Concentration Properties of Restricted Measures with Applications to Non-Lipschitz Functions

Size: px
Start display at page:

Download "Concentration Properties of Restricted Measures with Applications to Non-Lipschitz Functions"

Transcription

1 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 Subgaussian constant, spread constant, restricted measures, concentration of measure Abstract For any metric probability space (M, d, µ, with a subgaussian constant σ (µ and any Borel measurable set A M, we show that σ (µ A c log (e/ σ (µ, where µ A is a normalized restriction of µ to the set A and c is a universal constant As a consequence, we deduce concentration inequalities for non-lipschitz functions Introduction It is known that many high-dimensional probability distributions µ on the Euclidean space R n (and other metric spaces, including graphs possess strong concentration properties In a functional language, this may informally be stated as the assertion that any sufficiently smooth function f on R n, eg, having a bounded Lipschitz semi-norm, is almost a constant on almost all space There are several ways to quantify such a property One natural approach proposed by N Alon, R Boppana and J Spencer [A-B-S] associates, with a given metric probability space (M, d, µ, its spread constant, s (µ = sup Var µ (f = sup (f m dµ, where m = f dµ, and the sup is taken over all functions f on M with f Lip More information is contained in the so-called subgaussian constant σ = σ (µ which is defined as the infimum over all σ such that e tf dµ e σ t /, for all t R, ( in the class L of all f on M with m = and f Lip (cf [B-G-H] Describing the diameter of L in the Orlicz space L ψ (µ for the Young function ψ (t = e t (within School of Mathematics, University of Minnesota, Minneapolis, MN 55455; research supported in part by the Humboldt Foundation, NSF and BSF grants Institute of Mathematics & Applications, Minneapolis, MN 55455; address: nayar@mimuwedupl (corresponding author; research supported in part by NCN grant DEC-/5/B/ST/4 School of Mathematics and School of Computer Science, Georgia Institute of Technology, Atlanta, GA 333; research supported in part by NSF DMS-47657

2 universal factors, the quantity σ (µ appears as a parameter in a subgaussian concentration inequality for the class of all Borel subsets of M As an equivalent approach, it may also be introduced via the transport-entropy inequality connecting the classical Kantorovich distance and the relative entropy from an arbitrary probability measure on M to the measure µ (cf [B-G] While in general s σ, the latter characteristic allows one to control subgaussian tails under the probability measure µ uniformly in the entire class of Lipschitz functions on M More generally, when f Lip L, ( yields µ{ f m t} e t /(σ L, t > ( Classical and well-known examples include the standard Gaussian measure on M = R n in which case s = σ =, and the normalized Lebesgue measure on the unit sphere M = S n with s = σ = n The last example was a starting point in the study of the concentration of measure phenomena, a fruitful direction initiated in the early 97s by V D Milman Other examples come often after verification that µ satisfies certain Sobolev-type inequalities such as Poincaré-type inequalities λ Var µ (u u dµ, and logarithmic Sobolev inequalities [ ρ Ent µ (u = ρ u log u dµ u dµ log ] u dµ u dµ, where u may be any locally Lipschitz function on M, and the constants λ > and ρ > do not depend on u Here the modulus of the gradient may be understood in the generalized sense as the function u(x = lim sup y x u(x u(y, x M d(x, y (this is the so-called continuous setting, while in the discrete spaces, eg, graphs, we deal with other naturally defined gradients In both cases, one has respectively the well-known upper bounds s (µ λ, σ (µ ρ (3 For example, λ = ρ = n on the unit sphere (best possible values, [M-W], which can be used to make a corresponding statement about the spread and Gaussian constants One of the purposes of this note is to give new examples by involving the family of normalized restricted measures µ A (B = µ(a B, B M (Borel, where a Borel measurable set A M is fixed and has a positive measure As an example, returning to the standard Gaussian measure µ on R n, it is known that σ (µ A for any convex body A R n This remarkable property, discovered by D Bakry and M Ledoux [B-L] in a sharper form of a Gaussian-type isoperimetric inequality, has nowadays several proofs and generalizations, cf [B, B] Of course, in general, the set A may have a rather disordered structure, for instance, to be disconnected And then there is no hope for validity of a Poincaré-type inequality for the measure µ A Nevertheless, it turns out that the concentration property of µ A is inherited from µ, unless the measure of A is too small In particular, we have the following observation about abstract metric probability spaces

3 3 Theorem For any measurable set A M with >, the subgaussian constant σ (µ A of the normalized restricted measure satisfies σ (µ A c log σ (µ, (4 where c is an absolute constant Although this assertion is technically simple, we will describe two approaches: one is direct and refers to estimates on the ψ -norms over the restricted measures, and the other one uses a general comparison result due to F Barthe and E Milman on the concentration functions ([B-M] One may further generalize Theorem by defining the subgaussian constant σf (µ within a given fixed subclass F of functions on M, by using the same bound ( on the Laplace transform This is motivated by a possible different level of concentration for different classes; indeed, in case of M = R n, the concentration property may considerably be strengthened for the class F of all convex Lipschitz functions In particular, one result of M Talagrand [T, T] provides a dimension-free bound σf (µ C for an arbitrary product probability measure µ on the n-dimensional cube [, ] n Hence, a more general version of Theorem yields the bound σf(µ A c log with some absolute constant c, which holds for any Borel subset A of [, ] n (cf Section 6 below According to the very definition, the quantities σ (µ and σ (µ A might seem responsible for deviations of only Lipschitz functions f on M and A, respectively However, the inequality (4 may also be used to control deviations of non-lipschitz f on large parts of the space and under certain regularity hypotheses Assume, for example, f dµ (which is kind of a normalization condition and consider A = {x M : f(x L} (5 If L, this set has the measure L, and hence, σ (µ A cσ (µ with some absolute constant c If we assume that f has a Lipschitz semi-norm L on A, then, according to (, µ A {x A : f m t} e t /(cσ (µl, t >, (6 where m is the mean of f with respect to µ A It is in this sense one may say that f is almost a constant on the set A This also yields a corresponding deviation bound on the whole space, µ{x M : f m t} e t /cσ (µl + L Stronger integrability conditions posed on f can considerably sharpen the conclusion By a similar argument, Theorem yields, for example, the following exponential bound, known in the presence of a logarithmic Sobolev inequality for the space (M, d, µ, and with σ replaced by /ρ (cf [B-G] Corollary Let f be a locally Lipschitz function on M with Lipschitz semi-norms L on the sets (5 If e f dµ, then f is µ-integrable, and moreover, µ{x M : f m t} e t/cσ(µ, t >, where m is the µ-mean of f and c is an absolute constant

4 4 Equivalently (up to an absolute factor, we have a Sobolev-type inequality f m ψ cσ(µ f ψ, connecting the ψ -norm of f m with the ψ -norm of the modulus of the gradient of f We prove a more general version of this corollary in Section 6 (cf Theorem 6 As will be explained in the same section, similar assertions may also be made about convex f and product measures µ on M = [, ] n, thus extending Talagrand s theorem to the class of non-lipschitz functions In view of the right bound in (3 and (4, the spread and subgaussian constants for restricted measures can be controlled in terms of the logarithmic Sobolev constant ρ, via s (µ A σ (µ A c log ρ However, it may happen that ρ = and σ (µ =, while λ > (eg, for the product exponential distribution on R n Then one may wonder whether one can estimate the spread constant of a restricted measure in terms of the spectral gap In such a case there is a bound similar to (4 Theorem 3 Assume the metric probability space (M, d, µ satisfies a Poincaré-type inequality with λ > For any A M with >, with some absolute constant c ( s (µ A c log e (7 λ It should be mentioned that the logarithmic terms in (4 and (7 may not be removed and are actually asymptotically optimal as functions of, as is getting small, see Section 7 Our contribution below is organized into sections as follows: Bounds on ψ α -norms for restricted measures 3 Proof of Theorem Transport-entropy formulation 4 Proof of Theorem 3 Spectral gap 5 Examples 6 Deviations for non-lipschitz functions 7 Optimality 8 Appendix Bounds on ψ α -norms for restricted measures A measurable function f on the probability space (M, µ is said to have a finite ψ α -norm, α, if for some r >, e ( f /rα dµ The infimum over all such r represents the ψ α -norm f ψα or f L ψα (µ, which is just the Orlicz norm associated with the Young function ψ α (t = e t α We are mostly interested in the particular cases α = and α = In this section we recall well-known relations between the ψ and ψ -norms and the usual L p -norms f p = f L p (µ = ( f p dµ /p For the readers convenience, we include the proof in the appendix Lemma We have f p f p sup f p p L ψ (µ 4 sup, ( p p

