(1), 36 6 (1991) [14] Donsker, M. D., Varadhan, S. R. S.: Asymptotic evaluation of certain Markov process expectations for large time. IV. Comm. Pure Appl. Math., 18, (1983) [15] Fill, J.: Eigenvalue bounds on bonvergence to stationarity for nonreversible Markov chains, with an application to the exclusion process. Ann. App. Probab., 1(1), 6 87 (1991) [16] Gao, F., Quastel, J.: Exponential decay of entropy in the random transposition and Bernoulli Laplace models. Ann. Appl. Probab., 13, (003) [17] Guillin, A., Léonard, C., Wu, L. M., et al.: Transportation-information inequalities for Markov processes. Probab. Th. Relat. Fields, 144, (009) [18] Guillin, A., Joulin, A., Léonard, C., et al.: Transportation-information inequalities for Markov processes (III). Processes with jumps, preprint, (013) [19] Jerrum, M., Sinclair, A.: Approximating the permanent. SIAM J. Computer, 18, (1989) [0] Kahale, N.: A semidefinite bound for mixing rates of Markov chains, Integer Programming and Combinatorial Optimization, Lecture Notes in Computer Science, 1084, 1996, [1] Lawler, G. F., Sokal, A. D.: Bounds on the L spectrum for Markov chains and Markov processes: a generalization of Cheeger s inequalities. Trans. Amer. Math. Soc., 309, (1988) [] Lee, T. Y., Yau, H. T.: Logarithmic Sobolev inequality for some models of random walks. Ann. Probab., 6, (1998) [3] Liu, W., Ma, Y. T., Wu, L. M.: Spectral gap, isoperimetry and concentration on trees. Sci. China Math., 59, (016) [4] Roberto, C.: A path method for the logarithmic Sobolev constant. Combin. Probab. Comput., 1, (003) [5] Rothaus, O.: Diffusion on compact Riemannian manifolds and logarithmic Sobolev inequalities. J. Funct. Anal., (1981) [6] Rothaus, O.: Analytic inequalities, isoperimetric inequalities and logarithmic Sobolev inequalities. J. Funct. Anal., 64, (1985) [7] Saloff-Coste, L.: Lectures on finite Markov chains, In Lectures on Probability Theory and Statistics: École d Été de Probabilités de St-Flour, Vol of Lecture Notes in Mathematics, Springer, Berlin, 1996
16 136 Ma Y. T. et al. [8] Sammer, M., Tetali, P.: Concentration on the discrete torus using transportation. Combin. Probab. Comput., 18, (009) [9] Sinclair, A.: Improved bounds for mixing rates of Markov chains and multicommodity flow. Combin. Probab. Comput., 1, (199) [30] Villani, C.: Optimal transport. Old and new. Grundlehren der Mathematischen Wissenschaften [Fundamental Principles of Mathematical Sciences], 338, Springer-Verlag, Berlin, 009
215 Problem 1. (a) Define the total variation distance µ ν tv for probability distributions µ, ν on a finite set S. Show that
15 Problem 1. (a) Define the total variation distance µ ν tv for probability distributions µ, ν on a finite set S. Show that µ ν tv = (1/) x S µ(x) ν(x) = x S(µ(x) ν(x)) + where a + = max(a, 0). Show that
More informationcurvature, mixing, and entropic interpolation Simons Feb-2016 and CSE 599s Lecture 13
curvature, mixing, and entropic interpolation Simons Feb-2016 and CSE 599s Lecture 13 James R. Lee University of Washington Joint with Ronen Eldan (Weizmann) and Joseph Lehec (Paris-Dauphine) Markov chain
More informationAn example of application of discrete Hardy s inequalities
An example of application of discrete Hardy s inequalities Laurent Miclo Laboratoire de Statistique et Probabilités, UMR C5583 Université PaulSabatieretCNRS 8, route de Narbonne 3062 Toulouse cedex, France
More informationA NOTE ON THE POINCARÉ AND CHEEGER INEQUALITIES FOR SIMPLE RANDOM WALK ON A CONNECTED GRAPH. John Pike
A NOTE ON THE POINCARÉ AND CHEEGER INEQUALITIES FOR SIMPLE RANDOM WALK ON A CONNECTED GRAPH John Pike Department of Mathematics University of Southern California jpike@usc.edu Abstract. In 1991, Persi
