Monotonicity of facet numbers of random convex hulls

Size: px
Start display at page:

Download "Monotonicity of facet numbers of random convex hulls"

Transcription

1 Monotonicity of facet numbers of ranom convex hulls Gilles Bonnet, Julian Grote, Daniel Temesvari, Christoph Thäle, Nicola Turchi an Florian Wespi arxiv:173.31v1 [math.mg] 7 Mar 17 Abstract Let X 1,..., X n be inepenent ranom points that are istribute accoring to a probability measure on R an let P n be the ranom convex hull generate by X 1,..., X n n +1. Natural classes of probability istributions are characterize for which, by means of Blaschke-Petkantschin formulae from integral geometry, one can show that the mean facet number of P n is strictly monotonically increasing in n. Keywors. Blaschke-Petkantschin formula, mean facet number, ranom convex hull MSC. 5A, 5B5, 53C65, 6D5 1 Introuction an main result Fix a space imension. For an integer n +1, let X 1,..., X n be inepenent ranom points that are chosen accoring to an absolutely continuous probability istribution on R. By P n 1 an P n we enote the ranom convex hulls generate by X 1,..., X n 1 an X 1,..., X n, respectively. In our present text we are intereste in the mean number of facets E f 1 P n 1 an E f 1 P n of P n 1 an P n. More specifically, we ask the following monotonicity question: Is it true that E f 1 P n 1 E f 1 P n? This question has been put forwar an answere positively by Devillers, Glisse, Goaoc, Moroz an Reitzner [7] for ranom points that are uniformly istribute in a convex boy K R if = an, if 3, uner the aitional assumptions that the bounary of K is twice ifferentiable with strictly positive Gaussian curvature an that n is sufficiently large, that is, n nk, where nk is a constant epening on K. Moreover, an affirmative answer was obtaine by Beermann [4] if the ranom points are chosen with respect to the stanar Gaussian istribution on R or accoring to the uniform istribution in the -imensional unit ball for all. Beermann s proof essentially relies on a Blaschke-Petkantschin formula, a well known change-of-variables formula Faculty of Mathematics, Ruhr University Bochum, Germany. gilles.bonnet@rub.e Faculty of Mathematics, Ruhr University Bochum, Germany. julian.grote@rub.e Faculty of Mathematics, Ruhr University Bochum, Germany. aniel.temesvari@rub.e Faculty of Mathematics, Ruhr University Bochum, Germany. christoph.thaele@rub.e Faculty of Mathematics, Ruhr University Bochum, Germany. nicola.turchi@rub.e Institute of Mathematical Statistics an Actuarial Science, University of Bern, Switzerlan. florian.wespi@stat.unibe.ch 1

2 in integral geometry. Our aim in this text is to generalize her approach to other an more general probability istributions on R. In fact, we will be able to characterize all absolutely continuous rotationally symmetric istributions on R whose ensities satisfy a natural scaling property see 9 below, to which the methoology base on the Blaschke-Petkantschin formula can be applie an for which we can answer positively the monotonicity question pose above for any of these istributions. Moreover, we will apply our results to stuy similar monotonicity questions for a class of spherical convex hulls generate by ranom points on a half-sphere, which comprises as a special case the moel recently stuie by Bárány, Hug, Reitzner an Schneier [3]. To present our main result formally, we introuce four classes of probability measures: - G is the class of centre Gaussian istributions on R with ensity proportional to x exp x σ, σ >, - H is the class of heavy-taile istributions on R with ensity proportional to x 1+ x σ β, β > /, σ >, - B is the class of beta-type istributions on the -imensional centre ball B σ of raius σ with ensity proportional to x 1 x σ β, β > 1, σ >, - U comprises the uniform istributions on the 1-imensional centre spheres S 1 σ with raius σ >. It will turn out that the classes G, H, B an U contain precisely the absolutely continuous rotationally symmetric probability istributions on R, whose ensities satisfy the natural scaling property 9 below, for which monotonicity of the mean facet number of the associate ranom convex hulls can be shown by means of arguments base on a Blaschke-Petkantschin formula, see the iscussion at the en of Section 4 for further etails. In fact, our result shows that even the stronger strict monotonicity hols. Theorem 1 Let X 1,..., X n R, n + 1, be inepenent an ientically istribute accoring to a probability measure belonging to one of the classes G, H, B or U. Then, E f 1 P n > E f 1 P n 1. It shoul be emphasize that strict monotonicity of n f 1 P n cannot hol pathwise except for the trivial case n = + 1, since the aition of a further ranom point can reuce the facet number arbitrarily as the aitional point might see much more than vertices of the alreay constructe ranom convex hull. For this reason, the expectation in Theorem 1 is essential to euce a non-trivial result. We woul also like to remark that monotonicity questions relate to the volume of ranom convex hulls have recently attracte some interest in convex geometry because of their connection to the famous slicing problem. Namely, if K an L are two compact

3 convex sets in R with interior points, let V K an V L be the volume of the convex hull of + 1 inepenent ranom points uniformly istribute in K an L, respectively. One is intereste in the question whether the set inclusion K L implies the inequality EV K EV L. In particular, the work of Raemacher [11] shows that this is false in general whenever 4. Higher moments were treate by Reichenwallner an Reitzner [1], an we refer to the iscussion therein for further etails an backgroun material. Our text is structure as follows. In Section we recall the necessary backgroun material from integral geometry an introuce some more notation. Moreover, in Section 3 we evelop several auxiliary results that prepare for the proof of Theorem 1, which is presente in Section 4. We also iscuss in Section 4 the limitations an possible extensions of the metho we use. The final Section 5 contains the application of Theorem 1 to ranom convex hulls on a half-sphere. Backgroun material from integral geometry.1 General notation We enote by A, q the Grassmannian of all q-imensional affine subspaces of R, where q {, 1,..., }. It is a locally compact, homogeneous space with respect to the group of Eucliean motions in R. The corresponing locally finite, motion invariant measure is enote by µ q, which is normalize in such a way that µ q {E A, q : E B = } = κ q, see [14]. Here, B is the centre -imensional unit ball, κ q = π q/ is the q- Γ1+ q imensional volume of B q an Γ inicates the Gamma function. Moreover, the Beta function is given by Ba, b := 1 s a 1 1 s b 1 s = ΓaΓb, a, b >. Γa+ b We shall enote by S 1 the 1-imensional unit sphere an abbreviate by ω = κ its total spherical Lebesgue measure. For a subspace E A, q, we let λ E be the Lebesgue measure on E. For a set K R, we shall write H q K for the q-imensional Hausorff measure on K. The operators conv an span enote the convex an linear hull of the argument. We will use the notation 1 x 1,..., x to inicate the 1-imensional volume of the convex hull of points x 1,..., x.. Blaschke-Petkantschin formulae Our proof of Theorem 1 heavily relies on Blaschke-Petkantschin formulae from integral geometry. First, we rephrase a special case of the affine Blaschke-Petkantschin formula in R, which appears as Theorem 7..7 in [14]. 3