5 5 f p f p sup f p p L ψ (µ 6 sup p p ( Given a measurable subset A of M with >, we consider the normalized restricted measure µ A on M, ie, µ(a B µ A (B =, B M Our basic tool leading to Theorem will be the following assertion Proposition For any measurable function f on M, ( f L ψ (µa 4e log / e f L ψ (µ (3 Proof Assume that f L ψ (µ = and fix p By the left inequality in (, for any q, q q/ f q dµ f q dµ A, so But by the right inequality in (, f L q (µ A q ( /q f ψ f q 4 sup q q 4 f q p sup q p q Applying it on the space (M, µ A, we then get The obtained inequality, f L ψ (µa 4 f L p sup q (µ A q p q 4 p sup q p ( /q = 4 ( /p p f L ψ (µa 4 ( /p p, holds true for any p and therefore may be optimized over p Choosing p = log e, we arrive at (3 A possible weak point in the bound (3 is that the means of f are not involved For example, in applications, if f were defined only on A and had µ A -mean zero, we might need to find an extension of f to the whole space M keeping the mean zero with respect to µ In fact, this should not create any difficulty, since one may work with the symmetrization of f More precisely, we may apply Proposition on the product space (M M, µ µ to the product sets A A and functions of the form f(x f(y Then we get ( e f(x f(y L ψ (µa µ A 4e log / f(x f(y L ψ (µ µ Since log ( ( e log e, we arrive at: Corollary 3 For any measurable function f on M, f(x f(y L ψ (µa µ A 4e ( log / e f(x f(y L ψ (µ µ

6 6 Let us now derive an analog of Proposition for the ψ -norm, using similar arguments Assume that f L ψ (µ = and fix p By the left inequality in (, for any q, q q f q dµ f q dµ A, so But, by the inequality (, f L q (µ A q ( /q f L ψ f q 6 sup q q 6p sup q p f q q Applying it on the space (M, µ A, we get The obtained inequality, f Lq (µ f L ψ (µa 6p sup A q p q 6p sup q p ( ( /p, f L ψ (µa 6p /q ( /p = 6p holds true for any p and therefore may be optimized over p Choosing p = log e, we arrive at: Proposition 4 For any measurable function f on M, we have f L ψ (µa 6e log f L ψ (µ Similarly to Corollary 3, one may write down this relation on the product probability space (M M, µ µ with functions of the form f(x, y = f(x f(y and the product sets à = A A Then we get f(x f(y L ψ (µa µ A e log f(x f(y L ψ (µ µ (4 3 Proof of Theorem Transport-entropy formulation The finiteness of the subgaussian constant for a given metric probability space (M, d, µ means that ψ -norms of Lipschitz functions on M with mean zero are uniformly bounded Equivalently, for any (for all x M, we have that, for some λ >, e d(x,x /λ dµ(x < Definition ( of σ (µ inspires to consider another norm-like quantity [ ] σf = sup t t / log e tf dµ Here is a well-known relation (with explicit numerical constants which holds in the setting of an abstract probability space (M, µ Once again, we include a proof in the appendix for completeness

7 7 Lemma 3 If f has mean zero and finite ψ -norm, then 6 f ψ σ f 4 f ψ One can now relate the subgaussian constant of the restricted measure to the subgaussian constant of the original measure Let now (M, d, µ be a metric probability space First, Lemma 3 immediately yields an equivalent description in terms of ψ -norms, namely sup f ψ 6 f σ (µ 4 sup f ψ, (3 f where the supremum is running over all f : M R with µ-mean zero and f Lip Here, one can get rid of the mean zero assumption by considering functions of the form f(x f(y on the product space (M M, µ µ, d, where d is the l -type metric given by d ((x, y, (x, y = d(x, x + d(y, y If f has mean zero, then, by Jensen s inequality, e (f(x f(y /r dµ(x dµ(y e f(x /r dµ(x, which implies that f(x f(y L ψ (µ µ f L ψ (µ On the other hand, by the triangle inequality, f(x f(y L ψ (µ µ f L ψ (µ Hence, we arrive at another, more flexible relation, where the mean zero assumption may be removed Lemma 3 We have 4 6 sup f(x f(y L ψ (µ µ σ (µ 4 sup f(x f(y L ψ (µ µ, f f where the supremum is running over all functions f on M with f Lip Proof of Theorem We are prepared to make last steps for the proof of the inequality (4 We use the well-known Kirszbraun s theorem: Any function f : A R with Lipschitz semi-norm f Lip on A admits a Lipschitz extension to the whole space ([K], [MS] Namely, one may put [ ] f(x = inf f(a + d(a, x, x M a A Applying first Corollary 3 and then the left inequality of Lemma 3 to f, we get f(x f(y L ψ (µ A µ A = f(x f(y L ψ (µ A µ A ( 4e ( e log ( 4e ( e log f(x f(y L ψ (µ µ (4 6 σ (µ Another application of Lemma 3 in the space (A, d, µ A (now the right inequality yields σ (µ A 4 (4e ( e log (4 6 σ (µ This is exactly (4 with constant c = 4 (4e (4 6 = 3 e = 97967

8 8 Remark 33 Let us also record the following natural generalization of Theorem, which is obtained along the same arguments Given a collection F of (integrable functions on the probability space (M, µ, define σ F (µ as the infimum over all σ such that e t(f m dµ e σ t /, for all t R, for any f F, where m = f dµ Then with the same constant c as in Theorem, for any measurable A M, >, we have σf A (µ A c log σ F(µ, where F A denotes the collection of restrictions of functions f from F to the set A Let us now mention an interesting connection of the subgaussian constant with the Kantorovich distance W (µ, ν = inf d(x, y π(x, y and relative entropy D(ν µ = log dν dµ dν, (also called Kullback-Leibler distance or informational divergence Here, ν is a probability measure on M, which is absolutely continuous with respect to µ (for short, ν << µ, and the infimum in the definition of W is running over all probability measures π on the product space M M with marginal distributions µ and ν, ie, such that π(b M = µ(b, π(m B = ν(b (Borel B M As was shown in [B-G], if (M, d is a Polish space (complete separable, the subgaussian constant σ = σ (µ may be described as an optimal value in the transport-entropy inequality W (µ, ν σ D(ν µ (3 Hence, we obtain from the inequality (4 a similar relation for measures ν supported on given subsets of M Corollary 34 Given a Borel probability measure µ on a Polish space (M, d and a closed set A in M such that >, for any Borel probability measure ν supported on A, W (µ A, ν cσ (µ log D(ν µ A, where c is an absolute constant This assertion is actually equivalent to Theorem Note that, for ν supported on A, there is an identity D(ν µ A = log + D(ν µ In particular, D(ν µ A D(ν µ, so the relative entropies decrease when turning to restricted measures For another (almost equivalent description of the subgaussian constant, introduce the concentration function K µ (r = sup [ µ(a r ] (r >, where A r = {x M : d(x, a < r for some a A} denotes an open r-neighbourhood of A for the metric d, and the sup is running over all Borel sets A M of measure As is well-known, the transport-entropy inequality (3 gives rise to a concentration inequality

9 9 on (M, d, µ of a subgaussian type (K Marton s argument, but this can also be seen by a direct application of ( Indeed, for any function f on M with f Lip, it implies e t(f(x f(y dµ(x dµ(y e σ t, t R, and, by Chebyshev s inequality, we have a deviation bound (µ µ{(x, y M M : f(x f(y r} e r /4σ, r In particular, one may apply it to the distance functions f(x = d(a, x = inf a A d(a, x Assuming that, the measure on the left-hand side is greater than or equal to ( µ(ar, so that we obtain a concentration inequality µ(a r e r /4σ Therefore, K µ (r min {, e r /4σ } e r /8σ To argue in the opposite direction, suppose that the concentration function admits a bound of the form K µ (r e r /b for all r > with some constant b > Given a function f on M with f Lip, let m be a median of f under µ Then the set A = {f m} has measure, and by the Lipschitz property, Ar {f < m + r} for all r > Hence, by the concentration hypothesis, µ{f m r} K µ (r e r /b A similar deviation bound also holds for the function f with its median m, so that µ{ f m r} e r /b, r > This is sufficient to properly estimate ψ -norm of f m on (M, µ Namely, for any λ < /b, e λ f m dµ = + λ re λr µ{ f m r} dr + λ re λr e r /b dr = + λ b λ =, where in the last equality the value λ = 3b is chosen Thus, e f m /(3b dµ, which means that f m ψ 3 b The latter gives f(x f(y L ψ (µ µ 3 b Taking the supremum over f, it remains to apply Lemma 3, and then we get σ (µ 48 b Let us summarize Proposition 35 Let b = b(µ be an optimal value such that the concentration function of the space (M, d, µ satisfies a subgaussian bound K µ (r e r /b (r > Then 8 b (µ σ (µ 48 b (µ Once this description of the subgaussian constant is recognized, one may give another proof of Theorem, by relating the concentration function K µa to K µ In this connection let us state below, as a lemma, a general observation due to F Barthe and E Milman (cf [B-M], Lemma, p 585