More informationLogarithmic Harnack inequalities
Logarithmic Harnack inequalities F. R. K. Chung University of Pennsylvania Philadelphia, Pennsylvania 19104 S.-T. Yau Harvard University Cambridge, assachusetts 02138 1 Introduction We consider the relationship
More informationarxiv:math/ v1 [math.pr] 31 Jan 2001
Chin. Sci. Bulletin, 1999, 44(23), 2465 2470 (Chinese Ed.); 2000, 45:9 (English Ed.), 769 774 Eigenvalues, inequalities and ergodic theory arxiv:math/0101257v1 [math.pr] 31 Jan 2001 Mu-Fa Chen (Beijing
More informationSPECTRAL GAP, LOGARITHMIC SOBOLEV CONSTANT, AND GEOMETRIC BOUNDS. M. Ledoux University of Toulouse, France
SPECTRAL GAP, LOGARITHMIC SOBOLEV CONSTANT, AND GEOMETRIC BOUNDS M. Ledoux University of Toulouse, France Abstract. We survey recent works on the connection between spectral gap and logarithmic Sobolev
More informationEigenvalues of graphs
Eigenvalues of graphs F. R. K. Chung University of Pennsylvania Philadelphia PA 19104 September 11, 1996 1 Introduction The study of eigenvalues of graphs has a long history. From the early days, representation
More informationDiscrete Ricci curvature: Open problems
Discrete Ricci curvature: Open problems Yann Ollivier, May 2008 Abstract This document lists some open problems related to the notion of discrete Ricci curvature defined in [Oll09, Oll07]. Do not hesitate
More informationA note on the convex infimum convolution inequality
A note on the convex infimum convolution inequality Naomi Feldheim, Arnaud Marsiglietti, Piotr Nayar, Jing Wang Abstract We characterize the symmetric measures which satisfy the one dimensional convex
More informationLogarithmic Sobolev and Poincaré inequalities for the circular Cauchy distribution
Electron. Commun. Probab. 9 4), no., 9. DOI:.4/ECP.v9-37 ISSN: 83-589X ELECTRONIC COMMUNICATIONS in PROBABILITY Logarithmic Sobolev and Poincaré inequalities for the circular Cauchy distribution Yutao
More informationExpansion and Isoperimetric Constants for Product Graphs
Expansion and Isoperimetric Constants for Product Graphs C. Houdré and T. Stoyanov May 4, 2004 Abstract Vertex and edge isoperimetric constants of graphs are studied. Using a functional-analytic approach,
More informationarxiv: v1 [math.co] 27 Jul 2012
Harnack inequalities for graphs with non-negative Ricci curvature arxiv:1207.6612v1 [math.co] 27 Jul 2012 Fan Chung University of California, San Diego S.-T. Yau Harvard University May 2, 2014 Abstract
More informationReversible Markov chains
Reversible Markov chains Variational representations and ordering Chris Sherlock Abstract This pedagogical document explains three variational representations that are useful when comparing the efficiencies
More informationContents 1. Introduction 1 2. Main results 3 3. Proof of the main inequalities 7 4. Application to random dynamical systems 11 References 16
WEIGHTED CSISZÁR-KULLBACK-PINSKER INEQUALITIES AND APPLICATIONS TO TRANSPORTATION INEQUALITIES FRANÇOIS BOLLEY AND CÉDRIC VILLANI Abstract. We strengthen the usual Csiszár-Kullback-Pinsker inequality by
More informationUniqueness of Fokker-Planck equations for spin lattice systems (I): compact case
Semigroup Forum (213) 86:583 591 DOI 1.17/s233-12-945-y RESEARCH ARTICLE Uniqueness of Fokker-Planck equations for spin lattice systems (I): compact case Ludovic Dan Lemle Ran Wang Liming Wu Received:
More informationConvex inequalities, isoperimetry and spectral gap III
Convex inequalities, isoperimetry and spectral gap III Jesús Bastero (Universidad de Zaragoza) CIDAMA Antequera, September 11, 2014 Part III. K-L-S spectral gap conjecture KLS estimate, through Milman's
More informationIsoperimetric inequalities for cartesian products of graphs
