MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX

Size: px
Start display at page:

Download "MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX"

Transcription

1 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX J. WILLIAM HELTON, JEAN B. LASSERRE, AND MIHAI PUTINAR Abstract. We investigate an iscuss when the inverse of a multivariate truncate moment matrix of a measure µ has zeros in some prescribe entries. We escribe precisely which pattern of these zeroes correspons to inepenence, namely, the measure having a prouct structure. A more refine fining is that the key factor forcing a zero entry in this inverse matrix is a certain conitional triangularity property of the orthogonal polynomials associate with the measure µ. 1. Introuction It is well known that zeros in off-iagonal entries of the inverse M 1 of a n n covariance matrix M ientify pairs of ranom variables that have no partial correlation (an so are conitionally inepenent in case of normally istribute vectors); see e.g. Wittaker[7, Cor ]. Allowing zeros in the off-iagonal entries of M 1 is particularly useful for Bayesian estimation of regression moels in statistics, an is calle Bayesian covariance selection. Inee, estimating a covariance matrix is a ifficult problem for large number of variables, an exploiting sparsity in M 1 may yiel efficient methos for Graphical Gaussian Moels (GGM). For more etails, the intereste reaer is referre to Cripps et al. [3], an the many references therein. The covariance matrix can be thought of as a matrix whose entries are secon moments of a measure. This paper focuses on the truncate moment matrices, M, consisting of moments up to an orer etermine by. First we escribe precisely the pattern of zeroes of M 1 resulting from the measure having a prouct type structure. Next we turn to the stuy of a particular entry of M 1 being zero. We fin that the key is what we call the conitional triangularity property of orthonormal polynomials (OP) up to egree 2, associate with the measure. To give the flavor of what 1991 Mathematics Subject Classification. 52A20 52A. Key wors an phrases. Moment matrix; orthogonal polynomials. This work was initiate at Banff Research Station (Canaa) uring a workshop on Positive Polynomials, an complete at the Institute for Mathematics an its Applications (IMA, Minneapolis). All three authors wish to thank both institutes for their excellent working conitions an financial support. J.W. Helton was partially supporte by the NSF an For Motor Co., M. Putinar by the NSF an J.B. Lasserre by the (French) ANR. 1

2 2 HELTON, LASSERRE, AND PUTINAR this means, let for instance µ be the joint istribution µ of n ranom variables X = (X 1,..., X n ), an let {p σ } R[X] be its associate family of orthonormal polynomials. When (X k ) k i,j is fixe, they can be viewe as polynomials in R[X i, X j ]. If in oing so they exhibit a triangular structure (whence the name conitional triangularity w.r.t. (X k ) k i,j ), then entries of M 1 at precise locations vanish. Conversely, if these precise entries of M 1 vanish (robustly to perturbation), then the conitional triangularity w.r.t. (X k ) k i,j hols. An so, for the covariance matrix case = 1, this conitional triangularity property is equivalent to the zero partial correlation property well stuie in statistics (whereas in general, conitional inepenence is not etecte by zeros in the inverse of the covariance matrix). Interestingly, in a ifferent irection, one may relate this issue with a constraine matrix completion problem. Namely, given that the entries of M corresponing to marginals of the linear functional w.r.t. one variable at a time, are fixe, complete the missing entries with values that make M positive efinite. This is a constraine matrix completion problem as one has to respect the moment matrix structure when filling up the missing entries. Usually, for the classical matrix completion problem with no constraint on M, the solution which maxmizes an appropriate entropy, gives zeros to entries of M 1 corresponing to missing entries of M. But uner the aitional constraint of respecting the moment matrix structure, the maximum entropy solution oes not always fill in M 1 with zeros at the corresponing entries (as seen in examples by the authors). Therefore, any solution of this constraine matrix completion problem oes not always maximize the entropy. Its physical or probabilistic interpretation is still to be unerstoo. We point out another accomplishment of this paper. More generally than working with a measure is working with a linear functional l on the space of polynomials. One can consier moments with respect to l an moment matrices. Our results hol at this level of generality. 2. Notation an efinitions For a real symmetric matrix A R n n, the notation A 0 (resp. A 0) stans for A positive efinite (resp. semiefinite), an for a matrix B, let B or B T enote its transpose Monomials an polynomials. We now iscuss monomials at some length, since they are use in many ways, even to inex the moment matrices which are the subject of this paper. Let N enote the nonnegative integers an N n enote n tuples of them an for α = (α 1, α 2 α n ) N n, efine α := i α i. The set N n sits in one to one corresponence with the monomials via α N n X α := X α 1 1 Xα 2 2 X αn n.

3 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 3 Recall also the stanar notation eg X α = α = α α n. By abuse of notation we will freely interchange below X α with α, for instance speaking about eg α rather than eg X α, an so on. Define the the fully grae partial orer (FG orer), on monomials, or equivalently for γ, α N n by γ α, iff γ j α j for all j = 1,, g. Important to us is: α β iff X α ivies X β. Define the the grae lexicographic orer (GLex) < gl, on monomials, or equivalently for γ, α N n first by using eg γ eg α to create a partial orer. Next refine this to a total orer by breaking ties in two monomials X m 1, X m 2 of same egree m 1 = m 2, as woul a ictionary with X 1 = a, X 2 = b,. Beware γ < gl α oes not imply γ α; for example, (1, 1, 3) < gl (1, 3, 1) but fails. However, β α an β α implies β < gl α. It is convenient to list all monomials as an infinite vector v (X) := (X α ) α N n where the entries are liste in GLex orer, henceforth calle the tautological vector; v (X) = (X α ) α R s() enotes the finite vector consisting of the part of v (X) containing exactly the egree monomials. Let R[X] enote the ring of real polynomials in the variables X 1,..., X n an let R [X] R[X] be the R-vector space of polynomials of egree at most. A polynomial is a linear combination of polynomials an g R[X] can be written (2.1) g(x) = g α X α = g, v (X) α N n for some real vector g = (g α ), where the latter is the stanar non-egenerate pairing between R s() an R s() R R[X] Moment matrix. Let y = (y α ) α N n (i.e. a sequence inexe with respect to the orering GLex), an efine the linear functional L y : R[X] R to be: (2.2) g L y (g) := α N n g α y α, whenever g is as in (2.1). Given a sequence y = (y α ) α N n, the moment matrix M (y) associate with y has its rows an columns inexe by α, α, an M (y)(α, β) := L y (X α X β ) = y α+β, α, β N n with α, β.