10 Lemma 36 Let a Borel probability measure ν on M be absolutely continuous with respect to µ and have density p Suppose that, for some right-continuous, non-increasing function R : (, /4] (,, such that β(ε = ε/r(ε is increasing, we have ν{x M : p(x > R(ε} ε ( < ε 4 Then K ν (r β ( K µ (r/, for all r K µ (β(/4 Here β denotes the inverse function, and K µ (ε = inf{r > : K µ (r < ε} The nd proof of Theorem The normalized restricted measure ν = µ A has density p = A (thus taking only one non-zero value, and an optimal choice of R is the constant function R(ε = Hence, Lemma 36 yields the relation K µa (r K µ(r/, for r K µ (/4 In particular, if K µ (r e r /b, then K µa (r e r /(4b, for r b log(4/ Necessarily K µa (r, so the last relation may be extended to the whole positive half-axis Moreover, at the expense of a factor in the exponent, one can remove the factor ; more precisely, we get K µa (r e r / b with b = 4b log log 4, that is, b (µ A 4 log log 4 b (µ It remains to apply the two-sided bound of Proposition 35 4 Proof of Theorem 3 Spectral gap Theorem insures, in particular, that, for any function f on the metric probability space (M, d, µ with Lipschitz semi-norm f Lip, ( e Var µa (f c log σ (µ, up to some absolute constant c In fact, in order to reach a similar concentration property of the restricted measures, it is enough to start with a Poincaré-type inequality on M, λ Var µ (f f dµ Under this hypothesis, a well-known theorem due to Gromov-Milman and Borovkov-Utev asserts that mean zero Lipschitz functions f have bounded ψ -norm One may use a variant of this theorem proposed by Aida and Strook [A-S], who showed that e λ f dµ K = 7 ( f Lip

11 Hence e λ f dµ K and e λ f dµ K <, thus implying that f ψ λ In addition, e λ (f(x f(y dµ(xdµ(y K and e λ f(x f(y dµ(xdµ(y K < 6 From this, e 3 λ f(x f(y dµ(xdµ(y < 6 /3 <, which means that f(x f(y ψ 3 λ with respect to the product measure µ µ on the product space M M This inequality is translation invariant, so the mean zero assumption may be removed Thus, we arrive at: Lemma 4 Under the Poincaré-type inequality with spectral gap λ >, for any mean zero function f on (M, d, µ with f Lip, f ψ λ Moreover, for any f with f Lip, f(x f(y L ψ (µ µ 3 λ (4 This is a version of the concentration of measure phenomenon (with exponential integrability in the presence of a Poincaré-type inequality Our goal is therefore to extend this property to the normalized restricted measures µ A This can be achieved by virtue of the inequality (4 which when combined with (4 yields an upper bound ( e f(x f(y L ψ (µa µ A 36 e log λ Moreover, if f has µ A -mean zero, the left norm dominates f L ψ (µa (by Jensen s inequality We can summarize, taking into account once again Kirszbraun s theorem, as we did in the proof of Theorem Proposition 4 Assume the metric probability space (M, d, µ satisfies a Poincaré-type inequality with constant λ > Given a measurable set A M with >, for any function f : A R with µ A -mean zero and such that f Lip on A, f L ψ (µa 36 e log λ Theorem 3 is now easily obtained with the constant c = (36e, by noting that L - norms are dominated by L ψ -norms More precisely, since e t t, one has f ψ f Remark 43 Related stability results are known for various classes of probability distributions on the Euclidean spaces M = R n (and even in a more general stituation, where µ A is replaced by an absolutely continuous measure with respect to µ See, in particular, the works by E Milman [Mi,Mi] on convex bodies and log-concave measures

12 5 Examples Theorems and 3 involve a lot of interesting examples Here are some natural ones The standard Gaussian measure µ = γ on R n satisfies a logarithmic Sobolev inequality on M = R n with a dimension-free constant ρ = Hence, from Theorem we get: Corollary 5 For any measurable set A R n with γ(a >, the subgaussian constant σ (γ A of the normalized restricted measure γ A satisfies σ (γ A c log, γ(a where c is an absolute constant As it was already mentioned, if A is convex, there is a sharper bound σ (γ A However, it may not hold without convexity assumption Nevertheless, if γ(a is bounded away from zero, we obtain a more universal principle Clearly, Corollary 5 extends to all product measures µ = ν n on R n such that ν satisfies a logarithmic Sobolev inequality on the real line, and with constants c depending on ρ, only A characterization of the property ρ > in terms of the distribution function of the measure ν and the density of its absolutely continuous component may be found in [B-G] Consider a uniform distribution ν on the shell A ε = { x R n : ε x }, ε (n Corollary 5 The subgaussian constant of ν satisfies σ (ν c n, up to some absolute constant c In other words, mean zero Lipschitz functions f on A ε are such that n f are subgaussian with universal constant factor This property is well-known in the extreme cases on the unit Euclidean ball A = B n (ε = and on the unit sphere A = S n (ε = Let µ denote the normalized Lebesgue measure on B n In the case ε n, the shell A ε represents the part of B n of measure ( µ(a ε = n n e Since the logarithmic Sobolev constant of the unit ball is of order n, and therefore σ (µ c n, the assertion of Corollary 5 immediately follows from Theorem In case ε n, the assertion follows from a similar concentration property of the uniform distribution σ n on the unit sphere Indeed, with every Lipschitz function f on A ε one may associate its restriction to S n, which is also Lipschitz (with respect to the Euclidean distance We have f(rθ f(θ r ε n, for any r [ ε, ] and θ Sn Hence, f(r θ f(rθ f(θ f(θ + f(r θ f(θ + f(rθ f(θ f(θ f(θ + n, whenever r, r [ ε, ] and θ, θ S n, which implies f(r θ f(rθ f(θ f(θ + 8 n

13 3 But the map (r, θ θ pushes forward ν onto σ n, so, we obtain that, for any c >, exp{cn f(r θ f(rθ } dν(r, θ dν(r, θ e 8/n exp{cn f(θ f(θ } dσ n (θ dσ n (θ Here, for a certain numerical constant c >, the right-hand side is bounded by a universal constant, thus proving the claim 3 The two-sided product exponential measure µ on R n with density n e ( x + + xn satisfies a Poincaré-type inequality on M = R n with a dimension-free constant λ = /4 Hence, from Proposition 4 we get: Corollary 53 For any measurable set A R n with >, and for any function f : A R with µ A -mean zero and f Lip, we have f L ψ (µa c log, where c is an absolute constant In particular, ( s (µ A c log e Clearly, Corollary 53 extends to all product measures µ = ν n on R n such that ν satisfies a Poincaré-type inequality on the real line, and with constants c depending on λ, only A characterization of the property λ > may also be given in terms of the distribution function of ν and the density of its absolutely continuous component (cf [B-G] 4a Let us take the metric probability space ({, } n, d n, µ, where d n is the Hamming distance, that is, d n (x, y = {i : x i y i }, equipped with the uniform measure µ For this particular space, Marton established the transport-entropy inequality (3 with an optimal constant σ = n 4, cf [Mar] Using the relation (3 as an equivalent definition of the subgaussian constant, we obtain from Theorem : Corollary 54 For any non-empty set A {, } n, the subgaussian constant σ (µ A of the normalized restricted measure µ A satisfies, up to an absolute constant c, σ (µ A cn log (5 4b Let us now assume that A is monotone, ie, A satisfies the condition (x,, x n A = (y,, y n A, whenever y i x i, i =,, n Recall that the discrete cube can be equipped with a natural graph structure: there is an edge between x and y whenever they are of Hamming distance d n (x, y = For monotone sets A, the graph metric d A on the subgraph of A is equal to the restriction of d n to A A Indeed, we have: d n (x, y d A (x, y d A (x, x y + d A (y, x y = d n (x, x y + d n (y, x y = d n (x, y, where x y = (x y,, x n y n Thus, s (µ A, d A σ (µ A, d A cn log ( e

14 4 This can be compared with what follows from a recent result of Ding and Mossel (see [D-M] The authors proved that the conductance (Cheeger constant of (A, µ A satisfies φ(a 6n However, these type of isoperimetric results may not imply sharp concentration bounds Indeed, by using Cheeger inequality, the above inequality leads to λ c /n and s (µ A, d A /λ cn /, which is even worse than the trivial estimate s (µ A, d A diam(a n / 5 Let (M, d, µ be a (separable metric probability space with finite subgaussian constant σ (µ The previous example can be naturally generalized to the product space (M n, µ n, when it is equipped with the l -type metric n d n (x, y = d(x i, y i, x = (x,, x n, y = (y,, y n M n i= This can be done with the help of the following elementary observation Proposition 55 The subgaussian constant of the space (M n, d n, µ n is related to the subgaussian constant of (M, d, µ by the equality σ (µ n = nσ (µ Indeed, one may argue by induction on n Let f be a function on M n The Lipschitz property f Lip with respect to d n is equivalent to the assertion that f is coordinatewise Lipschitz, that is, any function of the form x i f(x has a Lipschitz semi-norm on M for all fixed coordinates x j M (j i Hence, in this case, for all t R, M e tf(x dµ(x n exp { t M f(x dµ(x n + σ t where σ = σ (µ Here the function (x,, x n M f(x dµ(x n is also coordinatewise Lipschitz Integrating the above inequality with respect to dµ n (x,, x n and applying the induction hypothesis, we thus get M n e tf(x dµ n (x exp { t }, M n f(x dµ n (x + n σ t But this means that σ (µ n nσ (µ For an opposite bound, it is sufficient to test ( for (M n, d n, µ n in the class of all coordinatewise Lipschitz functions of the form f(x = u(x + + u(x n with µ-mean zero functions u on M such that u Lip Corollary 56 For any Borel set A M n such that µ n (A >, the subgaussian constant of the normalized restricted measure µ n A with respect to the l -type metric d n satisfies ( σ (µ n A cnσ e (µ log µ n, (A where c is an absolute constant For example, if µ is a probability measure on M = R such that /λ dµ(x ex (λ >, then for the restricted product measures we have ( σ (µ n A cnλ e log µ n (5 (A with respect to the l -norm x = x + + x n on R n Indeed, by the integral hypothesis on µ, for any f on R with f Lip, e (f(x f(y /λ dµ(xdµ(y } e (x y /λ dµ(xdµ(y e (x +y /λ dµ(xdµ(y 4