Isoperimetric inequalities for cartesian products of graphs F. R. K. Chung University of Pennsylvania Philadelphia 19104 Prasad Tetali School of Mathematics Georgia Inst. of Technology Atlanta GA 3033-0160
More informationConcentration inequalities: basics and some new challenges
Concentration inequalities: basics and some new challenges M. Ledoux University of Toulouse, France & Institut Universitaire de France Measure concentration geometric functional analysis, probability theory,
More informationA Spectral Gap for the Brownian Bridge measure on hyperbolic spaces
1 A Spectral Gap for the Brownian Bridge measure on hyperbolic spaces X. Chen, X.-M. Li, and B. Wu Mathemtics Institute, University of Warwick,Coventry CV4 7AL, U.K. 1. Introduction Let N be a finite or
More informationConcentration Properties of Restricted Measures with Applications to Non-Lipschitz Functions
Concentration Properties of Restricted Measures with Applications to Non-Lipschitz Functions S G Bobkov, P Nayar, and P Tetali April 4, 6 Mathematics Subject Classification Primary 6Gxx Keywords and phrases
More informationSpectral Gap and Concentration for Some Spherically Symmetric Probability Measures
Spectral Gap and Concentration for Some Spherically Symmetric Probability Measures S.G. Bobkov School of Mathematics, University of Minnesota, 127 Vincent Hall, 26 Church St. S.E., Minneapolis, MN 55455,
More informationUPPER BOUNDS FOR EIGENVALUES OF THE DISCRETE AND CONTINUOUS LAPLACE OPERATORS
UPPER BOUNDS FOR EIGENVALUES OF THE DISCRETE AND CONTINUOUS LAPLACE OPERATORS F. R. K. Chung University of Pennsylvania, Philadelphia, Pennsylvania 904 A. Grigor yan Imperial College, London, SW7 B UK
More informationKLS-TYPE ISOPERIMETRIC BOUNDS FOR LOG-CONCAVE PROBABILITY MEASURES. December, 2014
KLS-TYPE ISOPERIMETRIC BOUNDS FOR LOG-CONCAVE PROBABILITY MEASURES Sergey G. Bobkov and Dario Cordero-Erausquin December, 04 Abstract The paper considers geometric lower bounds on the isoperimetric constant
More informationG(t) := i. G(t) = 1 + e λut (1) u=2
Note: a conjectured compactification of some finite reversible MCs There are two established theories which concern different aspects of the behavior of finite state Markov chains as the size of the state
More informationA REPRESENTATION FOR THE KANTOROVICH RUBINSTEIN DISTANCE DEFINED BY THE CAMERON MARTIN NORM OF A GAUSSIAN MEASURE ON A BANACH SPACE
Theory of Stochastic Processes Vol. 21 (37), no. 2, 2016, pp. 84 90 G. V. RIABOV A REPRESENTATION FOR THE KANTOROVICH RUBINSTEIN DISTANCE DEFINED BY THE CAMERON MARTIN NORM OF A GAUSSIAN MEASURE ON A BANACH
More informationConductance, the Normalized Laplacian, and Cheeger s Inequality
Spectral Graph Theory Lecture 6 Conductance, the Normalized Laplacian, and Cheeger s Inequality Daniel A. Spielman September 17, 2012 6.1 About these notes These notes are not necessarily an accurate representation
More informationFunctional inequalities for heavy tailed distributions and application to isoperimetry
E l e c t r o n i c J o u r n a l o f P r o b a b i l i t y Vol. 5 (200), Paper no. 3, pages 346 385. Journal URL http://www.math.washington.edu/~ejpecp/ Functional inequalities for heavy tailed distributions
More informationDisplacement convexity of the relative entropy in the discrete h
Displacement convexity of the relative entropy in the discrete hypercube LAMA Université Paris Est Marne-la-Vallée Phenomena in high dimensions in geometric analysis, random matrices, and computational
More informationConvergence to equilibrium of Markov processes (eventually piecewise deterministic)
Convergence to equilibrium of Markov processes (eventually piecewise deterministic) A. Guillin Université Blaise Pascal and IUF Rennes joint works with D. Bakry, F. Barthe, F. Bolley, P. Cattiaux, R. Douc,