4 4 HELTON, LASSERRE, AND PUTINAR For example, M 2 (y) is 1 X 1 X 2 X 2 1 X 1 X 2 X 2 2 M 2 (y) : 1 1 y 10 y 01 y 20 y 11 y 02 X 1 y 10 y 20 y 11 y 30 y 21 y 12 X 2 y 01 y 11 y 02 y 21 y 12 y 03 X1 2 y 20 y 30 y 21 y 40 y 31 y 22 X 1 X 2 y 11 y 21 y 12 y 31 y 22 y 13 X2 2 y 02 y 12 y 03 y 22 y 13 y 04 A sequence y is sai to have a representing measure µ on R n if y α = x α µ(x), α N n, R n assuming of course that the signe measure µ ecays fast enough at infinity, so that all monomials are integrable with respect to its total variation. Note that the functional L y prouces for every 0 a positive semiefinite moment matrix M (y) if an only if L y (P 2 ) 0, P R[X]. The associate matrices M (y) are positive efinite, for all 0 if an only if L y (P 2 ) = 0 implies P = 0. We will istinguish this latter case by calling L y a positive functional. 3. Measures of prouct form In this section, given a sequence y = (y α ) inexe by α, α 2, we investigate some properties of the the inverse M (y) 1 of a positive efinite moment matrix M (y) when entries of the latter satisfy a prouct form property. Definition 1. We say that the variables X = (X 1,..., X n ) are mutually inepenent, an the moment matrix M (y) 0 has the prouct form property, if (3.1) L y (X α ) = n i=1 L y (X α i i ), α N n, α 2. If M (y) 1 (α, β) = 0 for every y such that M (y) 0 has the prouct form property, then we say the pair (α, β) is a congenital zero for -moments. We can now state an intermeiate result. Theorem 1. The pair α, β is a congenital zero for the - moment problem if an only if the least common multiple X η of X α an X β has egree bigger than.

5 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 5 The above result can be conveniently rephrase in terms the max operation efine for α, β N n by max(α, β) := (max(α j, β j )) j=1,,n. Set η := max(α, β). Simple observations about this operation are: (1) X η is the least common multiple of X α an X β, (2) X α ivies X β iff X β = X η, X β ivies X α iff X α = X η, (3) η = n j=1 max(α j, β j ). Thus, Theorem 1 asserts that the entry (α, β) oes not correspon to a congenital zero in the matrix M (y) 1 if an only if max(α, β). Later in Theorem 4 we show that this LCM (least common multiple) characterization of zeros in M 1 is equivalent to a highly triangular structure of orthonormal polynomials associate with prouct measures. Example. In the case of M2 1 (y) in two variables X 1, X 2 we inicate below which entries M 2 (y) 1 (α, β) with β = 2, are congenital zeroes. These (α, β) inex the last three columns of M 2 (y) 1 an are X 2 1 X 1 X 2 X X 1 0 X 2 0 X X 1 X X Here means that the corresponing entry can be ifferent from zero. Note each correspons to X α failing to ivie X β. The proof relies on properties of orthogonal polynomials, so we begin by explaining in some etail the framework Orthonormal polynomials. A functional analytic viewpoint to polynomials is expeitious, so we begin with that. Let s() := ( ) n+ be the imension of vector space R [X]. Let, R s() enote the stanar inner prouct on R s(). Let f, h R[X] be the polynomials f(x) = s() α =0 f αx α an h(x) = s() α =0 h αx α. Then, f, h y := f, M (y)h R s() = L y (f(x)h(x)), efines a scalar prouct in R [X], provie M (y) is positive efinite. With a given y = (y α ) such that M (y) 0, one may associate a unique family (p α ) s() α =0 of orthonormal polynomials. That is, the p α s satisfy:

6 6 HELTON, LASSERRE, AND PUTINAR (3.2) p α lin.span{x β ; β gl α}, p α, p β y = δ αβ, α, β, p α, X β y = 0, if β < gl α, p α, X α y > 0, Note p α, X β y = 0, if β α an α β, since the latter implies β < gl α. Existence an uniqueness of such a family is guarantee by the Gram- Schmit orthonormalization process following the GLex orer on the monomials, an by the positivity of the moment (covariance) matrix, see for instance [1, Theorem , p. 68]. Computation. Suppose that we want to compute the orthonormal polynomials p σ for some inex σ. Then procee as follows: buil up the submoment matrix M (σ) (y) with columns inexe by all monomials β gl σ, an rows inexe by all monomials α < gl σ. Hence, M (σ) (y) has one row less than columns. Next, complete M (σ) (y) with an aitional last row escribe by [M (σ) (y)] σ,β = X β, for all β gl σ. Then up to a normalizing constant, p σ is nothing less than et (M σ (y)). To see this, let γ < gl σ. Then X γ p σ (X) µ(x) = et (B σ )(y), where the matrix B σ (y) is the same as M σ (y) except for the last row which is now the vector (L y (X γ+α )) α gl σ, alreay present in one of the rows above. Therefore, et (B σ )(y) = 0. Next, writing p σ (X) = ρ σβ X β, β gl σ its coefficient ρ σβ is just (again up to a normalizing constant) the cofactor of the element [M σ (y)] 1,β in the square matrix M σ (y) with rows an columns both inexe with α gl σ. Further properties. Now we give further properties of the orthonormal polynomials. Consier first one variable polynomials. The orthogonal polynomials p k have, by their very efinition a triangular form, namely p k (X 1 ) := l k ρ kl X l 1. The orthonormal polynomials inherit the prouct form property of M r (y), assuming that the latter hols. Namely, each orthonormal polynomial p α is a prouct (3.3) p α (X) = p α1 (X 1 )p α2 (X 2 ) p αn (X n )