4 Proposition Let f : R R be a non-negative measurable function. Then, R fx 1,..., x x 1,..., x = ω 1! A, 1 H fx 1,..., x 1 x 1,..., x λ H x 1,..., x µ 1 H. Besies the affine Blaschke-Petkantschin formula in R we nee its spherical counterpart, which is a special case of Theorem 1 in [15] an can also be foun in [1, Theorem 4]. Proposition 3 Let f : S 1 R be a non-negative measurable function. Then, 1 fx 1,..., x H x S 1 1,..., x = 1! S 1 A, 1 H S 1 fx 1,..., x 1 x 1,..., x 1 h H H S 1 x 1,..., x µ 1 H, where h enotes the istance from H to the origin..3 A slice integration formula Finally, we will make use of the following special case of the spherical slice integration formula taken from Theorem A.4 in []. Proposition 4 Let f : S 1 R be a non-negative measurable function. Then, S 1 1 fxh 1 x = 1 t 3 S 1 1 S ft, 1 t yh y t. S 3 Auxiliary results 3.1 An estimate for integrals of concave functions A version of the next lemma was alreay state in [4], but without proof. For the sake of completeness we inclue here the short argument. Lemma 5 Let h : R R be a non-negative measurable function which is strictly positive on a set of positive Lebesgue measure. Further, let g : R R be a linear function with negative slope an root s [, 1]. Moreover, let L : R R be positive an strictly concave on [, 1]. Then, wherels = Ls s s. 1 hsgsls 1 s > 1 hsgsls 1 s, 1 4

5 Proof. We start by exploiting the positivity an strict concavity of L. For s [, s, it implies that s Ls = L s s > s s Ls, while for s s, 1], it gives Ls < s s Ls. 3 Since g has a negative slope, it is positive on[, s an negative ons, 1]. Splitting the integral on the left han sie of 1 at the point s an using an 3, respectively, yiels 1 = > = hsgsls 1 s s s 1 hsgsls 1 s+ 1 s hsgsls 1 s s 1 1 s 1 hsgs s Ls s+ hsgs s Ls s s hsgsls 1 s. This completes the argument. 3. Computation of marginal ensities Recall the efinitions of the istribution classes H, B an U. It will turn out that it suffices to consier the cases where the scale parameters σ there are equal to 1. From now on we restrict to these cases an enote the ensity of a istribution in H by p H,β x = π / Γβ Γβ β, x R, β > /, 4 1+ x that of a istribution in B by p B,β x = π / Γ + β+1 1 x β, x B, β > 1, Γβ+ 1 an note that the uniform istribution on S 1 has ensity p U x = 1 ω, x S 1, with respect to the spherical Lebesgue measure. The next lemma provies formulas for the ensities of the one-imensional marginals of these istributions an shows, that the classes B an H are in some sense close uner one-imensional projections. Since all istributions we consier are rotationally symmetric, it is sufficient to consier projections onto the first coorinate. We woul like to emphasize that the proof of Lemma 6 uses in an essential way the scaling property 9 below of the involve ensities. 5

6 Lemma 6 Let Π : R R,x 1,..., x x 1 be the projection onto the first coorinate. i Let P H be a istribution with ensity p H,β for some β > /. Then, the image measure of P uner Π has ensity Γ β 1 f H,β x = π 1/ 1+ x 1 β, x R. Γ β ii Let P B be a istribution with ensity p B,β for some β > 1. Then, the image measure of P uner Π has ensity f B,β x = Γ β+1+ π 1/ 1 x 1 +β, x [ 1, 1]. Γ f U x = π 1/ β+ +1 iii Let P U be the uniform istribution on S 1. Then, the image measure of P uner Π has ensity Γ Γ 1 1 x 3, x [ 1, 1]. Proof. To prove i we put x = x 1,..., x R, y := x,..., x an also efine c H,,β := π / Γβ Γβ /. Then, R 1 c H,,β = 1+ x β x,..., x R 1 c H,,β 1+ x 1 β = 1+ x 1 β R 1 c H,,β = 1+ x 1 1 β c H,,β H,,β c H, 1,β 1+ x 1 1 β, β y 1+ y 1+ x1 1+ z β 1+ x 1 1 z c c H, 1,β H, 1,β R 1 1+ z β z where we use the substitution z = y/ 1+ x1. Plugging in the constants yiels the esire result. Next, we consier the istribution with ensity p B,β. For x = x 1,..., x B, we put again y := x,..., x an abbreviate c B,,β := π / Γ +β+1. Then, similarly as Γβ+1 6

7 above, we compute B 1 c B,,β = 1 x β x,..., x B 1 c B,,β 1 x 1 β = 1 x 1 β B 1 c B,,β = 1 x 1 1 +β c B,,β B,,β c B, 1,β 1 x 1 1 +β, β y 1 y 1 x1 1 z β 1 x 1 1 z c c B, 1,β B, 1,β B 1 1 z β z where we use the substitution z = y/ 1 x1. Again, simplification of the constants yiels the esire result. Finally, we consier the case of the uniform istribution on S 1. We enote by F the istribution function of the image measure of P = ω 1 H 1 uner the orthogonal S 1 projection map Π an let x 1 [ 1, 1]. Using the slice integration formula from Proposition 4, we obtain Fx 1 = 1 { } H 1 u S 1 : Πu [ 1, x ω S 1 1 ] = 1 1{Πu [ 1, x 1 ]}H 1 u ω S 1 S 1 = 1 ω x 1 1 = ω 1 ω 1 t 3 x 1 1 S 1 t 3 t. H S y t Differentiation with respect to x 1, together with the efinitions of ω an ω 1, complete the proof. In what follows, we shall enote by F H,β, F B,β an F U the istribution functions corresponing to the ensities f H,β, f B,β an f U compute in Lemma 6, respectively. Remark 7 The marginal ensities of the Gaussian istributions belonging to the class G can also be compute along the lines of the proof of Lemma 6. This yiels oneimensional Gaussian marginals. Since ranom convex hulls of Gaussian points have alreay been treate in [4], we ecie to concentrate on the classes H, B an U. 7