15 5 Hence, if f has µ-mean zero, by Jensen s inequality, e f(x /4λ dµ(x e (f(x f(y /4λ dµ(xdµ(y, meaning that f L ψ (µ λ By Lemma 3, cf (3, it follows that σ (µ 6λ, so, (5 holds true by an application of Corollary 56 6 Deviations for non-lipschitz functions Let us now turn to the interesting question on the relationship between the distribution of a locally Lipschitz function and the distribution of its modulus of the gradient We still keep the setting of a metric probability space (M, d, µ and assume it has a finite subgaussian constant σ = σ (µ (σ Let us say that a continuous function f on M is locally Lipschitz, if f(x is finite for all x M Recall that we consider the sets A = {x M : f(x L}, L > (6 First we state a more general version of Corollary Theorem 6 Assume that a locally Lipschitz function f on M has Lipschitz semi-norms L on sets of the form (6 If µ{ f L }, then for all t >, (µ µ { f(x f(y t } [ inf e t /cσ L + µ { f > L }], (6 L L where c is an absolute constant Proof Although the argument is already mentioned in Section, let us replace (6 with a slightly different bound First note that the Lipschitz semi-norm of f with respect to the metric d in M is the same as its Lipschitz semi-norm with respect to the metric on the set A induced from M (which is true for any non-empty subset of M Hence, we are in a position to apply Theorem, and then Definition ( for the normalized restriction µ A yields a subgaussian bound: e t(f(x f(y dµ A (xdµ A (y e cσ L t /, for all t R, where A is defined in (6 with L L, and c is a universal constant From this, for any t >, (µ A µ A {(x, y A A : f(x f(y t} e t /(cσ L, and therefore (µ µ {(x, y A A : f(x f(y t} e t /(cσ L The product measure of the complement of A A does not exceed µ{ f(x > L}, and we obtain (6 If e f dµ, we have, by Chebyshev s inequality, µ{ f L} e L, so one may take L = log 4 Theorem 6 then gives that, for any L log 4, (µ µ { f(x f(y t } e t /cσ L + 4e L

16 6 For t σ, one may choose here L = t σ, leading to (µ µ { f(x f(y t } 6 e t/cσ, for some absolute constant c > In case t σ, this inequality is fulfilled automatically, so it holds for all t As a result, with some absolute constant C, f(x f(y ψ Cσ, which is an equivalent way to state the inequality of Corollary As we have already mentioned, with the same arguments inequalities like (6 can be derived on the basis of subgaussian constants defined for different classes of functions For example, one may consider the subgaussian constant σf (µ for the class F of all convex Lipschitz functions f on the Euclidean space M = R n (which we equip with the Euclidean distance Note that f(x is everywhere finite in the n-space, when f is convex Keeping in mind Remark 43, what we need is the following analog of Kirszbraun s theorem: Lemma 6 Let f be a convex function on R n For any L >, there exists a convex function g on R n such that f = g on the set A = {x : f(x L} and g L on R n Accepting for a moment this lemma without proof, we get: Theorem 63 Assume that a convex function f on R n satisfies µ{ f L } Then for all t >, (µ µ { f(x f(y t } [ inf e t /cσ L + µ { f > L }], L L where σ = σf (µ and c is an absolute constant For illustration, let µ = µ µ n be an arbitrary product probability measure on the cube [, ] n If f is convex and Lipschitz on R n, thus with f, then (µ µ { f(x f(y t } e t /c (63 This is one of the forms of Talagrand s concentration phenomenon for the family of convex sets/functions (cf [T, T], [M], [L] That is, the subgaussian constants σf (µ are bounded for the class F of convex Lipschitz f and product measures µ on the cube Hence, using Theorem 63, Talagrand s deviation inequality (63 admits a natural extension to the class of non-lipschitz convex functions: Corollary 64 Let µ be a product probability measure on the cube, and let f be a convex function on R n If µ{ f L }, then for all t >, (µ µ { f(x f(y t } [ inf e t /cl + µ { f > L }], L L where c is an absolute constant In particular, we have a statement similar to Corollary for this family of functions, namely f m L ψ (µ c f L ψ (µ, where m is the µ-mean of f Proof of Lemma 6 An affine function l a,v (x = a + x, v (v R n, a R may be called a tangent function to f, if f l on R n and f(x = l a,v (x for at least one point x It is well-known that f(x = sup{l a,v (x : l a,v L},

17 7 where L denotes the collection of all tangent functions l a,v Put, g(x = sup{l a,v (x : l a,v L, v L} By the construction, g f on R n and, moreover, g Lip sup{ l a,v Lip : l a,v L, v L} = sup{ v : l a,v L, v L} L It remains to show that g = f on the set A = { f L} Let x A and let l a,v be tangent to f and such that l a,v (x = f(x This implies that f(y f(x y x, v for all y R n and hence f(x = lim sup y x f(y f(x y x Thus, v L, so that g(x l a,v (x = f(x 7 Optimality lim sup y x y x, v y x = v Here we show that the logarithmic dependence in in Theorems and 3 is optimal, up to the universal constant c We provide several examples Example Let us return to Example 4, Section 5, of the discrete hypercube M = {, } n, which we equip with the Hamming distance d n and the uniform measure µ Let us test the inequality (5 of Corollary 54 on the set A {, } n consisting of n + points (,,,,, (,,,,, (,,,,,, (,,,, We have = (n + / n / n The function f : A R, defined by f(x = {i : x i = } n, has a Lipschitz semi-norm f Lip with respect to d and the µ A -mean zero Moreover, f dµ A = n(n+ Expanding the inequality e tf dµ A e σ (µ A t / at the origin yields f dµ A σ (µ A Hence, recalling that σ (µ n 4, we get σ (µ A f dµ A n n ( 3 σ (µ 3 log σ (µ log This example shows the optimality of (5 in the regime Example Let γ n be the standard Gaussian measure on R n of dimension n We have σ (γ n = Consider the normalized measure γ AR on the set A R = { (x, x,, x n R n : x + x R }, R Using the property that the function (x + x has a standard exponential distribution under the measure γ n, we find that γ n (A R = e R / Moreover, s (γ AR Var γar (x = x dγ AR (x = (x + x dγ AR (x ( = re r dr = R e R / R / + = log e γ n (A R

18 8 Therefore, ( σ (γ AR s (γ AR log e γ n (A R showing that the inequality (4 of Theorem is optimal, up to the universal constant, for any value of γ n (A [, ] Example 3 A similar conclusion can be made about the uniform probability measure µ on the Euclidean ball B(, n of radius n, centred at the origin (asymptotically for growing dimension n To see this, it is sufficient to consider the cylinders A ε = { (x, y R R n : x n ε and y ε }, < ε n, and the function f(x = x We leave to the readers the corresponding computations Example 4 Let µ be the two-sided exponential measure on R with density e x In this case σ (µ =, but, as easy to see, s (µ 4 (recall that λ (µ = 4 We are going to test optimality of the inequality (7 on the sets A R = {x R : x R} (R Clearly, µ(a R = e R, and we find that Therefore, s (µ AR Var µar (x = x dµ AR (x = e R, R r e r dr = R + R + (R + = log µ(a R ( s (µ AR log e, µ(a R showing that the inequality (7 is optimal, up to the universal constant, for any value of (, ] Acknowledgment The authors gratefully acknowledge the support and hospitality of the Institute for Mathematics & Applications (IMA, and the University of Minnesota, Minneapolis, where much of this work was conducted The second named author would like to acknowledge the hospitality of the Georgia Institute of Technology, Atlanta, during the period /8-3/5 References [A-S] Aida, S; Strook, D Moment estimates derived from Poincaré and logarithmic Sobolev inequalities Math Research Letters (994, [A-B-S] Alon, N; Boppana, R; Spencer, J An asymptotic isoperimetric inequality Geometric and Functional Anal 8 (998, [B-L] Bakry, D; Ledoux, M Lévy Gromov s isoperimetric inequality for an infinite dimensional diffusion generator Invent Math 3 (996, 59 8 [B-M] Barthe, F; Milman, E Transference principles for log-sobolev and spectral-gap with applications to conservative spin systems Comm Math Phys 33 (3, no, [B] Bobkov, S G Localization proof of the isoperimetric Bakry-Ledoux inequality and some applications Teor Veroyatnost i Primenen 47 (, no, Translation in: Theory Probab Appl 47 (3, no, [B] Bobkov, S G Perturbations in the Gaussian isoperimetric inequality J Math Sciences (New York, 66 (, no 3, 5 38 Translated from: Problems in Math Analysis 45 (, 3 4