7 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 7 of orthogonal polynomials p αj (X j ) in one imension. Inee, by the prouct property n p α1 (X 1 )p α2 (X 2 ) p αn (X n ), X β y = p αj (X j ), X β j j y, whence the prouct of single variable orthogonal polynomials satisfies all requirements liste in 3.2. Triangularity in one variable an the prouct form property (3.3) forces p α to have what we call a fully triangular form: j=1 (3.4) p α (X) := γ α ρ αγ X γ, α. Also note that for any γ α there is a linear functional L y of prouct type making ρ αγ not zero. In orer to construct such a functional we consier first the Laguerre polynomials in one variable L (σ), that is L (σ) k (x) = ex x σ k k! x k (e x x n+σ ) = k j=0 k ( k + σ k j ) ( x) j. j! These polynomials satisfy an orthogonality conition on the semi-axis R +, with respect to the weight e x x σ, see for instance [4]. Remark that the egree in σ of the coefficient of x j is precisely k j. Thus the functional L y (p) = p(x 1,..., x n )e x 1... x n x σ xσn n x 1...x n, p R[X], R + n will have the property, that is the associate (Laguerre σ ) orthogonal polynomials are Λ α (X) = n j=1 L(σ j) α j (X j ). We formalize a simple observation as a lemma because we use it later. Lemma 2. The coefficients ρ α,β in the ecomposition Λ α (X) = β α ρ α,β X β are polynomials in σ = (σ 1,..., σ n ), viewe as inepenent variables, an the multi-egree of ρ α,β (σ) is α β. Note that for an appropriate choice of the parameters σ j, 1 j n, the coefficients ρ α,β in the ecomposition Λ α (X) = β α ρ α,β X β are linearly inepenent over the rational fiel, an hence non-null. To prove this evaluate σ on an n-tuple of algebraically inepenent transcenental real numbers over the rational fiel.

8 8 HELTON, LASSERRE, AND PUTINAR 3.2. Proof of Theorem 1. Proof. Let L y be a linear functional for which M (y) 0 an let (p α ) enote the family of orthogonal polynomials with respect to L y. Orthogonality in (3.2) for expansions (3.4) reas δ αβ = p α, p β y = ρ αγ ρ βσ X γ, X σ y. In matrix notation this is just γ α, σ β I = D M (y) D T where D is the matrix D = (ρ αγ ) α, γ. Its columns are inexe (as before) by monomials arrange in GLex orer, an likewise for its rows. That ρ αγ = 0 if γ α, implies that ρ αγ = 0 if α < gl γ which says precisely that D is lower triangular. Moreover, its iagonal entries ρ ββ are not 0, since p β must have X β as its highest orer term. Because of this an triangularity, D is invertible. Write M (y) = D 1 (D T ) 1 an M (y) 1 = D T D. Our goal is to etermine which entries of M (y) 1 are force to be zero an we procee by writing the formula Z := M (y) 1 = D T D as z αβ = (3.5) ρ γα ρ γβ = ρ γα ρ γβ = γ max(α,β) γ, γ β γ, α γ, γ ρ γα ρ γβ We emphasize (since it arises later) that this uses only the full triangularity of the orthogonal polynomials rather than that they are proucts of one variable polynomials. If full triangularity were replace by triangularity w. r. to < gl, then the first two equalities in (3.5) woul be the same except that β γ, α γ, γ woul be replace by β gl γ, α gl γ, γ. To continue with our proof, consier (α, β) an set η := max(α, β). If max(α, β) >, then z α,β = 0, since the sum in equation (3.5) is empty. This is the forwar sie of Theorem 1. Conversely, when max(α, β) the entry z αβ is a sum of one or more proucts ρ γα ρ γβ an so is a polynomial in σ. If this polynomial is not ientically zero, then some value of σ makes z αβ 0, so (α, β) is not a congenital zero. Now we set out to show that z αβ as a polynomial in σ is not ientically 0. Lemma 2 tells us each prouct ρ γ,α ρ γ,β is a polynomial whose multiegree in σ is exactly 2γ α β. The multi-inex γ is subject to the constraints max(α, β) γ an γ. We fix an inex, say j = 1 an choose ˆγ = max(α, β) + ( max(α, β), 0,..., 0).