More informationINTERPOLATION BETWEEN LOGARITHMIC SOBOLEV AND POINCARÉ INEQUALITIES
INTERPOLATION BETWEEN LOGARITHMIC SOBOLEV AND POINCARÉ INEQUALITIES ANTON ARNOLD, JEAN-PHILIPPE BARTIER, AND JEAN DOLBEAULT Abstract. This paper is concerned with intermediate inequalities which interpolate
More informationHYPERCONTRACTIVE MEASURES, TALAGRAND S INEQUALITY, AND INFLUENCES
HYPERCONTRACTIVE MEASURES, TALAGRAND S INEQUALITY, AND INFLUENCES D. Cordero-Erausquin, M. Ledoux University of Paris 6 and University of Toulouse, France Abstract. We survey several Talagrand type inequalities
More informationStability results for Logarithmic Sobolev inequality
Stability results for Logarithmic Sobolev inequality Daesung Kim (joint work with Emanuel Indrei) Department of Mathematics Purdue University September 20, 2017 Daesung Kim (Purdue) Stability for LSI Probability
More informationL -uniqueness of Schrödinger operators on a Riemannian manifold
L -uniqueness of Schrödinger operators on a Riemannian manifold Ludovic Dan Lemle Abstract. The main purpose of this paper is to study L -uniqueness of Schrödinger operators and generalized Schrödinger
More informationPCMI LECTURE NOTES ON PROPERTY (T ), EXPANDER GRAPHS AND APPROXIMATE GROUPS (PRELIMINARY VERSION)
PCMI LECTURE NOTES ON PROPERTY (T ), EXPANDER GRAPHS AND APPROXIMATE GROUPS (PRELIMINARY VERSION) EMMANUEL BREUILLARD 1. Lecture 1, Spectral gaps for infinite groups and non-amenability The final aim of
More informationCapacitary inequalities in discrete setting and application to metastable Markov chains. André Schlichting
Capacitary inequalities in discrete setting and application to metastable Markov chains André Schlichting Institute for Applied Mathematics, University of Bonn joint work with M. Slowik (TU Berlin) 12
More informationAPPLICATIONS OF THE KANTOROVICH-RUBINSTEIN MAXIMUM PRINCIPLE IN THE THEORY OF MARKOV OPERATORS
12 th International Workshop for Young Mathematicians Probability Theory and Statistics Kraków, 20-26 September 2009 pp. 43-51 APPLICATIONS OF THE KANTOROVICH-RUBINSTEIN MAIMUM PRINCIPLE IN THE THEORY
More informationOllivier Ricci curvature for general graph Laplacians
for general graph Laplacians York College and the Graduate Center City University of New York 6th Cornell Conference on Analysis, Probability and Mathematical Physics on Fractals Cornell University June
More informationarxiv: v2 [math.co] 2 Jul 2013
OLLIVIER-RICCI CURVATURE AND THE SPECTRUM OF THE NORMALIZED GRAPH LAPLACE OPERATOR FRANK BAUER, JÜRGEN JOST, AND SHIPING LIU arxiv:11053803v2 [mathco] 2 Jul 2013 Abstract We prove the following estimate
More informationM. Ledoux Université de Toulouse, France
ON MANIFOLDS WITH NON-NEGATIVE RICCI CURVATURE AND SOBOLEV INEQUALITIES M. Ledoux Université de Toulouse, France Abstract. Let M be a complete n-dimensional Riemanian manifold with non-negative Ricci curvature
More informationLocal semiconvexity of Kantorovich potentials on non-compact manifolds
Local semiconvexity of Kantorovich potentials on non-compact manifolds Alessio Figalli, Nicola Gigli Abstract We prove that any Kantorovich potential for the cost function c = d / on a Riemannian manifold
More informationModern Discrete Probability Spectral Techniques
Modern Discrete Probability VI - Spectral Techniques Background Sébastien Roch UW Madison Mathematics December 22, 2014 1 Review 2 3 4 Mixing time I Theorem (Convergence to stationarity) Consider a finite
More informationthe neumann-cheeger constant of the jungle gym
the neumann-cheeger constant of the jungle gym Itai Benjamini Isaac Chavel Edgar A. Feldman Our jungle gyms are dimensional differentiable manifolds M, with preferred Riemannian metrics, associated to