19 9 [B-G] Bobkov, S G; Götze, F Exponential integrability and transportation cost related to logarithmic Sobolev inequalities J Funct Anal 63 (999, no, pp 8 [B-G-H] Bobkov, S G; Houdré, C; Tetali, P The subgaussian constant and concentration inequalities Israel J Math 56 (6, [D-M] Ding, J; Mossel, E Mixing under monotone censoring Electronic Comm Probab 9 (4, 6 [K] [L] Kirszbraun, M D Über die zusammenziehende und Lipschitzsche Transformationen Fund Math ( Ledoux, M The concentration of measure phenomenon Mathematical Surveys and Monographs 89 (, Amer Math Soc, Providence, RI [Mar] Marton, K Bounding d-distance by informational divergence: a method to prove measure concentration, Ann Probab 4 (996, no, [M] Maurey, B Some deviation inequalities Geom Funct Anal (99, [MS] McShane, E J Extension of range of functions Bull Amer Math Soc 4 (934, no, [Mi] Milman, E On the role of convexity in isoperimetry, spectral gap and concentration Invent Math 77 (9, no, 43 [Mi] Milman, E Properties of isoperimetric, functional and transport-entropy inequalities via concentration Probab Theory Related Fields 5 (, no 3 4, [M-W] Mueller, C E; Weissler, F B Hypercontractivity for the heat semigroup for ultraspherical polynomials and on the n-sphere J Funct Anal 48 (99, 5 83 [T] Talagrand, M An isoperimetric theorem on the cube and the Khinchine Kahane inequalities Proc Amer Math Soc 4 (988, [T] Talagrand, M Concentration of measure and isoperimetric inequalities in product spaces Publ Math IHES 8 (995, 73 5 Appendix Proof of Lemma Using the homogeneity, in order to derive the right-hand side inequality f in (, we may assume that sup p p p Then f p dµ p p/ for all p, and by Chebyshev s inequality, ( p p, F (t µ{ f t} for all t > t If t, choose here p = 4 t, in which case F (t 4 t Integrating by parts, we have, for any < ε < log 4, e εf dµ = = + ε + ε = e 4ε + e εt d( F (t te εt ( F (t dt + ε te εt dt + ε ε log 4 ε e (log 4ε te εt ( F (t dt te εt e log 4 t dt = e ( 4ε ε + ( log 4 ε

20 If ε log 8, the latter expression does not exceed 3 e4ε which does not exceed for ε log(4/3 4 Both inequalities are fulfilled for ε = log, and with this value e εf dµ Hence f L ψ (µ = ε log < 4, which yields the right inequality in ( Conversely, if f L ψ (µ =, then e 3 4 f dµ Since u(t = t p e 3 4 t p is maximized in t > at t = 3, we get ( p f p p = u( f e f p dµ u(t = 3e Hence, f p p /p 3e <, which yields the left inequality f Now, let us turn to ( and assume that sup p p p = Then f p dµ p p for all p, and by Chebyshev s inequality, for all t >, ( p p F (t µ{ f t} t If t, we may choose here p = t in which case F (t t, while for t < we choose p =, so that F (t log t Arguing as before, we have, for any < ε <, e ε f dµ = + ε e εt ( F (t dt + ε e εt ( F (t dt + ε e εt ( F (t dt + ε e εt e εt dt + ε t dt + ε The pre-last integral can be bounded by e ε t e ε f dµ e ε + εe ε log + e εt e log t dt dt = e ε log, so ε log log ε e ( ε For ε = 6, the latter expression is equal to 98939, and thus e ε f dµ < Hence f L ψ (µ ε = 6 Conversely, if f L ψ (µ =, then e 3 4 f dµ = Since u(t = t p e 3 4 t is maximized at t = p, we get ( p f p p = u( f e 3 4p 4 f dµ u(t = 3e Hence, f p p /p 4 3e <, which yields the left inequality Proof of Lemma 3 First assume that f ψ =, in particular e 7 8 f dµ The function u(t = log e tf dµ is smooth, convex, with u( = and u (t = fe tf dµ e tf dµ

21 In particular, u ( = Note that, by Jensen s inequality, e tf dµ, so u(t Further differentiation gives u (t = f e tf dµ ( fe tf dµ ( e tf dµ f e tf dµ Using tf t +f and the elementary inequality x e 3 8 x 8 3 e, we get, for t, f e tf dµ f e t +f dµ = e t / f e 3 8 f e 7 8 f dµ e / 8 3 e e 7 8 f dµ 4 Thus, u (t 4, and by Taylor s formula, u(t t On the hand, for t, by Cauchy s inequality, e tf dµ e t +f dµ = e t / e f / dµ ( e t / 4/7 e 7 8 f dµ = 4/7 e t / e ( log t e t Hence, in this case u(t t Thus, σf u(t = sup t t / 4, proving the right inequality of Lemma 3 For the left inequality, let σ f = Then e tf dµ e t / for all t R, which implies F (t µ{ f t} e t /, t From this, integrating by parts, we have, for any < ε <, e εf dµ = = + ε + 4ε e εt df (t = te εt ( F (t dt te εt e t / dt = + e εt d( F (t ε ε The last expression is equal to for ε = 6, which means that f ψ 6

A note on the convex infimum convolution inequality

A 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 information

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011 LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS S. G. Bobkov and F. L. Nazarov September 25, 20 Abstract We study large deviations of linear functionals on an isotropic

More information

Spectral Gap and Concentration for Some Spherically Symmetric Probability Measures

Spectral 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 information

KLS-TYPE ISOPERIMETRIC BOUNDS FOR LOG-CONCAVE PROBABILITY MEASURES. December, 2014

KLS-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 information

Concentration inequalities: basics and some new challenges

Concentration 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 information

Convex inequalities, isoperimetry and spectral gap III

Convex 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 information

On isotropicity with respect to a measure

On isotropicity with respect to a measure On isotropicity with respect to a measure Liran Rotem Abstract A body is said to be isoptropic with respect to a measure µ if the function θ x, θ dµ(x) is constant on the unit sphere. In this note, we

More information

Contents 1. Introduction 1 2. Main results 3 3. Proof of the main inequalities 7 4. Application to random dynamical systems 11 References 16

Contents 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 information

GAUSSIAN MEASURE OF SECTIONS OF DILATES AND TRANSLATIONS OF CONVEX BODIES. 2π) n

GAUSSIAN MEASURE OF SECTIONS OF DILATES AND TRANSLATIONS OF CONVEX BODIES. 2π) n GAUSSIAN MEASURE OF SECTIONS OF DILATES AND TRANSLATIONS OF CONVEX BODIES. A. ZVAVITCH Abstract. In this paper we give a solution for the Gaussian version of the Busemann-Petty problem with additional

More information

High-dimensional distributions with convexity properties

High-dimensional distributions with convexity properties High-dimensional distributions with convexity properties Bo az Klartag Tel-Aviv University A conference in honor of Charles Fefferman, Princeton, May 2009 High-Dimensional Distributions We are concerned

More information

Heat Flows, Geometric and Functional Inequalities

Heat 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 information

1 Cheeger differentiation

1 Cheeger differentiation 1 Cheeger differentiation after J. Cheeger [1] and S. Keith [3] A summary written by John Mackay Abstract We construct a measurable differentiable structure on any metric measure space that is doubling

More information

Expansion and Isoperimetric Constants for Product Graphs

Expansion 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 information

On Isoperimetric Functions of Probability Measures Having Log-Concave Densities with Respect to the Standard Normal Law

On Isoperimetric Functions of Probability Measures Having Log-Concave Densities with Respect to the Standard Normal Law On Isoerimetric Functions of Probability Measures Having Log-Concave Densities with Resect to the Standard Normal Law Sergey G. Bobkov Abstract Isoerimetric inequalities are discussed for one-dimensional

More information

ON THE REGULARITY OF SAMPLE PATHS OF SUB-ELLIPTIC DIFFUSIONS ON MANIFOLDS

ON THE REGULARITY OF SAMPLE PATHS OF SUB-ELLIPTIC DIFFUSIONS ON MANIFOLDS Bendikov, A. and Saloff-Coste, L. Osaka J. Math. 4 (5), 677 7 ON THE REGULARITY OF SAMPLE PATHS OF SUB-ELLIPTIC DIFFUSIONS ON MANIFOLDS ALEXANDER BENDIKOV and LAURENT SALOFF-COSTE (Received March 4, 4)

More information

Phenomena in high dimensions in geometric analysis, random matrices, and computational geometry Roscoff, France, June 25-29, 2012

Phenomena in high dimensions in geometric analysis, random matrices, and computational geometry Roscoff, France, June 25-29, 2012 Phenomena in high dimensions in geometric analysis, random matrices, and computational geometry Roscoff, France, June 25-29, 202 BOUNDS AND ASYMPTOTICS FOR FISHER INFORMATION IN THE CENTRAL LIMIT THEOREM

More information

KLS-type isoperimetric bounds for log-concave probability measures

KLS-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 information

2 (Bonus). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure?