9 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 9 Note the prouct ρˆγα ρˆγβ is inclue in the sum (3.5) for z α,β an it is a polynomial of egree 2 2 max(α, β) + 2 max(α 1, β 1 ) α 1 β 1 with respect to σ 1. By the extremality of our construction of ˆγ, every other term ρ γα ρ γβ in z αβ will have smaller σ 1 egree. Hence ρˆγα ρˆγβ can not be cancelle, proving that z αβ is not the zero polynomial. 4. Partial inepenence In this section we consier the case where only a partial inepenence property hols. We ecompose the variables into isjoint sets X = (X(1),..., X(k)) where X(1) = (X(1) 1,..., X(1) 1 ), an so on. The linear functional L y is sai to satisfy a partial inepenence property (w.r. to the fixe grouping of variables), if L y (p 1 (X(1))...p k (X(k))) = k L y (p j (X(j)), where p j is a polynomial in the variables from the set X(j), respectively. Denote by eg X(j) Q(X) the egree of a polynomial Q in the variables X(j). Assuming that L y is a positive functional, one can associate in a unique way the orthogonal polynomials p α, α N n. Note that the lexicographic orer on N n respects the grouping of variables, in the sense j=1 (α 1,..., α k ) < gl (β 1,..., β k ) if an only if, either α 1 < gl β 1, or, if α 1 = β 1, then, either α 2 < gl β 2, an so on. Let α = (α 1,..., α k ) be a multi-inex ecompose with respect to the groupings X(1),..., X(k). Then, the uniqueness property of the orthonormal polynomials implies p α (X) = p α1 (X(1))...p αk (X(k)), where p αj (X(j)) are orthonormal polynomials epening solely on X(j), an arrange in lexicographic orer within this group of variables. Theorem 3. Let L y be a positive linear functional satisfying a partial inepenence property with respect to the groups of variables X = (X(1),..., X(k)). Let α = (α 1,..., α k ), β = (β 1,..., β k ) be two multi-inices ecompose accoring to the fixe groups of variables, an satisfying α, β. Then the (α, β)-entry in the matrix M (y) 1 is congenitally zero if an only if for every γ = (γ 1,..., γ k ) satisfying γ j gl α j, β j, 1 j k, we have γ >. The proof will repeat that of Theorem 1, with the only observation that p α (X) = γ. c α,γx 1 j k γ j gl α j

10 10 HELTON, LASSERRE, AND PUTINAR 5. Full triangularity A secon look at the proof of Theorem 1 reveals that the only property of the multivariate orthogonal polynomial we have use was the full triangularity form (3.4). In this section we provie an example of a nonprouct measure which has orthogonal polynomials in full triangular form, an, on the other han, we prove that the zero pattern appearing in our main result, in the inverse moment matrices M r (y) 1, r, implies the full triangular form of the associate orthogonal polynomials. Therefore, zeros in the inverse M 1 are coming from some triangularity property of orthogonal polynomials rather than from a prouct form of M. Example 1. We work in two real variables (x, y), with the measure µ = (1 x 2 y 2 ) t xy, restricte to the unit isk x 2 + y 2 < 1, where t > 1 is a parameter. Let P k (u; s) enote the orthonormalize Jacobi polynomials, that is the univariate orthogonal polynomials on the segment [ 1, 1], with respect to the measure (1 u 2 ) s u, with s > 1. Accoring to [6, Example 1, Chapter X], the orthonormal polynomials associate to the measure µ on the unit isk are: Q m+n,n (x, y) = P m (x, t + n + 1/2)(1 x 2 ) n/2 y P n ( ; t) 1 x 2 an Q n,m+n (x, y) = P m (y, t + n + 1/2)(1 y 2 ) n/2 x P n ( ; t). 1 y 2 Remark that these polynomials have full triangular form, yet the generating measure is not a prouct of measures. Theorem 4 (Full triangularity theorem). Let y = (y α ) α N n be a multisequence, such that the associate Hankel forms M (y) are positive efinite, where is a fixe positive integer. Then the following hols. For every r, the (α, β)-entry in M r (y) 1 is 0 whenever max(α, β) > r if an only if the associate orthogonal polynomials P α, α, have full triangular form. Proof. The proof of the forwar sie is exactly the same as in the proof of Theorem 1. The converse proof begins by expaning each orthogonal polynomial p α as (5.1) p α (X) := ρ αγ X γ, α γ gl α where we emphasize that γ gl α is use as oppose to (3.4) an we want to prove that β gl α an β α implies ρ αβ = 0. Note that when α = the inequality (5.2) β α is equivalent to max(α, β) >.

11 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 11 The first step is to use the zero locations of M (y) 1 to prove that (5.3) ρ αβ = 0 if max(α, β) >, only for α =. Once this is establishe, then we apply the same argument to prove (5.2) for α = where is smaller. If n = 1 there is nothing to prove. Assume n > 1 an ecompose N n as N N n 1. The corresponing inices will be enote by (i, α), i N, α N n 1. We shall prove (5.3) by escening inuction on the grae lexicographic orer applie to the inex (i, α) the following statement: Let i + α = an assume that (j, β) < gl (i, α) an (j, β) (i, α). Then ρ (i,α),(j,β) = 0. The precise statement we shall use is equivalent (because of (5.2)) to: The inuction hypothesis: Suppose that (5.4) ρ (i,α ),(j,β) = 0 if max(i, j) + max(α, β) >, hols for all inices (i, α ) > gl (i, α), with i + α = i + α =. We want to prove ρ (i,α),(j,β) = 0. Since we shall procee by inuction from the top, we assume that i + α = that (j, β) (i, α) that (j, β) < gl (i, α) an let (i, α) enote the largest such w. r. to < gl orer. Clearly, i =. There is only one corresponing term in the grae lexicographic sequence of inices of length less than or equal to, namely (, 0). We shall prove that for every β N n 1, (j, β) gl (, 0), β > 0, we have ρ (,0),(j,β) = 0. Since the corresponing entry in M (y) 1, enote henceforth as before by z : z (,0),(j,β) = 0, is zero by assumption, an because we obtain ρ (,0),(j,β) = 0. z (,0),(j,β) = ρ (,0),(,0) ρ (,0),(j,β) Now we turn to proving the main inuction step. Assuming (5.4), we want to prove ρ (i,α),(j,β) = 0. Let (j, β) gl (i, α) subject to the conition max(i, j) + max(α, β) >. Then by hypothesis 0 = z (i,α),(j,β), so the GLex version of expansion (3.5) gives 0 = ρ (i,α),(i,α) ρ (i,α),(j,β) + + i >i, i + α = i =i, α > gl α, i + α = ρ (i,α ),(i,α)ρ (i,α ),(j,β). ρ (i,α ),(i,α)ρ (i,α ),(j,β)