More informationProbability and Measure
Part II Year 2018 2017 2016 2015 2014 2013 2012 2011 2010 2009 2008 2007 2006 2005 2018 84 Paper 4, Section II 26J Let (X, A) be a measurable space. Let T : X X be a measurable map, and µ a probability
More informationON THE ZERO-ONE LAW AND THE LAW OF LARGE NUMBERS FOR RANDOM WALK IN MIXING RAN- DOM ENVIRONMENT
Elect. Comm. in Probab. 10 (2005), 36 44 ELECTRONIC COMMUNICATIONS in PROBABILITY ON THE ZERO-ONE LAW AND THE LAW OF LARGE NUMBERS FOR RANDOM WALK IN MIXING RAN- DOM ENVIRONMENT FIRAS RASSOUL AGHA Department
More informationSpectral Gap for Complete Graphs: Upper and Lower Estimates
ISSN: 1401-5617 Spectral Gap for Complete Graphs: Upper and Lower Estimates Pavel Kurasov Research Reports in Mathematics Number, 015 Department of Mathematics Stockholm University Electronic version of
More informationStein s method, logarithmic Sobolev and transport inequalities
Stein s method, logarithmic Sobolev and transport inequalities M. Ledoux University of Toulouse, France and Institut Universitaire de France Stein s method, logarithmic Sobolev and transport inequalities
More informationStochastic relations of random variables and processes
Stochastic relations of random variables and processes Lasse Leskelä Helsinki University of Technology 7th World Congress in Probability and Statistics Singapore, 18 July 2008 Fundamental problem of applied
More informationHeat Flows, Geometric and Functional Inequalities
Heat Flows, Geometric and Functional Inequalities M. Ledoux Institut de Mathématiques de Toulouse, France heat flow and semigroup interpolations Duhamel formula (19th century) pde, probability, dynamics
More informationON PARABOLIC HARNACK INEQUALITY
ON PARABOLIC HARNACK INEQUALITY JIAXIN HU Abstract. We show that the parabolic Harnack inequality is equivalent to the near-diagonal lower bound of the Dirichlet heat kernel on any ball in a metric measure-energy
More informationMULTIPLE SOLUTIONS FOR THE p-laplace EQUATION WITH NONLINEAR BOUNDARY CONDITIONS
Electronic Journal of Differential Equations, Vol. 2006(2006), No. 37, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) MULTIPLE
More informationEigenvalues, random walks and Ramanujan graphs
Eigenvalues, random walks and Ramanujan graphs David Ellis 1 The Expander Mixing lemma We have seen that a bounded-degree graph is a good edge-expander if and only if if has large spectral gap If G = (V,
More informationIntertwinings for Markov processes
Intertwinings for Markov processes Aldéric Joulin - University of Toulouse Joint work with : Michel Bonnefont - Univ. Bordeaux Workshop 2 Piecewise Deterministic Markov Processes ennes - May 15-17, 2013
More informationarxiv: v1 [math.ap] 18 May 2017
Littlewood-Paley-Stein functions for Schrödinger operators arxiv:175.6794v1 [math.ap] 18 May 217 El Maati Ouhabaz Dedicated to the memory of Abdelghani Bellouquid (2/2/1966 8/31/215) Abstract We study
More informationDiscrete Ricci curvature via convexity of the entropy
Discrete Ricci curvature via convexity of the entropy Jan Maas University of Bonn Joint work with Matthias Erbar Simons Institute for the Theory of Computing UC Berkeley 2 October 2013 Starting point McCann
More informationFAT AND THIN SETS FOR DOUBLING MEASURES IN EUCLIDEAN SPACE
Annales Academiæ Scientiarum Fennicæ Mathematica Volumen 38, 2013, 535 546 FAT AND THIN SETS FOR DOUBLING MEASURES IN EUCLIDEAN SPACE Wen Wang, Shengyou Wen and Zhi-Ying Wen Yunnan University, Department
More informationLecture 8: Path Technology
Counting and Sampling Fall 07 Lecture 8: Path Technology Lecturer: Shayan Oveis Gharan October 0 Disclaimer: These notes have not been subjected to the usual scrutiny reserved for formal publications.