2 (Bonus). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure? MA 645-4A (Real Analysis), Dr. Chernov Homework assignment 1 (Due 9/5). Prove that every countable set A is measurable and µ(a) = 0. 2 (Bonus). Let A consist of points (x, y) such that either x or y is

More information

Discrete Ricci curvature: Open problems

Discrete 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 information

A converse Gaussian Poincare-type inequality for convex functions

A converse Gaussian Poincare-type inequality for convex functions Statistics & Proaility Letters 44 999 28 290 www.elsevier.nl/locate/stapro A converse Gaussian Poincare-type inequality for convex functions S.G. Bokov a;, C. Houdre ; ;2 a Department of Mathematics, Syktyvkar

More information

3 (Due ). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure?

3 (Due ). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure? MA 645-4A (Real Analysis), Dr. Chernov Homework assignment 1 (Due ). Show that the open disk x 2 + y 2 < 1 is a countable union of planar elementary sets. Show that the closed disk x 2 + y 2 1 is a countable

More information

Entropy and Ergodic Theory Lecture 17: Transportation and concentration

Entropy and Ergodic Theory Lecture 17: Transportation and concentration Entropy and Ergodic Theory Lecture 17: Transportation and concentration 1 Concentration in terms of metric spaces In this course, a metric probability or m.p. space is a triple px, d, µq in which px, dq

More information

Local semiconvexity of Kantorovich potentials on non-compact manifolds

Local 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 information

Weak and strong moments of l r -norms of log-concave vectors

Weak and strong moments of l r -norms of log-concave vectors Weak and strong moments of l r -norms of log-concave vectors Rafał Latała based on the joint work with Marta Strzelecka) University of Warsaw Minneapolis, April 14 2015 Log-concave measures/vectors A measure

More information

From the Brunn-Minkowski inequality to a class of Poincaré type inequalities

From the Brunn-Minkowski inequality to a class of Poincaré type inequalities arxiv:math/0703584v1 [math.fa] 20 Mar 2007 From the Brunn-Minkowski inequality to a class of Poincaré type inequalities Andrea Colesanti Abstract We present an argument which leads from the Brunn-Minkowski

More information

Logarithmic Sobolev Inequalities

Logarithmic Sobolev Inequalities Logarithmic Sobolev Inequalities M. Ledoux Institut de Mathématiques de Toulouse, France logarithmic Sobolev inequalities what they are, some history analytic, geometric, optimal transportation proofs

More information

Solutions to Tutorial 11 (Week 12)

Solutions to Tutorial 11 (Week 12) THE UIVERSITY OF SYDEY SCHOOL OF MATHEMATICS AD STATISTICS Solutions to Tutorial 11 (Week 12) MATH3969: Measure Theory and Fourier Analysis (Advanced) Semester 2, 2017 Web Page: http://sydney.edu.au/science/maths/u/ug/sm/math3969/

More information

MATH 51H Section 4. October 16, Recall what it means for a function between metric spaces to be continuous:

MATH 51H Section 4. October 16, Recall what it means for a function between metric spaces to be continuous: MATH 51H Section 4 October 16, 2015 1 Continuity Recall what it means for a function between metric spaces to be continuous: Definition. Let (X, d X ), (Y, d Y ) be metric spaces. A function f : X Y is

More information

Entropy for zero-temperature limits of Gibbs-equilibrium states for countable-alphabet subshifts of finite type

Entropy for zero-temperature limits of Gibbs-equilibrium states for countable-alphabet subshifts of finite type Entropy for zero-temperature limits of Gibbs-equilibrium states for countable-alphabet subshifts of finite type I. D. Morris August 22, 2006 Abstract Let Σ A be a finitely primitive subshift of finite

More information

Lecture 4 Lebesgue spaces and inequalities

Lecture 4 Lebesgue spaces and inequalities Lecture 4: Lebesgue spaces and inequalities 1 of 10 Course: Theory of Probability I Term: Fall 2013 Instructor: Gordan Zitkovic Lecture 4 Lebesgue spaces and inequalities Lebesgue spaces We have seen how

More information

1.1. MEASURES AND INTEGRALS

1.1. MEASURES AND INTEGRALS CHAPTER 1: MEASURE THEORY In this chapter we define the notion of measure µ on a space, construct integrals on this space, and establish their basic properties under limits. The measure µ(e) will be defined

More information

3 Integration and Expectation

3 Integration and Expectation 3 Integration and Expectation 3.1 Construction of the Lebesgue Integral Let (, F, µ) be a measure space (not necessarily a probability space). Our objective will be to define the Lebesgue integral R fdµ

More information

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction SHARP BOUNDARY TRACE INEQUALITIES GILES AUCHMUTY Abstract. This paper describes sharp inequalities for the trace of Sobolev functions on the boundary of a bounded region R N. The inequalities bound (semi-)norms

More information

Maths 212: Homework Solutions

Maths 212: Homework Solutions Maths 212: Homework Solutions 1. The definition of A ensures that x π for all x A, so π is an upper bound of A. To show it is the least upper bound, suppose x < π and consider two cases. If x < 1, then

More information

MATH MEASURE THEORY AND FOURIER ANALYSIS. Contents

MATH MEASURE THEORY AND FOURIER ANALYSIS. Contents MATH 3969 - MEASURE THEORY AND FOURIER ANALYSIS ANDREW TULLOCH Contents 1. Measure Theory 2 1.1. Properties of Measures 3 1.2. Constructing σ-algebras and measures 3 1.3. Properties of the Lebesgue measure

More information

Inverse Brascamp-Lieb inequalities along the Heat equation

Inverse 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 information

MAJORIZING MEASURES WITHOUT MEASURES. By Michel Talagrand URA 754 AU CNRS

MAJORIZING MEASURES WITHOUT MEASURES. By Michel Talagrand URA 754 AU CNRS The Annals of Probability 2001, Vol. 29, No. 1, 411 417 MAJORIZING MEASURES WITHOUT MEASURES By Michel Talagrand URA 754 AU CNRS We give a reformulation of majorizing measures that does not involve measures,

More information

PROPERTY OF HALF{SPACES. July 25, Abstract

PROPERTY OF HALF{SPACES. July 25, Abstract A CHARACTERIZATION OF GAUSSIAN MEASURES VIA THE ISOPERIMETRIC PROPERTY OF HALF{SPACES S. G. Bobkov y and C. Houdre z July 25, 1995 Abstract If the half{spaces of the form fx 2 R n : x 1 cg are extremal

More information

SPECTRAL 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 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 information

Displacement convexity of the relative entropy in the discrete h

Displacement 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 information

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 21, 2003, 211 226 SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS Massimo Grosi Filomena Pacella S.

More information

The small ball property in Banach spaces (quantitative results)

The small ball property in Banach spaces (quantitative results) The small ball property in Banach spaces (quantitative results) Ehrhard Behrends Abstract A metric space (M, d) is said to have the small ball property (sbp) if for every ε 0 > 0 there exists a sequence

More information

ON CONCENTRATION FUNCTIONS OF RANDOM VARIABLES. Sergey G. Bobkov and Gennadiy P. Chistyakov. June 2, 2013

ON CONCENTRATION FUNCTIONS OF RANDOM VARIABLES. Sergey G. Bobkov and Gennadiy P. Chistyakov. June 2, 2013 ON CONCENTRATION FUNCTIONS OF RANDOM VARIABLES Sergey G. Bobkov and Gennadiy P. Chistyakov June, 3 Abstract The concentration functions are considered for sums of independent random variables. Two sided

More information

STABILITY RESULTS FOR THE BRUNN-MINKOWSKI INEQUALITY

STABILITY RESULTS FOR THE BRUNN-MINKOWSKI INEQUALITY STABILITY RESULTS FOR THE BRUNN-MINKOWSKI INEQUALITY ALESSIO FIGALLI 1. Introduction The Brunn-Miknowski inequality gives a lower bound on the Lebesgue measure of a sumset in terms of the measures of the

More information

N. GOZLAN, C. ROBERTO, P-M. SAMSON

N. GOZLAN, C. ROBERTO, P-M. SAMSON FROM DIMENSION FREE CONCENTRATION TO THE POINCARÉ INEQUALITY N. GOZLAN, C. ROBERTO, P-M. SAMSON Abstract. We prove that a probability measure on an abstract metric space satisfies a non trivial dimension

More information

Integral Jensen inequality

Integral Jensen inequality Integral Jensen inequality Let us consider a convex set R d, and a convex function f : (, + ]. For any x,..., x n and λ,..., λ n with n λ i =, we have () f( n λ ix i ) n λ if(x i ). For a R d, let δ a

More information

Integration on Measure Spaces

Integration on Measure Spaces Chapter 3 Integration on Measure Spaces In this chapter we introduce the general notion of a measure on a space X, define the class of measurable functions, and define the integral, first on a class of

More information

Distance-Divergence Inequalities

Distance-Divergence Inequalities Distance-Divergence Inequalities Katalin Marton Alfréd Rényi Institute of Mathematics of the Hungarian Academy of Sciences Motivation To find a simple proof of the Blowing-up Lemma, proved by Ahlswede,

More information

6.2 Fubini s Theorem. (µ ν)(c) = f C (x) dµ(x). (6.2) Proof. Note that (X Y, A B, µ ν) must be σ-finite as well, so that.