12 12 HELTON, LASSERRE, AND PUTINAR We will prove that the two summations above are zero. Inee, if i > i, then max(i, i ) + max(α, α) > i + α =, an the inuction hypothesis implies ρ (i,α ),(i,α) = 0. Which eliminates the secon sum. Assume i = i, so that α = α. Then if max(α, α ) equals to either α or α, we get α = α, but this can not be, since α > gl α. Thus i+ max(α, α ) > an the inuction hypothesis yiels in this case ρ (i,α ),(i,α) = 0. Which eliminates the first sum. In conclusion ρ (i,α),(i,α) ρ (i,α),(j,β) = 0, which implies ρ (i,α),(j,β) = 0, as esire. Our inuction hypothesis is vali an we initialize it successfully, so we obtain the working hypothesis: ρ (i,α),(j,β) = 0, whenever (j, β) < gl (i, α), (i, α) =, an max( (j, β), (i, α) ) >. By (5.2) this is full triangularity uner the assumption i + α =. In contrast to the above full triangularity criteria, the prouct ecomposition of a potential truncate moment sequence (y α ) αi can be ecie by elementary linear algebra. Assume for simplicity that n = 2, an write the corresponing inices as α = (i, j) N 2. Then there are numerical sequences (u i ) i an (v j ) j with the property if an only if y (i,j) = u i v j, 0 i, j, rank(y (i,j) ) i,j=0 1. A similar rank conition, for a corresponing multilinear map, can be euce for arbitrary n. 6. Conitional Triangularity The aim of this section is to exten the full triangularity theorem of 5, in a more general context Conitional triangularity. In this new setting we consier two tuples of variables X = (x 1,..., x n ), Y = (y 1,..., y m ), an we will impose on the concatenate tuple (X, Y ) the full triangularity only with respect to the set of variables Y. The conclusion is as expecte: this assumption will reflect the appearance of some zeros in the inverse M 1 of the associate truncate moment matrix. The proof below is quite similar

13 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 13 to that of Theorem 4 an we inicate only sufficiently many etails to make clear the ifferences. We enote the set of inices by (α, β), with α N n, β N m, equippe with the grae lexicographic orer < gl. In aition, the set of inices β N m which refers to the set of variables Y, is also equippe with the full grae orer. Let y = (y α ) α N n be a multi-sequence, such that the associate Hankel forms M (y) are positive efinite, where is a positive integer. As before we enote: p (α,β) (X, Y ) = ρ (α,β),(α,β )X α Y β (α,β) gl (α,β ) the associate orthogonal polynomials, an by z (α,β),(α,β ) = ρ (γ,σ),(α,β) ρ (γ,σ),(α,β ) the entries in M (y) 1. (γ,σ) gl (α,β),(α,β ) Definition 2. (Conitional triangularity) The orthonormal polynomials p α,β R[X, Y ], with α + β 2, satisfy the conitional triangularity with respect to X, if when X is fixe an consiere as a parameter, the resulting family enote {p α,β X} R[Y ] is in full triangular form with respect to the Y variables. More precisely, the following (O) conition below hols. (O) : [ (α, β ) gl (α, β), (α, β), an β β ] ρ (α,β),(α,β ) = 0 Next, for a fixe egree 1 we will have to consier the following zero in the inverse conition Definition 3. (zero in the inverse conition (V ) ) Let (α, β ) gl (α, β) with (α, β), be fixe, arbitrary. If (γ, σ) > whenever (γ, σ) gl (α, β), (α, β ) an σ max(β, β )), then z (α,β),(α,β ) = 0. The main result of this paper asserts that both conitions (V ) an (O) are in fact equivalent. Theorem 5 (Conitional triangularity). Let y = (y α ) α N n be a multisequence an let be an integer such that the associate Hankel form M (y) is positive efinite. Then the zero in the inverse conition (V ) r, r, hols if an only if (O) hols, i.e., if an only if the orthonormal polynomials satisfy the conitional triangularity with respect to X. Proof. Clearly, from its efinition, (O) implies (O) r for all r. One irection is obvious: Let r be fixe, arbitrary. If conition (O) r hols, then a pair ((α, β ) gl (α, β)) subject to the assumptions in (V ) r will leave not a single term in the sum giving z (α,β),(α,β ).