More informationHeat Kernels on Manifolds, Graphs and Fractals
Heat Kernels on Manifolds, Graphs and Fractals Alexander Grigor yan Abstract. We consider heat kernels on different spaces such as Riemannian manifolds, graphs, and abstract metric measure spaces including
More informationOn the simplest expression of the perturbed Moore Penrose metric generalized inverse
Annals of the University of Bucharest (mathematical series) 4 (LXII) (2013), 433 446 On the simplest expression of the perturbed Moore Penrose metric generalized inverse Jianbing Cao and Yifeng Xue Communicated
More informationInverse Brascamp-Lieb inequalities along the Heat equation
Inverse Brascamp-Lieb inequalities along the Heat equation Franck Barthe and Dario Cordero-Erausquin October 8, 003 Abstract Adapting Borell s proof of Ehrhard s inequality for general sets, we provide
More informationKLS-type isoperimetric bounds for log-concave probability measures
Annali di Matematica DOI 0.007/s03-05-0483- KLS-type isoperimetric bounds for log-concave probability measures Sergey G. Bobkov Dario Cordero-Erausquin Received: 8 April 04 / Accepted: 4 January 05 Fondazione
More informationarxiv: v1 [math.pr] 17 Apr 2018
MULTIPLE SETS EXPONENTIAL CONCENTRATION AND HIGHER ORDER EIGENVALUES NATHAËL GOZLAN & RONAN HERRY arxiv:804.0633v [math.pr] 7 Apr 208 Abstract. On a generic metric measured space, we introduce a notion
More informationA Note on the Central Limit Theorem for a Class of Linear Systems 1
A Note on the Central Limit Theorem for a Class of Linear Systems 1 Contents Yukio Nagahata Department of Mathematics, Graduate School of Engineering Science Osaka University, Toyonaka 560-8531, Japan.
More informationTHE SUBGAUSSIAN CONSTANT AND CONCENTRATION INEQUALITIES
THE SUBGAUSSIAN CONSTANT AND CONCENTRATION INEQUALITIES S.G. Bobkov, C. Houdré, P. Tetali Abstract We study concentration inequalities for Lipschitz functions on graphs by estimating the optimal constant
More informationThe coupling method - Simons Counting Complexity Bootcamp, 2016
The coupling method - Simons Counting Complexity Bootcamp, 2016 Nayantara Bhatnagar (University of Delaware) Ivona Bezáková (Rochester Institute of Technology) January 26, 2016 Techniques for bounding
More informationADJOINTS, ABSOLUTE VALUES AND POLAR DECOMPOSITIONS
J. OPERATOR THEORY 44(2000), 243 254 c Copyright by Theta, 2000 ADJOINTS, ABSOLUTE VALUES AND POLAR DECOMPOSITIONS DOUGLAS BRIDGES, FRED RICHMAN and PETER SCHUSTER Communicated by William B. Arveson Abstract.
More informationAll Good (Bad) Words Consisting of 5 Blocks
Acta Mathematica Sinica, English Series Jun, 2017, Vol 33, No 6, pp 851 860 Published online: January 25, 2017 DOI: 101007/s10114-017-6134-2 Http://wwwActaMathcom Acta Mathematica Sinica, English Series
More information(somewhat) expanded version of the note in C. R. Acad. Sci. Paris 340, (2005). A (ONE-DIMENSIONAL) FREE BRUNN-MINKOWSKI INEQUALITY
(somewhat expanded version of the note in C. R. Acad. Sci. Paris 340, 30 304 (2005. A (ONE-DIMENSIONAL FREE BRUNN-MINKOWSKI INEQUALITY M. Ledoux University of Toulouse, France Abstract. We present a one-dimensional
More informationTHE NEARLY ADDITIVE MAPS
Bull. Korean Math. Soc. 46 (009), No., pp. 199 07 DOI 10.4134/BKMS.009.46..199 THE NEARLY ADDITIVE MAPS Esmaeeil Ansari-Piri and Nasrin Eghbali Abstract. This note is a verification on the relations between
More informationarxiv: v1 [math.co] 14 Apr 2012
arxiv:1204.3168v1 [math.co] 14 Apr 2012 A brief review on geometry and spectrum of graphs 1 Introduction Yong Lin April 12, 2012 Shing-Tung Yau This is a survey paper. We study the Ricci curvature and
More informationAN INEQUALITY FOR TAIL PROBABILITIES OF MARTINGALES WITH BOUNDED DIFFERENCES
Lithuanian Mathematical Journal, Vol. 4, No. 3, 00 AN INEQUALITY FOR TAIL PROBABILITIES OF MARTINGALES WITH BOUNDED DIFFERENCES V. Bentkus Vilnius Institute of Mathematics and Informatics, Akademijos 4,
More informationMODIFIED LOG-SOBOLEV INEQUALITIES AND ISOPERIMETRY