6.2 Fubini s Theorem. (µ ν)(c) = f C (x) dµ(x). (6.2) Proof. Note that (X Y, A B, µ ν) must be σ-finite as well, so that. 6.2 Fubini s Theorem Theorem 6.2.1. (Fubini s theorem - first form) Let (, A, µ) and (, B, ν) be complete σ-finite measure spaces. Let C = A B. Then for each µ ν- measurable set C C the section x C is

More information

Introduction and Preliminaries

Introduction and Preliminaries Chapter 1 Introduction and Preliminaries This chapter serves two purposes. The first purpose is to prepare the readers for the more systematic development in later chapters of methods of real analysis

More information

Stability results for Logarithmic Sobolev inequality

Stability 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 information

Approximately Gaussian marginals and the hyperplane conjecture

Approximately Gaussian marginals and the hyperplane conjecture Approximately Gaussian marginals and the hyperplane conjecture Tel-Aviv University Conference on Asymptotic Geometric Analysis, Euler Institute, St. Petersburg, July 2010 Lecture based on a joint work

More information

Course 212: Academic Year Section 1: Metric Spaces

Course 212: Academic Year Section 1: Metric Spaces Course 212: Academic Year 1991-2 Section 1: Metric Spaces D. R. Wilkins Contents 1 Metric Spaces 3 1.1 Distance Functions and Metric Spaces............. 3 1.2 Convergence and Continuity in Metric Spaces.........

More information

MATH 202B - Problem Set 5

MATH 202B - Problem Set 5 MATH 202B - Problem Set 5 Walid Krichene (23265217) March 6, 2013 (5.1) Show that there exists a continuous function F : [0, 1] R which is monotonic on no interval of positive length. proof We know there

More information

MATHS 730 FC Lecture Notes March 5, Introduction

MATHS 730 FC Lecture Notes March 5, Introduction 1 INTRODUCTION MATHS 730 FC Lecture Notes March 5, 2014 1 Introduction Definition. If A, B are sets and there exists a bijection A B, they have the same cardinality, which we write as A, #A. If there exists

More information

CHAPTER 6. Differentiation

CHAPTER 6. Differentiation CHPTER 6 Differentiation The generalization from elementary calculus of differentiation in measure theory is less obvious than that of integration, and the methods of treating it are somewhat involved.

More information

L p Spaces and Convexity

L p Spaces and Convexity L p Spaces and Convexity These notes largely follow the treatments in Royden, Real Analysis, and Rudin, Real & Complex Analysis. 1. Convex functions Let I R be an interval. For I open, we say a function

More information

Notions such as convergent sequence and Cauchy sequence make sense for any metric space. Convergent Sequences are Cauchy

Notions such as convergent sequence and Cauchy sequence make sense for any metric space. Convergent Sequences are Cauchy Banach Spaces These notes provide an introduction to Banach spaces, which are complete normed vector spaces. For the purposes of these notes, all vector spaces are assumed to be over the real numbers.

More information

Jensen s inequality for multivariate medians

Jensen s inequality for multivariate medians Jensen s inequality for multivariate medians Milan Merkle University of Belgrade, Serbia emerkle@etf.rs Given a probability measure µ on Borel sigma-field of R d, and a function f : R d R, the main issue

More information

arxiv: v1 [math.fa] 20 Dec 2011

arxiv: v1 [math.fa] 20 Dec 2011 PUSH FORWARD MEASURES AND CONCENTRATION PHENOMENA arxiv:1112.4765v1 [math.fa] 20 Dec 2011 C. HUGO JIMÉNEZ, MÁRTON NASZÓDI, AND RAFAEL VILLA Abstract. In this note we study how a concentration phenomenon

More information

COMMENT ON : HYPERCONTRACTIVITY OF HAMILTON-JACOBI EQUATIONS, BY S. BOBKOV, I. GENTIL AND M. LEDOUX

COMMENT ON : HYPERCONTRACTIVITY OF HAMILTON-JACOBI EQUATIONS, BY S. BOBKOV, I. GENTIL AND M. LEDOUX COMMENT ON : HYPERCONTRACTIVITY OF HAMILTON-JACOBI EQUATIONS, BY S. BOBKOV, I. GENTIL AND M. LEDOUX F. OTTO AND C. VILLANI In their remarkable work [], Bobkov, Gentil and Ledoux improve, generalize and

More information

On John type ellipsoids

On John type ellipsoids On John type ellipsoids B. Klartag Tel Aviv University Abstract Given an arbitrary convex symmetric body K R n, we construct a natural and non-trivial continuous map u K which associates ellipsoids to

More information

The Hilbert Transform and Fine Continuity

The Hilbert Transform and Fine Continuity Irish Math. Soc. Bulletin 58 (2006), 8 9 8 The Hilbert Transform and Fine Continuity J. B. TWOMEY Abstract. It is shown that the Hilbert transform of a function having bounded variation in a finite interval

More information

Moment Measures. Bo az Klartag. Tel Aviv University. Talk at the asymptotic geometric analysis seminar. Tel Aviv, May 2013

Moment Measures. Bo az Klartag. Tel Aviv University. Talk at the asymptotic geometric analysis seminar. Tel Aviv, May 2013 Tel Aviv University Talk at the asymptotic geometric analysis seminar Tel Aviv, May 2013 Joint work with Dario Cordero-Erausquin. A bijection We present a correspondence between convex functions and Borel

More information

On the isotropic constant of marginals

On the isotropic constant of marginals On the isotropic constant of marginals Grigoris Paouris Abstract Let p < and n. We write µ B,p,n for the probability measure in R n with density B n p, where Bp n := {x R n : x p b p,n} and Bp n =. Let

More information

ITERATED FUNCTION SYSTEMS WITH CONTINUOUS PLACE DEPENDENT PROBABILITIES

ITERATED FUNCTION SYSTEMS WITH CONTINUOUS PLACE DEPENDENT PROBABILITIES UNIVERSITATIS IAGELLONICAE ACTA MATHEMATICA, FASCICULUS XL 2002 ITERATED FUNCTION SYSTEMS WITH CONTINUOUS PLACE DEPENDENT PROBABILITIES by Joanna Jaroszewska Abstract. We study the asymptotic behaviour

More information

Entropy and Ergodic Theory Lecture 15: A first look at concentration

Entropy 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 information

g 2 (x) (1/3)M 1 = (1/3)(2/3)M.

g 2 (x) (1/3)M 1 = (1/3)(2/3)M. COMPACTNESS If C R n is closed and bounded, then by B-W it is sequentially compact: any sequence of points in C has a subsequence converging to a point in C Conversely, any sequentially compact C R n is

More information

ON THE CONVEX INFIMUM CONVOLUTION INEQUALITY WITH OPTIMAL COST FUNCTION

ON THE CONVEX INFIMUM CONVOLUTION INEQUALITY WITH OPTIMAL COST FUNCTION ON THE CONVEX INFIMUM CONVOLUTION INEQUALITY WITH OPTIMAL COST FUNCTION MARTA STRZELECKA, MICHA L STRZELECKI, AND TOMASZ TKOCZ Abstract. We show that every symmetric random variable with log-concave tails

More information

BOUNDS ON THE DEFICIT IN THE LOGARITHMIC SOBOLEV INEQUALITY

BOUNDS ON THE DEFICIT IN THE LOGARITHMIC SOBOLEV INEQUALITY BOUNDS ON THE DEFICIT IN THE LOGARITHMIC SOBOLEV INEQUALITY S. G. BOBKOV, N. GOZLAN, C. ROBERTO AND P.-M. SAMSON Abstract. The deficit in the logarithmic Sobolev inequality for the Gaussian measure is

More information

L p Functions. Given a measure space (X, µ) and a real number p [1, ), recall that the L p -norm of a measurable function f : X R is defined by