14 14 HELTON, LASSERRE, AND PUTINAR Conversely, assume that (V ) hols. We will prove the vanishing statement (O) by escening inuction with respect to the grae lexicographical orer. To this aim, we label all inices (α, β), (α, β) = in ecreasing grae lexicographic orer: (α 0, β 0 ) > gl (α 1, β 1 ) > gl (α 2, β 2 ).... In particular = α 0 α 1... an 0 = β 0 β 1... To initialize the inuction, consier (α, β ) gl (α 0, β 0 ) = (α 0, 0), with β 0, that is β 0. Then 0 = z (α0,β 0 ),(α,β ) = ρ (α0,β 0 ),(α 0,β 0 )ρ (α0,β 0 ),(α,β ). Since the leaing coefficient ρ (α0,β 0 ),(α 0,β 0 ) in the orthogonal polynomial is non-zero, we infer [(α, β ) < gl (α 0, β 0 ), β β 0 ] ρ (α0,β 0 ),(α,β ) = 0, which is exactly conition (O) applie to this particular choice of inices. Assume that (O) hols for all (α j, β j ), j < k. Let (α, β ) < gl (α k, β k ) with β β k, that is, max(β, β k ) > β k. In view of (V ), k 1 z (αk,β k ),(α,β ) = ρ (αk,β k ),(α k,β k )ρ (αk,β k ),(α,β ) + ρ (αj,β j ),(α k,β k )ρ (αj,β j ),(α,β ). Note that the inuction hypothesis implies that for every 0 j k 1, at least one factor ρ (αj,β j ),(α k,β k ) or ρ (αj,β j ),(α,β ) vanishes. Thus, j=0 0 = z (αk,β k ),(α,β ) = ρ (αk,β k ),(α k,β k )ρ (αk,β k ),(α,β ), whence ρ (αk,β k ),(α,β ) = 0. Once we have exhauste by the above inuction all inices of length, we procee similarly to those of length 1, using now the zero in the inverse property (V ) 1, an so on. Remark that the orering (X, Y ) with the tuple of full triangular variables Y on the secon entry is important. A low egree example will be consiere in the last section. We call Theorem 5 the conitional triangularity theorem because when the variables X are fixe (an so can be consiere as parameters), then the orthogonal polynomials now consiere as elements of R[Y ], are in full triangular form, rephrase as in triangular form conitional to X is fixe The link with partial correlation. Let us specialize to the case = 1. Assume that the unerlying joint istribution on the ranom vector X = (X 1,..., X n ) is centere, that is, X i µ = 0 for all i = 1,..., n; then M reas M = 1 0 an M 1 = R 0 R 1

15 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 15 where R is just the so-calle covariance matrix. Partitionning the ranom vector in (Y, X i, X j ) with Y = (X k ) k i,j, yiels R = var (Y ) cov (Y, X i) cov (Y, X j ) cov (Y, X i ) var (X i ) cov (X i, X j ), cov (Y, X j ) cov (X i, X j ) var (X j ) where var an cov have obvious meanings. The partial covariance of X i an X j given Y, enote cov (X i, X j Y ) in Wittaker [7, p. 135], satisfies: (6.1) cov (X i, X j Y ) := cov (X i, X j ) cov (Y, X i )var (Y ) 1 cov (Y, X j ). After scaling R 1 to have a unit iagonal, the partial correlation between X i an X j (partialle on Y ) is the negative of cov (X i, X j Y ), an as alreay mentione, R 1 (i, j) = 0 if an only if X i an X j have zero partial correlation, i.e., cov (X i, X j Y ) = 0. See e.g. Wittaker [7, Cor an 5.8.4]. Corollary 6. Let = 1. Then R 1 (i, j) = 0 if an only if the orthonormal polynomials of egree up to 2, associate with M 1, satisfy the conitional triangularity with respect to X = (X k ) k i,j. Proof. To recast the problem in the framework of 6.1, let Y = (X i, X j ) an rename X := (X k ) k i,j. In view of Definition 3 with = 1, we only nee consier pairs (α, β ) gl (α, β) with α = α = 0 an β = (0, 1), β = (1, 0). But then σ max[β, β ] = (1, 1) implies (γ, σ) 2 >, an so as R 1 (i, j) = 0, the zero in the inverse conition (V ) hols. Equivalently, by Theorem 5, (O) hols. Corollary 6 states that the pair (X i, X j ) has zero partial correlation if an only if the orthonormal polynomials up to egree 2, satisfy the conitional triangularity with respect to X = (X k ) k i,j. That is, partial correlation an conitional triangularity are equivalent. Example 2. Let = 1, an consier the case of three ranom variables (X, Y, Z) with (centere) joint istribution µ. Then suppose that the orthonormal polynomials up to egree = 1 satisfy the conitional triangularity property (V ) 1 w.r.t. X. That is, p 000 = 1 an p 100 = α 1 + β 1 X; p 010 = α 2 + β 2 X + γ 2 Y ; p 001 = α 3 + β 3 X + γ 3 Z, for some coefficients (α i β i γ i ). Notice that because of (O) 1, we cannot have a linear term in Y in p 001. Orthogonality yiels that X γ, p α = 0 for all γ < gl α, i.e., with E being the expectation w.r.t. µ, β 2 E(X 2 ) + γ 2 E(XY ) = 0 β 3 E(X 2 ) + γ 3 E(XZ) = 0 β 3 E(XY ) + γ 3 E(Y Z) = 0. Stating that the eterminant of the last two linear equations in (β 3, γ 3 ) is zero yiels E(Y Z) E(X, Y )E(X 2 ) 1 E(X, Z) = 0,