8 4 Proof of Theorem 1 an iscussion 4.1 Proof of Theorem 1 Base on the results from the two previous sections we are now able to present the proof of our main result. In what follows, we enote all constants by c. Unless otherwise state, they only epen on the space imension an the parameter β of the unerlying probability istribution. Their value might change from instance to instance. Proof of Theorem 1. For the classes G, H, B an U it is sufficient to consier the case that the scale parameter σ is equal to 1, since the mean facet number is invariant uner rescalings. We start with the istributions from class G. However, since this case has alreay been treate in [4], we refer to Theorem there. Next, we consier the heavy-taile istribution on R with ensity p H,β x H,,β 1+ x β, where β > / an c H,,β = π / start with the equality Γβ Γβ /. We follow the ieas from [4] an E f 1 P n = E = 1 i 1 <...<i n 1{convX i1,..., X i is a facet of P n } n PconvX 1,..., X is a facet of P n, 5 which hols ue to the fact that the ranom points X 1,..., X n are inepenent an ientically istribute. Let us enote by H A, 1 the affine hull of the 1- imensional simplex P spanne by X 1,..., X. In the case that P is a facet of P n, all the remaining points X +1,..., X n have to lie in one of the open half-spaces etermine by H. If we enote by Π H the orthogonal projection onto H, the orthogonal complement of H, we observe that P is a facet of P n if an only if the point Π H P is not containe in the interior of the interval Π H P n on H. Therefore, using Lemma 6, the affine Blaschke-Petkantschin formula from Proposition an the abbreviation F = F H,β Π H P, we get for the probability that P is a facet of P n, PconvX 1,..., X is a facet of P n = 1 F n +F n c H,,β 1+ x i β x 1,..., x i=1 R A, 1 H 1 F n +F n 1 x 1,..., x λ H x 1,..., x µ 1 H. i=1 c H,,β 1+ x i β Next, we use the theorem of Pythagoras to ecompose, for each i {1,..., }, the norm x i. Namely, writing H for the Eucliean norm in H A, 1 an h for the istance from H to the origin in R, we have that x i = x i H + h. 8

9 Therefore an as alreay use in the proof of Lemma 6, the last term of the integran can be rewritten as 1+ x i β = 1+h + x i H β = 1+h 1+ β x i β H 1+ h. 6 Moreover, since each hyperplane H = Hu, h is uniquely etermine by its unit normal vector u S 1 an its istance h [, to the origin, the integration over A, 1 can be replace by a twofol integral over S 1 an [,. Using the substitutions y i = x i / 1+h with λ H x i = 1+h 1/ λ H y i, the rotational invariance of the unerlying probability measure, an writing Fh for F H,β h as well as fh for f H,β h, gives in view of Lemma 6 that PconvX 1,..., X is a facet of P n S 1 S 1 H 1 Fh n + Fh n 1 x 1,..., x 1+h β c H,,β 1+ x i β H 1+h i=1 λ H x 1,..., x hh 1 u S 1 1 Fh n + Fh n 1+h 1 β + 1 hh 1 u S 1 β 1 y 1,..., y c H, 1,β 1+ y i H λ H y 1,..., y H i=1 1 Fh n + Fh n 1+h β h 1 Fh n fh 1+h 1 h, where we also use the fact that the integral over H is a finite constant given by Equation 7 in [1] an which only epens on the space imension an on β. Write now s = Fh an Ls = f F 1 s 1+F 1 s to obtain 1 PconvX 1,..., X is a facet of P n 1 s n Ls 1 s. Thus, combination of the above computation with 5 yiels the representation E f 1 P n E f 1 P n 1 1 [ ] n n 1 1 s 1 s n 1 Ls 1 s. In orer to apply Lemma 5, we have to verify that Ls is strictly concave on, 1. We prove this by showing that the secon erivative of Ls is negative. So, let c H,1,β := 9 7

10 Γβ π 1/ Γβ 1/ an recall that fx H,1,β1+ x 1 β from Lemma 6. Furthermore, from the efinition of F it follows that F 1 1 s = f F 1 s = c H,1,β 1+F 1 β s We recall that Ls = f F 1 s 1+F 1 s H,1,β 1+F 1 s β. Hence, using 8, the first erivative of Ls is L s H,1,β β 1+F 1 s β F 1 s F 1 s = β 1+F 1 s 1 F 1 s an, thus, for the secon erivative we fin that [ L s = β 1+F 1 s 1 F 1 s 1 1+F 1 s 3 ] F 1 s F 1 s = = c H,1,β = c H,1,β <, [ β F 1 s 1+F 1 s 1 β 1+F 1 s β 1 [ 1+F 1 s F 1 s ] 1+F 1 s β 1 β 1+F 1 s 3 ] F 1 s where the last inequality follows from the fact that β > /. As a consequence, we can apply Lemma 5 to euce that E f 1 P n E f 1 P n 1 1 [ ] n n 1 1 s 1 s n 1 Ls 1 s L/n > /n L/n = /n =, 1 1 n 1 n 1 s n 1 s 1 1 s n n B, n +1 n n B, n s where we use the well-known relation B, n +1 = n n B, n for the beta function. 1