MODIFIED LOG-SOBOLEV INEQUALITIES AND ISOPERIMETRY ALEXANDER V. KOLESNIKOV Abstract. We find sufficient conditions for a probability measure µ to satisfy an inequality of the type f f f F dµ C f c dµ +
More informationFrom Concentration to Isoperimetry: Semigroup Proofs
Contemporary Mathematics Volume 545, 2011 From Concentration to Isoperimetry: Semigroup Proofs Michel Ledoux Abstract. In a remarkable series of works, E. Milman recently showed how to reverse the usual
More informationConvex decay of Entropy for interacting systems
Convex decay of Entropy for interacting systems Paolo Dai Pra Università degli Studi di Padova Cambridge March 30, 2011 Paolo Dai Pra Convex decay of Entropy for interacting systems Cambridge, 03/11 1
More informationRegularizing objective functionals in semi-supervised learning
Regularizing objective functionals in semi-supervised learning Dejan Slepčev Carnegie Mellon University February 9, 2018 1 / 47 References S,Thorpe, Analysis of p-laplacian regularization in semi-supervised
More informationCharacterization of cutoff for reversible Markov chains
Characterization of cutoff for reversible Markov chains Yuval Peres Joint work with Riddhi Basu and Jonathan Hermon 23 Feb 2015 Joint work with Riddhi Basu and Jonathan Hermon Characterization of cutoff
More informationCentral limit theorems for ergodic continuous-time Markov chains with applications to single birth processes
Front. Math. China 215, 1(4): 933 947 DOI 1.17/s11464-15-488-5 Central limit theorems for ergodic continuous-time Markov chains with applications to single birth processes Yuanyuan LIU 1, Yuhui ZHANG 2
More informationOberwolfach workshop on Combinatorics and Probability
Apr 2009 Oberwolfach workshop on Combinatorics and Probability 1 Describes a sharp transition in the convergence of finite ergodic Markov chains to stationarity. Steady convergence it takes a while to
More informationRichard F. Bass Krzysztof Burdzy University of Washington
ON DOMAIN MONOTONICITY OF THE NEUMANN HEAT KERNEL Richard F. Bass Krzysztof Burdzy University of Washington Abstract. Some examples are given of convex domains for which domain monotonicity of the Neumann
More informationLecture 1 Measure concentration
CSE 29: Learning Theory Fall 2006 Lecture Measure concentration Lecturer: Sanjoy Dasgupta Scribe: Nakul Verma, Aaron Arvey, and Paul Ruvolo. Concentration of measure: examples We start with some examples
More informationThe Logarithmic Sobolev Constant of Some Finite Markov Chains. Wai Wai Liu
CORNELL UNIVERSITY MATHEMATICS DEPARTMENT SENIOR THESIS The Logarithmic Sobolev Constant of Some Finite Markov Chains A THESIS PRESENTED IN PARTIAL FULFILLMENT OF CRITERIA FOR HONORS IN MATHEMATICS Wai
More informationCONCENTRATION OF MEASURE
CONCENTRATION OF MEASURE Nathanaël Berestycki and Richard Nickl with an appendix by Ben Schlein University of Cambridge Version of: December 1, 2009 Contents 1 Introduction 3 1.1 Foreword.................................
More informationJ. Kinnunen and R. Korte, Characterizations of Sobolev inequalities on metric spaces, arxiv: v2 [math.ap] by authors
J. Kinnunen and R. Korte, Characterizations of Sobolev inequalities on metric spaces, arxiv:79.197v2 [math.ap]. 28 by authors CHARACTERIZATIONS OF SOBOLEV INEQUALITIES ON METRIC SPACES JUHA KINNUNEN AND
More informationCurrent; Forest Tree Theorem; Potential Functions and their Bounds
April 13, 2008 Franklin Kenter Current; Forest Tree Theorem; Potential Functions and their Bounds 1 Introduction In this section, we will continue our discussion on current and induced current. Review
More informationNote on the Chen-Lin Result with the Li-Zhang Method
J. Math. Sci. Univ. Tokyo 18 (2011), 429 439. Note on the Chen-Lin Result with the Li-Zhang Method By Samy Skander Bahoura Abstract. We give a new proof of the Chen-Lin result with the method of moving
More informationCLOSED RANGE POSITIVE OPERATORS ON BANACH SPACES
Acta Math. Hungar., 142 (2) (2014), 494 501 DOI: 10.1007/s10474-013-0380-2 First published online December 11, 2013 CLOSED RANGE POSITIVE OPERATORS ON BANACH SPACES ZS. TARCSAY Department of Applied Analysis,