L p Functions. Given a measure space (X, µ) and a real number p [1, ), recall that the L p -norm of a measurable function f : X R is defined by L p Functions Given a measure space (, µ) and a real number p [, ), recall that the L p -norm of a measurable function f : R is defined by f p = ( ) /p f p dµ Note that the L p -norm of a function f may

More information

THE HUTCHINSON BARNSLEY THEORY FOR INFINITE ITERATED FUNCTION SYSTEMS

THE HUTCHINSON BARNSLEY THEORY FOR INFINITE ITERATED FUNCTION SYSTEMS Bull. Austral. Math. Soc. Vol. 72 2005) [441 454] 39b12, 47a35, 47h09, 54h25 THE HUTCHINSON BARNSLEY THEORY FOR INFINITE ITERATED FUNCTION SYSTEMS Gertruda Gwóźdź- Lukawska and Jacek Jachymski We show

More information

HYPERCONTRACTIVE MEASURES, TALAGRAND S INEQUALITY, AND INFLUENCES

HYPERCONTRACTIVE 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 information

Estimates for probabilities of independent events and infinite series

Estimates for probabilities of independent events and infinite series Estimates for probabilities of independent events and infinite series Jürgen Grahl and Shahar evo September 9, 06 arxiv:609.0894v [math.pr] 8 Sep 06 Abstract This paper deals with finite or infinite sequences

More information

Dimensional behaviour of entropy and information

Dimensional behaviour of entropy and information Dimensional behaviour of entropy and information Sergey Bobkov and Mokshay Madiman Note: A slightly condensed version of this paper is in press and will appear in the Comptes Rendus de l Académies des

More information

LECTURE 15: COMPLETENESS AND CONVEXITY

LECTURE 15: COMPLETENESS AND CONVEXITY LECTURE 15: COMPLETENESS AND CONVEXITY 1. The Hopf-Rinow Theorem Recall that a Riemannian manifold (M, g) is called geodesically complete if the maximal defining interval of any geodesic is R. On the other

More information

Metric Spaces and Topology

Metric Spaces and Topology Chapter 2 Metric Spaces and Topology From an engineering perspective, the most important way to construct a topology on a set is to define the topology in terms of a metric on the set. This approach underlies

More information

NOTES ON THE REGULARITY OF QUASICONFORMAL HOMEOMORPHISMS

NOTES ON THE REGULARITY OF QUASICONFORMAL HOMEOMORPHISMS NOTES ON THE REGULARITY OF QUASICONFORMAL HOMEOMORPHISMS CLARK BUTLER. Introduction The purpose of these notes is to give a self-contained proof of the following theorem, Theorem.. Let f : S n S n be a

More information

+ 2x sin x. f(b i ) f(a i ) < ɛ. i=1. i=1

+ 2x sin x. f(b i ) f(a i ) < ɛ. i=1. i=1 Appendix To understand weak derivatives and distributional derivatives in the simplest context of functions of a single variable, we describe without proof some results from real analysis (see [7] and

More information

Part III. 10 Topological Space Basics. Topological Spaces

Part III. 10 Topological Space Basics. Topological Spaces Part III 10 Topological Space Basics Topological Spaces Using the metric space results above as motivation we will axiomatize the notion of being an open set to more general settings. Definition 10.1.

More information

Probability and Measure

Probability 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 information

arxiv: v1 [math.ca] 31 Jan 2016

arxiv: v1 [math.ca] 31 Jan 2016 ASYMPTOTIC STABILITY OF THE CAUCHY AND JENSEN FUNCTIONAL EQUATIONS ANNA BAHYRYCZ, ZSOLT PÁLES, AND MAGDALENA PISZCZEK arxiv:160.00300v1 [math.ca] 31 Jan 016 Abstract. The aim of this note is to investigate

More information

Measurable functions are approximately nice, even if look terrible.

Measurable functions are approximately nice, even if look terrible. Tel Aviv University, 2015 Functions of real variables 74 7 Approximation 7a A terrible integrable function........... 74 7b Approximation of sets................ 76 7c Approximation of functions............

More information

curvature, 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 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 information

Invariances in spectral estimates. Paris-Est Marne-la-Vallée, January 2011

Invariances in spectral estimates. Paris-Est Marne-la-Vallée, January 2011 Invariances in spectral estimates Franck Barthe Dario Cordero-Erausquin Paris-Est Marne-la-Vallée, January 2011 Notation Notation Given a probability measure ν on some Euclidean space, the Poincaré constant

More information

at time t, in dimension d. The index i varies in a countable set I. We call configuration the family, denoted generically by Φ: U (x i (t) x j (t))

at time t, in dimension d. The index i varies in a countable set I. We call configuration the family, denoted generically by Φ: U (x i (t) x j (t)) Notations In this chapter we investigate infinite systems of interacting particles subject to Newtonian dynamics Each particle is characterized by its position an velocity x i t, v i t R d R d at time

More information

PREVALENCE OF SOME KNOWN TYPICAL PROPERTIES. 1. Introduction

PREVALENCE OF SOME KNOWN TYPICAL PROPERTIES. 1. Introduction Acta Math. Univ. Comenianae Vol. LXX, 2(2001), pp. 185 192 185 PREVALENCE OF SOME KNOWN TYPICAL PROPERTIES H. SHI Abstract. In this paper, some known typical properties of function spaces are shown to

More information

The Lusin Theorem and Horizontal Graphs in the Heisenberg Group

The Lusin Theorem and Horizontal Graphs in the Heisenberg Group Analysis and Geometry in Metric Spaces Research Article DOI: 10.2478/agms-2013-0008 AGMS 2013 295-301 The Lusin Theorem and Horizontal Graphs in the Heisenberg Group Abstract In this paper we prove that

More information

Poincaré Inequalities and Moment Maps

Poincaré 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 information

Random Bernstein-Markov factors

Random Bernstein-Markov factors Random Bernstein-Markov factors Igor Pritsker and Koushik Ramachandran October 20, 208 Abstract For a polynomial P n of degree n, Bernstein s inequality states that P n n P n for all L p norms on the unit

More information

Construction of a general measure structure

Construction of a general measure structure Chapter 4 Construction of a general measure structure We turn to the development of general measure theory. The ingredients are a set describing the universe of points, a class of measurable subsets along

More information

Examples of Dual Spaces from Measure Theory

Examples of Dual Spaces from Measure Theory Chapter 9 Examples of Dual Spaces from Measure Theory We have seen that L (, A, µ) is a Banach space for any measure space (, A, µ). We will extend that concept in the following section to identify an

More information

Basic Properties of Metric and Normed Spaces

Basic Properties of Metric and Normed Spaces Basic Properties of Metric and Normed Spaces Computational and Metric Geometry Instructor: Yury Makarychev The second part of this course is about metric geometry. We will study metric spaces, low distortion

More information

THEOREMS, ETC., FOR MATH 515

THEOREMS, ETC., FOR MATH 515 THEOREMS, ETC., FOR MATH 515 Proposition 1 (=comment on page 17). If A is an algebra, then any finite union or finite intersection of sets in A is also in A. Proposition 2 (=Proposition 1.1). For every

More information

Part II Probability and Measure

Part II Probability and Measure Part II Probability and Measure Theorems Based on lectures by J. Miller Notes taken by Dexter Chua Michaelmas 2016 These notes are not endorsed by the lecturers, and I have modified them (often significantly)

More information

AN INEQUALITY FOR TAIL PROBABILITIES OF MARTINGALES WITH BOUNDED DIFFERENCES

AN 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 information

BERNOULLI ACTIONS OF SOFIC GROUPS HAVE COMPLETELY POSITIVE ENTROPY

BERNOULLI ACTIONS OF SOFIC GROUPS HAVE COMPLETELY POSITIVE ENTROPY BERNOULLI ACTIONS OF SOFIC GROUPS HAVE COMPLETELY POSITIVE ENTROPY DAVID KERR Abstract. We prove that every Bernoulli action of a sofic group has completely positive entropy with respect to every sofic

More information

THEOREMS, ETC., FOR MATH 516

THEOREMS, ETC., FOR MATH 516 THEOREMS, ETC., FOR MATH 516 Results labeled Theorem Ea.b.c (or Proposition Ea.b.c, etc.) refer to Theorem c from section a.b of Evans book (Partial Differential Equations). Proposition 1 (=Proposition

More information

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9 MAT 570 REAL ANALYSIS LECTURE NOTES PROFESSOR: JOHN QUIGG SEMESTER: FALL 204 Contents. Sets 2 2. Functions 5 3. Countability 7 4. Axiom of choice 8 5. Equivalence relations 9 6. Real numbers 9 7. Extended

More information

THE INVERSE FUNCTION THEOREM FOR LIPSCHITZ MAPS

THE INVERSE FUNCTION THEOREM FOR LIPSCHITZ MAPS THE INVERSE FUNCTION THEOREM FOR LIPSCHITZ MAPS RALPH HOWARD DEPARTMENT OF MATHEMATICS UNIVERSITY OF SOUTH CAROLINA COLUMBIA, S.C. 29208, USA HOWARD@MATH.SC.EDU Abstract. This is an edited version of a

More information