11 As the next case we consier the class B of beta-type istribution on the unit ball B with ensity f B,β for some β > 1. In this case the proof follows almost line by line the proof for H, up to some minor moifications. In particular, 7 stays the same except that now Ls = f F 1 s 1 F 1 s, where Fh = F B,β h an fh = f B,β h. Therefore, it follows that L s = β+ 1 F 1 s β 1, c B,1,β where the constant c B,1,β is c B,1,β := π 1/ Γβ+ 3 Γβ Since F 1 s 1, 1, we obtain L s < an can conclue as in the proof for the class H presente above. Finally, we consier the case of the uniform istribution on S 1. Here we get by applying the spherical Blaschke-Petkantschin formula from Proposition 3 an using the abbreviations Fh = F U h an fh = f U h, PconvX 1,..., X is a facet of P n 1 Fh n + Fh n 1 x 1,..., x 1 h A, 1 H S 1 S 1 S H H S 1 x 1,..., x µ 1 H H S 1 1 Fh n + Fh n 1 x 1,..., x 1 h H H S 1 x 1,..., x hh 1 S 1 u 1 Fh n + Fh n 1 h + 1 hh 1 S 1 u 1 y 1,..., y H y S 1,..., y, S where the substitution x i = y i 1 h with H H S 1 x i = 1 h H H S 1 y i was use. In particular, this transforms the integration over H S 1 into a -fol integral over the unit sphere in H, which in turn has been ientifie with S ue to rotational invariance. Since the integral over S is a known positive constant only epening on the precise value can be euce from [14, Theorem 8..3], for example, we get by rotational invariance of the unerlying istribution that PconvX 1,..., X is a facet of P n Fh n + Fh n 1 h h 1 Fh n fh 1 h 1 h. 11

12 As a consequence, also for the uniform istribution on S 1 we arrive at an expression of the form 7, this time with Ls = ff 1 s 1 F 1 s. From this point on, the proof can be complete as in the case of the istribution class H or B. This completes the argument. 4. Discussion Let p : R [, enote a probability ensity. By a careful inspection of the proof of Theorem 1 we see that the following properties of the ensity p have been use there. First of all, we use that p is spherically symmetric, that is, px only epens on x = x 1,..., x R via x. By abuse of notation, we shall write pr :, [, with r = x x for the raial part of the ensity p. This was essential to apply the Blaschke-Petkantschin formulae, which use the invariant hyperplane measure µ 1. Moreover, given H A, 1 with istance h to the origin, we have use that we can fin ϕh, ψh > such that p r r + h = ϕh p 9 ψh for all r >. For example, for the ensity p H,β, β > /, the scaling property 9 is satisfie with ϕh = 1+h β an ψh = 1+ h, see 6. This scaling property was essential when we separate what happens within H from the contribution that arises from the istance of H to the origin. However, all rotationally symmetric ensities with almost everywhere ifferentiable raial part satisfying the scaling property 9 with an almost everywhere ifferentiable function ψ have been classifie by Miles [1] see p. 376 there an Ruben an Miles [13]. They precisely correspon to the istributions in the classes G, H, B as well as to the exceptional istributions in U, for which Theorem 1 is formulate. On the other han, this oes not mean that G, H, B an U contain the only rotationally symmetric istributions on R for which such computations are possible. For example, the ensity with raial part p β,j r β,,j r j /1+r β, r >, j {, 1,,...} an β > j+/, which oes not belong to the class H whenever j >, satisfies the following generalization of the scaling property 9: with ϕ k h = p β,j r + h = j r ϕ k hp β,k ψh k= j h k j 1+h β k =,..., j an ψh = 1+ h k. One can check that the 1-imensional marginal ensity of p β,j equals f β,j x 1 = j k= j cβ,,j x k j k c 1 1+ x 1 1 k+ β, β, 1,k an that from here on the argument base on the affine Blaschke-Petkantschin formula can be applie term-by-term. Unfortunately, the computations in such an similar situations become quite involve. Moreover, to classify all rotationally symmetric ensities on R for which these computations can be performe seems to be out of reach. 1

13 One might also ask whether the metho base on Blaschke-Petkantschin formulae yiels monotonicity of the mean facet number in such situations where the ranom points X 1,..., X n are inepenent with istributions belonging to one of the classes G, H, B an U, but not necessarily the same a so-calle mixe case. That is, some of the X i s are Gaussian, some istribute accoring to a istribution in H etc. but within each class we choose every time the same scale parameter σ. Unfortunately, this oes not work an, in fact, the metho breaks own. The reason is that each istribution class requires its iniviual substitution, which is aapte to its respective scaling property 9. The resulting ifferent rescalings in the hyperplane H istort the relationship between the 1-volume in H before an after the transformation, cf. [13]. 5 Ranom convex hulls on a half-sphere In this section we consier an application of Theorem 1 to convex hulls generate by ranom points on a half-sphere. We fix, enote by S the -imensional unit sphere in R +1 an efine the half-sphere S + = {y = y 1,..., y +1 S : y +1 > }. Furthermore, we let S be the class of probability istributions on S + that have ensity p S,α y S,α y α +1, y = y 1,..., y +1 S +, α > 1, with respect to the spherical Lebesgue measure on S +. Here, c S,α > is a suitable normalization constant. In particular, choosing α = shows that the uniform istribution on S + belongs to the class S. For fixe α > 1 an n + 1 we let X 1,..., X n be inepenent ranom points that are istribute on S + accoring to the ensity p S,α. By S n we enote the spherical convex hull of X 1,..., X n, that is, the smallest spherically convex set in S + containing the points X 1,..., X n. For the special choice α =, this moel has recently been stuie in [3]. In particular, it is shown in [3] that for this choice of α the mean number of facets E f 1 S n of the spherical ranom polytope S n converges to a finite constant only epening on, as n a similar result is in fact vali for all istributions in S, see [1, 6, 8]. As a special case, our next result shows the somewhat surprising fact that this limit is approache in a strictly monotone way. Theorem 8 Let X 1,..., X n, n +1, be inepenent an ientically istribute accoring to a probability measure belonging to the class S. Then, E f 1 S n > E f 1 S n 1. Proof. Let g : R S + be the mapping efine as x gx = 1,..., 1+ x x 1+ x, 1 1+ x, with inverse given by g 1 y = y1 y +1,..., y y +1 13