More informationNeighbor Sum Distinguishing Total Colorings of Triangle Free Planar Graphs
Acta Mathematica Sinica, English Series Feb., 2015, Vol. 31, No. 2, pp. 216 224 Published online: January 15, 2015 DOI: 10.1007/s10114-015-4114-y Http://www.ActaMath.com Acta Mathematica Sinica, English
More informationFunctional central limit theorem for super α-stable processes
874 Science in China Ser. A Mathematics 24 Vol. 47 No. 6 874 881 Functional central it theorem for super α-stable processes HONG Wenming Department of Mathematics, Beijing Normal University, Beijing 1875,
More informationAsymptotic stability of an evolutionary nonlinear Boltzmann-type equation
Acta Polytechnica Hungarica Vol. 14, No. 5, 217 Asymptotic stability of an evolutionary nonlinear Boltzmann-type equation Roksana Brodnicka, Henryk Gacki Institute of Mathematics, University of Silesia
More informationOn metric characterizations of some classes of Banach spaces
On metric characterizations of some classes of Banach spaces Mikhail I. Ostrovskii January 12, 2011 Abstract. The first part of the paper is devoted to metric characterizations of Banach spaces with no
More informationTRANSPORT INEQUALITIES FOR STOCHASTIC
TRANSPORT INEQUALITIES FOR STOCHASTIC PROCESSES Soumik Pal University of Washington, Seattle Jun 6, 2012 INTRODUCTION Three problems about rank-based processes THE ATLAS MODEL Define ranks: x (1) x (2)...
More informationEntropy and Ergodic Theory Lecture 15: A first look at concentration
Entropy and Ergodic Theory Lecture 15: A first look at concentration 1 Introduction to concentration Let X 1, X 2,... be i.i.d. R-valued RVs with common distribution µ, and suppose for simplicity that
More informationPoincaré Inequalities and Moment Maps
Tel-Aviv University Analysis Seminar at the Technion, Haifa, March 2012 Poincaré-type inequalities Poincaré-type inequalities (in this lecture): Bounds for the variance of a function in terms of the gradient.
More informationIndependence of some multiple Poisson stochastic integrals with variable-sign kernels
Independence of some multiple Poisson stochastic integrals with variable-sign kernels Nicolas Privault Division of Mathematical Sciences School of Physical and Mathematical Sciences Nanyang Technological
More informationVertex and edge expansion properties for rapid mixing
Vertex and edge expansion properties for rapid mixing Ravi Montenegro Abstract We show a strict hierarchy among various edge and vertex expansion properties of Markov chains. This gives easy proofs of
More informationStepanov s Theorem in Wiener spaces
Stepanov s Theorem in Wiener spaces Luigi Ambrosio Classe di Scienze Scuola Normale Superiore Piazza Cavalieri 7 56100 Pisa, Italy e-mail: l.ambrosio@sns.it Estibalitz Durand-Cartagena Departamento de
More informationPseudo-Boolean Functions, Lovász Extensions, and Beta Distributions
Pseudo-Boolean Functions, Lovász Extensions, and Beta Distributions Guoli Ding R. F. Lax Department of Mathematics, LSU, Baton Rouge, LA 783 Abstract Let f : {,1} n R be a pseudo-boolean function and let
More informationRecent developments in elliptic partial differential equations of Monge Ampère type
Recent developments in elliptic partial differential equations of Monge Ampère type Neil S. Trudinger Abstract. In conjunction with applications to optimal transportation and conformal geometry, there
More informationConstructive proof of deficiency theorem of (g, f)-factor
SCIENCE CHINA Mathematics. ARTICLES. doi: 10.1007/s11425-010-0079-6 Constructive proof of deficiency theorem of (g, f)-factor LU HongLiang 1, & YU QingLin 2 1 Center for Combinatorics, LPMC, Nankai University,
More informationTHE SET OF RECURRENT POINTS OF A CONTINUOUS SELF-MAP ON AN INTERVAL AND STRONG CHAOS
J. Appl. Math. & Computing Vol. 4(2004), No. - 2, pp. 277-288 THE SET OF RECURRENT POINTS OF A CONTINUOUS SELF-MAP ON AN INTERVAL AND STRONG CHAOS LIDONG WANG, GONGFU LIAO, ZHENYAN CHU AND XIAODONG DUAN
More information