14 this is known as the gnomonic projection. Let Dg be the Jacobian matrix of g an put J g x := et Dgx Dgx. Then, it hols that J g x = 1+ x +1, see [5, Proposition 4.]. Moreover, for a measurable subset A R an a measurable function f : A R the area formula [9, Theorem 3..3] says that A fx x = ga f g 1 yj g g 1 y 1 H S +y. Next, we notice that 1+ g 1 y = y +1 an apply the formula with fx = p H,βx for some β > /: A c H,,β 1+ x β x = ga c H,,β y β 1 +1 H S +y, where c H,,β = π / Γβ/Γβ is the normalization constant of the ensity p H,β efine in 4. As a result, we see that the ensity p S,β 1 on S + is the push-forwar of the ensity p H,β on R uner g. Note also that β 1 > 1 since β > / an that the uniform measure on the half-sphere correspons to the choice β = + 1/. The above iscussion shows the following. Let P n be the ranom convex hull in R generate by n inepenent points with ensity p H,β. Then, the push-forwar of P n has the same istribution as the spherical ranom polytope S n with α = β 1. Moreover, the facets of P n are in one-to-one corresponence with those of S n. As a consequence, the mean facet number of the spherical ranom polytope S n is the same as the mean facet number of the ranom convex hull P n, i.e., E f 1 S n = E f 1 P n. Thus, the monotonicity follows from Theorem 1. Acknowlegement We woul like to thank Zakhar Kabluchko Münster for a number of useful conversations an for bringing references [8] an [13] to our attention. Thanks go also to Matthias Reitzner Osnabrück for his valuable remarks on an earlier version of this text. JG, DT an NT have been supporte by the Deutsche Forschungsgemeinschaft DFG via RTG 131 High-imensional Phenomena in Probability Fluctuations an Discontinuity. References [1] Alous, D., Fristet, D., Griffin, P. an Pruitt, W.: The number of extreme points in the convex hull of a ranom sample. J. Appl. Probab. 8, [] Axler, S., Bouron, P. an Ramey, W.: Harmonic Function Theory. Volume 137 of Grauate Texts in Mathematics, Springer, New York, secon eition 1 14

15 [3] Bárány, I., Hug, D., Reitzner, M. an Schneier, R.: Ranom points in halfspheres. Ranom Structures Algorithms 5, [4] Beermann, M.: Ranom Polytopes. Dissertation, University of Osnabrück 14. [5] Besau, F. an Werner, W.: The spherical convex floating boy. Av. Math. 31, [6] Carnal, H.: Die konvexe Hülle von n rotationssymmetrisch verteilten Punkten. Z. Wahrscheinlichkeitstheorie verw. Geb. 15, [7] Devillers, O., Glisse, M., Goaoc, X., Moroz, G. an Reitzner, M.: The monotonicity of f-vectors of ranom polytopes. Electron. Commun. Probab. 18, article [8] Ey, W.F. an Gale, J.D.: The convex hull of a spherically symmetric sample. Av. in Appl. Probab. 13, [9] Feerer, H.: Geometric Measure Theory. Springer, Berlin [1] Miles, R.E.: Isotropic ranom simplices. Av. in Appl. Probab. 3, [11] Raemacher, L.: On the monotonicity of the expecte volume of a ranom simplex. Mathematika 58, [1] Reichenwallner, B. an Reitzner, M.: On the monotonicity of the moments of volumes of ranom simplices. Mathematika 6, [13] Ruben, H. an Miles, R.E.: A canonical ecomposition of the probability measure of sets of isotropic ranom points in R n. J. Multivariate Anal. 1, [14] Schneier, R. an Weil, W.: Stochastic an Integral Geometry. Springer, Berlin 8. [15] Zähle, M.: A kinematic formula an moment measures of ranom sets. Math. Nachr. 149,

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

arxiv: v3 [math.mg] 3 Nov 2017

arxiv: v3 [math.mg] 3 Nov 2017 arxiv:702.0069v3 [math.mg] 3 ov 207 Random polytopes: central limit theorems for intrinsic volumes Christoph Thäle, icola Turchi and Florian Wespi Abstract Short and transparent proofs of central limit

More information

Gaussian polytopes: variances and limit theorems

Gaussian polytopes: variances and limit theorems Gaussian polytopes: variances an limit theorems Daniel Hug an Matthias Reitzner October 9, 4 Abstract The convex hull of n inepenent ranom points in R chosen accoring to the normal istribution is calle

More information

Large Cells in Poisson-Delaunay Tessellations

Large Cells in Poisson-Delaunay Tessellations Large Cells in Poisson-Delaunay Tessellations Daniel Hug an Rolf Schneier Mathematisches Institut, Albert-Luwigs-Universität, D-79104 Freiburg i. Br., Germany aniel.hug, rolf.schneier}@math.uni-freiburg.e

More information

LECTURE NOTES ON DVORETZKY S THEOREM

LECTURE NOTES ON DVORETZKY S THEOREM LECTURE NOTES ON DVORETZKY S THEOREM STEVEN HEILMAN Abstract. We present the first half of the paper [S]. In particular, the results below, unless otherwise state, shoul be attribute to G. Schechtman.

More information

arxiv: v1 [math.mg] 10 Apr 2018

arxiv: v1 [math.mg] 10 Apr 2018 ON THE VOLUME BOUND IN THE DVORETZKY ROGERS LEMMA FERENC FODOR, MÁRTON NASZÓDI, AND TAMÁS ZARNÓCZ arxiv:1804.03444v1 [math.mg] 10 Apr 2018 Abstract. The classical Dvoretzky Rogers lemma provies a eterministic

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

Acute sets in Euclidean spaces

Acute sets in Euclidean spaces Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of

More information

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

LARGE TYPICAL CELLS IN POISSON DELAUNAY MOSAICS

LARGE TYPICAL CELLS IN POISSON DELAUNAY MOSAICS LARGE TYPICAL CELLS IN POISSON DELAUNAY MOSAICS DANIEL HUG an ROLF SCHNEIDER Deicate to Tuor Zamfirescu on the occasion of his sixtieth birthay It is prove that the shape of the typical cell of a Poisson

More information

arxiv: v1 [math.mg] 27 Jan 2016

arxiv: v1 [math.mg] 27 Jan 2016 On the monotonicity of the moments of volumes of random simplices arxiv:67295v [mathmg] 27 Jan 26 Benjamin Reichenwallner and Matthias Reitzner University of Salzburg and University of Osnabrueck Abstract

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower Bounds for the Smoothed Number of Pareto optimal Solutions Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.

More information

Lower bounds on Locality Sensitive Hashing

Lower bounds on Locality Sensitive Hashing Lower bouns on Locality Sensitive Hashing Rajeev Motwani Assaf Naor Rina Panigrahy Abstract Given a metric space (X, X ), c 1, r > 0, an p, q [0, 1], a istribution over mappings H : X N is calle a (r,

More information

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

WUCHEN LI AND STANLEY OSHER

WUCHEN LI AND STANLEY OSHER CONSTRAINED DYNAMICAL OPTIMAL TRANSPORT AND ITS LAGRANGIAN FORMULATION WUCHEN LI AND STANLEY OSHER Abstract. We propose ynamical optimal transport (OT) problems constraine in a parameterize probability

More information

Tractability results for weighted Banach spaces of smooth functions

Tractability results for weighted Banach spaces of smooth functions Tractability results for weighte Banach spaces of smooth functions Markus Weimar Mathematisches Institut, Universität Jena Ernst-Abbe-Platz 2, 07740 Jena, Germany email: markus.weimar@uni-jena.e March

More information

FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction

FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS ALINA BUCUR, CHANTAL DAVID, BROOKE FEIGON, MATILDE LALÍN 1 Introuction In this note, we stuy the fluctuations in the number

More information

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz

A note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz A note on asymptotic formulae for one-imensional network flow problems Carlos F. Daganzo an Karen R. Smilowitz (to appear in Annals of Operations Research) Abstract This note evelops asymptotic formulae

More information

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,

NOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy, NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

Lower Bounds for k-distance Approximation

Lower Bounds for k-distance Approximation Lower Bouns for k-distance Approximation Quentin Mérigot March 21, 2013 Abstract Consier a set P of N ranom points on the unit sphere of imension 1, an the symmetrize set S = P ( P). The halving polyheron

More information

Discrete Mathematics

Discrete Mathematics Discrete Mathematics 309 (009) 86 869 Contents lists available at ScienceDirect Discrete Mathematics journal homepage: wwwelseviercom/locate/isc Profile vectors in the lattice of subspaces Dániel Gerbner

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

Multi-View Clustering via Canonical Correlation Analysis

Multi-View Clustering via Canonical Correlation Analysis Technical Report TTI-TR-2008-5 Multi-View Clustering via Canonical Correlation Analysis Kamalika Chauhuri UC San Diego Sham M. Kakae Toyota Technological Institute at Chicago ABSTRACT Clustering ata in

More information

Least-Squares Regression on Sparse Spaces

Least-Squares Regression on Sparse Spaces Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction

More information

A LIMIT THEOREM FOR RANDOM FIELDS WITH A SINGULARITY IN THE SPECTRUM

A LIMIT THEOREM FOR RANDOM FIELDS WITH A SINGULARITY IN THE SPECTRUM Teor Imov r. ta Matem. Statist. Theor. Probability an Math. Statist. Vip. 81, 1 No. 81, 1, Pages 147 158 S 94-911)816- Article electronically publishe on January, 11 UDC 519.1 A LIMIT THEOREM FOR RANDOM

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

Agmon Kolmogorov Inequalities on l 2 (Z d ) Journal of Mathematics Research; Vol. 6, No. ; 04 ISSN 96-9795 E-ISSN 96-9809 Publishe by Canaian Center of Science an Eucation Agmon Kolmogorov Inequalities on l (Z ) Arman Sahovic Mathematics Department,

More information

Some Examples. Uniform motion. Poisson processes on the real line

Some Examples. Uniform motion. Poisson processes on the real line Some Examples Our immeiate goal is to see some examples of Lévy processes, an/or infinitely-ivisible laws on. Uniform motion Choose an fix a nonranom an efine X := for all (1) Then, {X } is a [nonranom]

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

Math 1271 Solutions for Fall 2005 Final Exam

Math 1271 Solutions for Fall 2005 Final Exam Math 7 Solutions for Fall 5 Final Eam ) Since the equation + y = e y cannot be rearrange algebraically in orer to write y as an eplicit function of, we must instea ifferentiate this relation implicitly

More information

The Press-Schechter mass function

The Press-Schechter mass function The Press-Schechter mass function To state the obvious: It is important to relate our theories to what we can observe. We have looke at linear perturbation theory, an we have consiere a simple moel for

More information

Math 1B, lecture 8: Integration by parts

Math 1B, lecture 8: Integration by parts Math B, lecture 8: Integration by parts Nathan Pflueger 23 September 2 Introuction Integration by parts, similarly to integration by substitution, reverses a well-known technique of ifferentiation an explores

More information

d dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1

d dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1 Lecture 5 Some ifferentiation rules Trigonometric functions (Relevant section from Stewart, Seventh Eition: Section 3.3) You all know that sin = cos cos = sin. () But have you ever seen a erivation of

More information

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the

More information

An Optimal Algorithm for Bandit and Zero-Order Convex Optimization with Two-Point Feedback

An Optimal Algorithm for Bandit and Zero-Order Convex Optimization with Two-Point Feedback Journal of Machine Learning Research 8 07) - Submitte /6; Publishe 5/7 An Optimal Algorithm for Banit an Zero-Orer Convex Optimization with wo-point Feeback Oha Shamir Department of Computer Science an

More information

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu

More information

7.1 Support Vector Machine

7.1 Support Vector Machine 67577 Intro. to Machine Learning Fall semester, 006/7 Lecture 7: Support Vector Machines an Kernel Functions II Lecturer: Amnon Shashua Scribe: Amnon Shashua 7. Support Vector Machine We return now to

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

Sturm-Liouville Theory

Sturm-Liouville Theory LECTURE 5 Sturm-Liouville Theory In the three preceing lectures I emonstrate the utility of Fourier series in solving PDE/BVPs. As we ll now see, Fourier series are just the tip of the iceberg of the theory

More information

Topic 7: Convergence of Random Variables

Topic 7: Convergence of Random Variables Topic 7: Convergence of Ranom Variables Course 003, 2016 Page 0 The Inference Problem So far, our starting point has been a given probability space (S, F, P). We now look at how to generate information

More information

Quantum Mechanics in Three Dimensions

Quantum Mechanics in Three Dimensions Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

The Principle of Least Action

The Principle of Least Action Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of

More information

Schrödinger s equation.

Schrödinger s equation. Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control 19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior

More information

arxiv: v4 [math.pr] 27 Jul 2016

arxiv: v4 [math.pr] 27 Jul 2016 The Asymptotic Distribution of the Determinant of a Ranom Correlation Matrix arxiv:309768v4 mathpr] 7 Jul 06 AM Hanea a, & GF Nane b a Centre of xcellence for Biosecurity Risk Analysis, University of Melbourne,

More information

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu ARCHIVUM MATHEMATICUM (BRNO Tomus 46 (21, 177 184 SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE Bing Ye Wu Abstract. In this paper we stuy the geometry of Minkowski plane an obtain some results. We focus

More information

arxiv: v4 [cs.ds] 7 Mar 2014

arxiv: v4 [cs.ds] 7 Mar 2014 Analysis of Agglomerative Clustering Marcel R. Ackermann Johannes Blömer Daniel Kuntze Christian Sohler arxiv:101.697v [cs.ds] 7 Mar 01 Abstract The iameter k-clustering problem is the problem of partitioning

More information

u!i = a T u = 0. Then S satisfies

u!i = a T u = 0. Then S satisfies Deterministic Conitions for Subspace Ientifiability from Incomplete Sampling Daniel L Pimentel-Alarcón, Nigel Boston, Robert D Nowak University of Wisconsin-Maison Abstract Consier an r-imensional subspace

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

05 The Continuum Limit and the Wave Equation

05 The Continuum Limit and the Wave Equation Utah State University DigitalCommons@USU Founations of Wave Phenomena Physics, Department of 1-1-2004 05 The Continuum Limit an the Wave Equation Charles G. Torre Department of Physics, Utah State University,

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

A. Incorrect! The letter t does not appear in the expression of the given integral

A. Incorrect! The letter t does not appear in the expression of the given integral AP Physics C - Problem Drill 1: The Funamental Theorem of Calculus Question No. 1 of 1 Instruction: (1) Rea the problem statement an answer choices carefully () Work the problems on paper as neee (3) Question

More information

Solution to the exam in TFY4230 STATISTICAL PHYSICS Wednesday december 1, 2010

Solution to the exam in TFY4230 STATISTICAL PHYSICS Wednesday december 1, 2010 NTNU Page of 6 Institutt for fysikk Fakultet for fysikk, informatikk og matematikk This solution consists of 6 pages. Solution to the exam in TFY423 STATISTICAL PHYSICS Wenesay ecember, 2 Problem. Particles

More information

GLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS

GLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS Electronic Journal of Differential Equations, Vol. 015 015), No. 99, pp. 1 14. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu GLOBAL SOLUTIONS FOR D COUPLED

More information

REAL ANALYSIS I HOMEWORK 5

REAL ANALYSIS I HOMEWORK 5 REAL ANALYSIS I HOMEWORK 5 CİHAN BAHRAN The questions are from Stein an Shakarchi s text, Chapter 3. 1. Suppose ϕ is an integrable function on R with R ϕ(x)x = 1. Let K δ(x) = δ ϕ(x/δ), δ > 0. (a) Prove

More information

A simple tranformation of copulas

A simple tranformation of copulas A simple tranformation of copulas V. Durrleman, A. Nikeghbali & T. Roncalli Groupe e Recherche Opérationnelle Créit Lyonnais France July 31, 2000 Abstract We stuy how copulas properties are moifie after

More information

Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs

Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Ashish Goel Michael Kapralov Sanjeev Khanna Abstract We consier the well-stuie problem of fining a perfect matching in -regular bipartite

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

Quantile function expansion using regularly varying functions

Quantile function expansion using regularly varying functions Quantile function expansion using regularly varying functions arxiv:705.09494v [math.st] 9 Aug 07 Thomas Fung a, an Eugene Seneta b a Department of Statistics, Macquarie University, NSW 09, Australia b

More information

Vectors in two dimensions

Vectors in two dimensions Vectors in two imensions Until now, we have been working in one imension only The main reason for this is to become familiar with the main physical ieas like Newton s secon law, without the aitional complication

More information

Physics 251 Results for Matrix Exponentials Spring 2017

Physics 251 Results for Matrix Exponentials Spring 2017 Physics 25 Results for Matrix Exponentials Spring 27. Properties of the Matrix Exponential Let A be a real or complex n n matrix. The exponential of A is efine via its Taylor series, e A A n = I + n!,

More information

Calculus of Variations

Calculus of Variations Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,

More information

On the number of isolated eigenvalues of a pair of particles in a quantum wire

On the number of isolated eigenvalues of a pair of particles in a quantum wire On the number of isolate eigenvalues of a pair of particles in a quantum wire arxiv:1812.11804v1 [math-ph] 31 Dec 2018 Joachim Kerner 1 Department of Mathematics an Computer Science FernUniversität in

More information

LOCAL AND GLOBAL MINIMALITY RESULTS FOR A NONLOCAL ISOPERIMETRIC PROBLEM ON R N

LOCAL AND GLOBAL MINIMALITY RESULTS FOR A NONLOCAL ISOPERIMETRIC PROBLEM ON R N LOCAL AND GLOBAL MINIMALITY RSULTS FOR A NONLOCAL ISOPRIMTRIC PROBLM ON R N M. BONACINI AND R. CRISTOFRI Abstract. We consier a nonlocal isoperimetric problem efine in the whole space R N, whose nonlocal

More information

Least Distortion of Fixed-Rate Vector Quantizers. High-Resolution Analysis of. Best Inertial Profile. Zador's Formula Z-1 Z-2

Least Distortion of Fixed-Rate Vector Quantizers. High-Resolution Analysis of. Best Inertial Profile. Zador's Formula Z-1 Z-2 High-Resolution Analysis of Least Distortion of Fixe-Rate Vector Quantizers Begin with Bennett's Integral D 1 M 2/k Fin best inertial profile Zaor's Formula m(x) λ 2/k (x) f X(x) x Fin best point ensity

More information

arxiv: v1 [physics.flu-dyn] 8 May 2014

arxiv: v1 [physics.flu-dyn] 8 May 2014 Energetics of a flui uner the Boussinesq approximation arxiv:1405.1921v1 [physics.flu-yn] 8 May 2014 Kiyoshi Maruyama Department of Earth an Ocean Sciences, National Defense Acaemy, Yokosuka, Kanagawa

More information

Introduction to variational calculus: Lecture notes 1

Introduction to variational calculus: Lecture notes 1 October 10, 2006 Introuction to variational calculus: Lecture notes 1 Ewin Langmann Mathematical Physics, KTH Physics, AlbaNova, SE-106 91 Stockholm, Sween Abstract I give an informal summary of variational

More information

inflow outflow Part I. Regular tasks for MAE598/494 Task 1

inflow outflow Part I. Regular tasks for MAE598/494 Task 1 MAE 494/598, Fall 2016 Project #1 (Regular tasks = 20 points) Har copy of report is ue at the start of class on the ue ate. The rules on collaboration will be release separately. Please always follow the

More information

Monotonicity for excited random walk in high dimensions

Monotonicity for excited random walk in high dimensions Monotonicity for excite ranom walk in high imensions Remco van er Hofsta Mark Holmes March, 2009 Abstract We prove that the rift θ, β) for excite ranom walk in imension is monotone in the excitement parameter

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay

More information

arxiv: v1 [math.co] 15 Sep 2015

arxiv: v1 [math.co] 15 Sep 2015 Circular coloring of signe graphs Yingli Kang, Eckhar Steffen arxiv:1509.04488v1 [math.co] 15 Sep 015 Abstract Let k, ( k) be two positive integers. We generalize the well stuie notions of (k, )-colorings

More information

Iterated Point-Line Configurations Grow Doubly-Exponentially

Iterated Point-Line Configurations Grow Doubly-Exponentially Iterate Point-Line Configurations Grow Doubly-Exponentially Joshua Cooper an Mark Walters July 9, 008 Abstract Begin with a set of four points in the real plane in general position. A to this collection

More information

3 The variational formulation of elliptic PDEs

3 The variational formulation of elliptic PDEs Chapter 3 The variational formulation of elliptic PDEs We now begin the theoretical stuy of elliptic partial ifferential equations an bounary value problems. We will focus on one approach, which is calle

More information

Chapter 6: Energy-Momentum Tensors

Chapter 6: Energy-Momentum Tensors 49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.

More information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:

More information

Function Spaces. 1 Hilbert Spaces

Function Spaces. 1 Hilbert Spaces Function Spaces A function space is a set of functions F that has some structure. Often a nonparametric regression function or classifier is chosen to lie in some function space, where the assume structure

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

arxiv:hep-th/ v1 3 Feb 1993

arxiv:hep-th/ v1 3 Feb 1993 NBI-HE-9-89 PAR LPTHE 9-49 FTUAM 9-44 November 99 Matrix moel calculations beyon the spherical limit arxiv:hep-th/93004v 3 Feb 993 J. Ambjørn The Niels Bohr Institute Blegamsvej 7, DK-00 Copenhagen Ø,

More information

Existence of equilibria in articulated bearings in presence of cavity

Existence of equilibria in articulated bearings in presence of cavity J. Math. Anal. Appl. 335 2007) 841 859 www.elsevier.com/locate/jmaa Existence of equilibria in articulate bearings in presence of cavity G. Buscaglia a, I. Ciuperca b, I. Hafii c,m.jai c, a Centro Atómico

More information

Convergence rates of moment-sum-of-squares hierarchies for optimal control problems

Convergence rates of moment-sum-of-squares hierarchies for optimal control problems Convergence rates of moment-sum-of-squares hierarchies for optimal control problems Milan Kora 1, Diier Henrion 2,3,4, Colin N. Jones 1 Draft of September 8, 2016 Abstract We stuy the convergence rate

More information

arxiv: v2 [math.cv] 2 Mar 2018

arxiv: v2 [math.cv] 2 Mar 2018 The quaternionic Gauss-Lucas Theorem Riccaro Ghiloni Alessanro Perotti Department of Mathematics, University of Trento Via Sommarive 14, I-38123 Povo Trento, Italy riccaro.ghiloni@unitn.it, alessanro.perotti@unitn.it

More information

SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES

SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES Communications on Stochastic Analysis Vol. 2, No. 2 (28) 289-36 Serials Publications www.serialspublications.com SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES

More information

SMOOTHED PROJECTIONS OVER WEAKLY LIPSCHITZ DOMAINS

SMOOTHED PROJECTIONS OVER WEAKLY LIPSCHITZ DOMAINS SMOOHED PROJECIONS OVER WEAKLY LIPSCHIZ DOMAINS MARIN WERNER LICH Abstract. We evelop finite element exterior calculus over weakly Lipschitz omains. Specifically, we construct commuting projections from

More information

1 Heisenberg Representation

1 Heisenberg Representation 1 Heisenberg Representation What we have been ealing with so far is calle the Schröinger representation. In this representation, operators are constants an all the time epenence is carrie by the states.

More information

1. Aufgabenblatt zur Vorlesung Probability Theory

1. Aufgabenblatt zur Vorlesung Probability Theory 24.10.17 1. Aufgabenblatt zur Vorlesung By (Ω, A, P ) we always enote the unerlying probability space, unless state otherwise. 1. Let r > 0, an efine f(x) = 1 [0, [ (x) exp( r x), x R. a) Show that p f

More information

arxiv: v2 [cond-mat.stat-mech] 11 Nov 2016

arxiv: v2 [cond-mat.stat-mech] 11 Nov 2016 Noname manuscript No. (will be inserte by the eitor) Scaling properties of the number of ranom sequential asorption iterations neee to generate saturate ranom packing arxiv:607.06668v2 [con-mat.stat-mech]

More information

On combinatorial approaches to compressed sensing

On combinatorial approaches to compressed sensing On combinatorial approaches to compresse sensing Abolreza Abolhosseini Moghaam an Hayer Raha Department of Electrical an Computer Engineering, Michigan State University, East Lansing, MI, U.S. Emails:{abolhos,raha}@msu.eu

More information