16 16 HELTON, LASSERRE, AND PUTINAR which is just (6.1), i.e., the zero partial correlation conition, up to a multiplicative constant. This immeiately raises two questions: (i) What are the istributions for which the orthonormal polynomials up to egree 2 satisfy the conitional triangularity with respect to a given pair (X i, X j )? (ii) Among such istributions, what are those for which conitional inepenence with respect to X = (X k i,j ) also hols? An answer to the latter woul characterize istributions for which zero partial correlation imply conitional inepenence (like for the normal istribution) Conitional inepenence an zeros in the inverse. We have alreay mentione that in general, conitional inepenence is not etecte from zero entries in the inverse of R 1 (equivalently, M1 1 ), except for the normal joint istribution, a common assumption in Graphical Gaussian Moels. Therefore, a natural question of potential interest is to search for conitions on when conitional inepenence in the non gaussian case is relate to the zero in the inverse property (V ), or equivalently, the conitional triangularity (O), not only for = 1 but also for > 1. A rather negative result in this irection is as follows. Let be fixe, arbitrary, an let M = (y ijk ) 0 be the moment matrix of an arbitrary joint istribution µ of three ranom variables (X, Y 1, Y 2 ) on R. As we are consiering only finitely many moments (up to orer 2), by Tchakaloff s theorem there exists a measure ϕ finitely supporte on, say s, points (x (l), y (l) 1, y(l) 2 ) R 3 (with associate probabilities {p l }), l = 1,..., s, an whose all moments up to orer 2 match those of µ; see e.g. Reznick [5, Theor. 7.18]. Let us efine a sequence {ϕ t } of probability measures as follows. Perturbate each point (x (l), y (l) 1, y(l) 2 ) to (x(l) + ɛ(t, l), y (l) 1, y(l) 2 ), l = 1,..., s, in such a way that no two points x (l) + ɛ(t, l) are the same, an keep the same weights {p l }. It is clear that ϕ t satisfies: 1 = Prob[Y = (y (l) 1, y(l) 2 ) X = x(l) + ɛ(t, l)] = Prob[Y 1 = y (l) 1 X = x(l) + ɛ(t, l)] Prob[Y 2 = y (l) 2 X = x(l) + ɛ(t, l)] for all l = 1,..., s. That is, conitional to X, the variables Y 1 an Y 2 are inepenent. Take a sequence with ɛ(t, l) 0 for all l, as t, an consier the moment matrix M (t) associate with ϕ t. Clearly, as t, X i Y j 1 Y k 2 ϕ t X i Y j 1 Y k 2 µ = y ijk, i, j, k : i + j + k 2, i.e., M (t) M. Therefore, if the zero in the inverse property (V ) oes not hol for M, then by a simple continuity argument, it cannot hol for any M (t) with

17 MEASURES WITH ZEROS IN THE INVERSE OF THEIR MOMENT MATRIX 17 sufficiently large t, an still the conitional inepenence property hols for each ϕ t. One has just shown that for every fixe, one may easily construct examples of measures with the conitional inepenence property, which violate the zero in the inverse property (V ). References [1] C.F. Dunkl, Yuan Xu. Orthogonal Polynomials of Several Variables, Cambrige University Press, Cambrige, [2] C. Berg. Fibonacci numbers an orthogonal polynomials. Preprint. [3] E. Cripps, C. Carter, R. Kohn. Variable selection an covariance selection in multiregression moels. Technical report # , Statistical an Applie Mathematical Sciences Institute, Research Triangle Park, NC, [4] W. Magnus, F. Oberhettinger, Formulas an Theorems for the Functions of Mathematical Physics, Chelsea reprint, New York, [5] B. Reznick. Sums o Even Powers of real Linear Forms, Amer. Math. Soc. Memoirs vol. 96, Amer. Math. Soc. Provience, R.I., [6] P. K. Suetin, Orthogonal polynomials in two variables (in Russian), Nauka, Moscow, [7] J. Wittaker. Graphical Moels in Applie Mathematical Analysis, Wiley, New York, 1990.

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

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

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS MARK SCHACHNER Abstract. When consiere as an algebraic space, the set of arithmetic functions equippe with the operations of pointwise aition an

More information

SYMMETRIC KRONECKER PRODUCTS AND SEMICLASSICAL WAVE PACKETS

SYMMETRIC KRONECKER PRODUCTS AND SEMICLASSICAL WAVE PACKETS SYMMETRIC KRONECKER PRODUCTS AND SEMICLASSICAL WAVE PACKETS GEORGE A HAGEDORN AND CAROLINE LASSER Abstract We investigate the iterate Kronecker prouct of a square matrix with itself an prove an invariance

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

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations Diophantine Approximations: Examining the Farey Process an its Metho on Proucing Best Approximations Kelly Bowen Introuction When a person hears the phrase irrational number, one oes not think of anything

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

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

Robustness and Perturbations of Minimal Bases

Robustness and Perturbations of Minimal Bases Robustness an Perturbations of Minimal Bases Paul Van Dooren an Froilán M Dopico December 9, 2016 Abstract Polynomial minimal bases of rational vector subspaces are a classical concept that plays an important

More information

Conservation Laws. Chapter Conservation of Energy

Conservation Laws. Chapter Conservation of Energy 20 Chapter 3 Conservation Laws In orer to check the physical consistency of the above set of equations governing Maxwell-Lorentz electroynamics [(2.10) an (2.12) or (1.65) an (1.68)], we examine the action

More information

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

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

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

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

DECOMPOSITION OF POLYNOMIALS AND APPROXIMATE ROOTS

DECOMPOSITION OF POLYNOMIALS AND APPROXIMATE ROOTS DECOMPOSITION OF POLYNOMIALS AND APPROXIMATE ROOTS ARNAUD BODIN Abstract. We state a kin of Eucliian ivision theorem: given a polynomial P (x) an a ivisor of the egree of P, there exist polynomials h(x),

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

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

Characterizing Real-Valued Multivariate Complex Polynomials and Their Symmetric Tensor Representations

Characterizing Real-Valued Multivariate Complex Polynomials and Their Symmetric Tensor Representations Characterizing Real-Value Multivariate Complex Polynomials an Their Symmetric Tensor Representations Bo JIANG Zhening LI Shuzhong ZHANG December 31, 2014 Abstract In this paper we stuy multivariate polynomial

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

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

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

TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH

TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH English NUMERICAL MATHEMATICS Vol14, No1 Series A Journal of Chinese Universities Feb 2005 TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH He Ming( Λ) Michael K Ng(Ξ ) Abstract We

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

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7. Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency

More information

On the enumeration of partitions with summands in arithmetic progression

On the enumeration of partitions with summands in arithmetic progression AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 8 (003), Pages 149 159 On the enumeration of partitions with summans in arithmetic progression M. A. Nyblom C. Evans Department of Mathematics an Statistics

More information

Witt#5: Around the integrality criterion 9.93 [version 1.1 (21 April 2013), not completed, not proofread]

Witt#5: Around the integrality criterion 9.93 [version 1.1 (21 April 2013), not completed, not proofread] Witt vectors. Part 1 Michiel Hazewinkel Sienotes by Darij Grinberg Witt#5: Aroun the integrality criterion 9.93 [version 1.1 21 April 2013, not complete, not proofrea In [1, section 9.93, Hazewinkel states

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

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

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

Make graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides

Make graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides Reference 1: Transformations of Graphs an En Behavior of Polynomial Graphs Transformations of graphs aitive constant constant on the outsie g(x) = + c Make graph of g by aing c to the y-values on the graph

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

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

Permanent vs. Determinant

Permanent vs. Determinant Permanent vs. Determinant Frank Ban Introuction A major problem in theoretical computer science is the Permanent vs. Determinant problem. It asks: given an n by n matrix of ineterminates A = (a i,j ) an

More information

LeChatelier Dynamics

LeChatelier Dynamics LeChatelier Dynamics Robert Gilmore Physics Department, Drexel University, Philaelphia, Pennsylvania 1914, USA (Date: June 12, 28, Levine Birthay Party: To be submitte.) Dynamics of the relaxation of a

More information

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1 Assignment 1 Golstein 1.4 The equations of motion for the rolling isk are special cases of general linear ifferential equations of constraint of the form g i (x 1,..., x n x i = 0. i=1 A constraint conition

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

Equilibrium in Queues Under Unknown Service Times and Service Value

Equilibrium in Queues Under Unknown Service Times and Service Value University of Pennsylvania ScholarlyCommons Finance Papers Wharton Faculty Research 1-2014 Equilibrium in Queues Uner Unknown Service Times an Service Value Laurens Debo Senthil K. Veeraraghavan University

More information

RODRIGUES TYPE FORMULA FOR ORTHOGONAL POLYNOMIALS ON THE UNIT BALL

RODRIGUES TYPE FORMULA FOR ORTHOGONAL POLYNOMIALS ON THE UNIT BALL RODRIGUES TYPE FORMULA FOR ORTHOGONAL POLYNOMIALS ON THE UNIT BALL YUAN XU Abstract. For a class of weight function invariant uner reflection groups on the unit ball, a family of orthogonal polynomials

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

Unit vectors with non-negative inner products

Unit vectors with non-negative inner products Unit vectors with non-negative inner proucts Bos, A.; Seiel, J.J. Publishe: 01/01/1980 Document Version Publisher s PDF, also known as Version of Recor (inclues final page, issue an volume numbers) Please

More information

All s Well That Ends Well: Supplementary Proofs

All s Well That Ends Well: Supplementary Proofs All s Well That Ens Well: Guarantee Resolution of Simultaneous Rigi Boy Impact 1:1 All s Well That Ens Well: Supplementary Proofs This ocument complements the paper All s Well That Ens Well: Guarantee

More information

Some vector algebra and the generalized chain rule Ross Bannister Data Assimilation Research Centre, University of Reading, UK Last updated 10/06/10

Some vector algebra and the generalized chain rule Ross Bannister Data Assimilation Research Centre, University of Reading, UK Last updated 10/06/10 Some vector algebra an the generalize chain rule Ross Bannister Data Assimilation Research Centre University of Reaing UK Last upate 10/06/10 1. Introuction an notation As we shall see in these notes the

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

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

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

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

Capacity Analysis of MIMO Systems with Unknown Channel State Information

Capacity Analysis of MIMO Systems with Unknown Channel State Information Capacity Analysis of MIMO Systems with Unknown Channel State Information Jun Zheng an Bhaskar D. Rao Dept. of Electrical an Computer Engineering University of California at San Diego e-mail: juzheng@ucs.eu,

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

Hyperbolic Moment Equations Using Quadrature-Based Projection Methods

Hyperbolic Moment Equations Using Quadrature-Based Projection Methods Hyperbolic Moment Equations Using Quarature-Base Projection Methos J. Koellermeier an M. Torrilhon Department of Mathematics, RWTH Aachen University, Aachen, Germany Abstract. Kinetic equations like the

More information

2Algebraic ONLINE PAGE PROOFS. foundations

2Algebraic ONLINE PAGE PROOFS. foundations Algebraic founations. Kick off with CAS. Algebraic skills.3 Pascal s triangle an binomial expansions.4 The binomial theorem.5 Sets of real numbers.6 Surs.7 Review . Kick off with CAS Playing lotto Using

More information

On colour-blind distinguishing colour pallets in regular graphs

On colour-blind distinguishing colour pallets in regular graphs J Comb Optim (2014 28:348 357 DOI 10.1007/s10878-012-9556-x On colour-blin istinguishing colour pallets in regular graphs Jakub Przybyło Publishe online: 25 October 2012 The Author(s 2012. This article

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

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

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

Some properties of random staircase tableaux

Some properties of random staircase tableaux Some properties of ranom staircase tableaux Sanrine Dasse Hartaut Pawe l Hitczenko Downloae /4/7 to 744940 Reistribution subject to SIAM license or copyright; see http://wwwsiamorg/journals/ojsaphp Abstract

More information

Regular tree languages definable in FO and in FO mod

Regular tree languages definable in FO and in FO mod Regular tree languages efinable in FO an in FO mo Michael Beneikt Luc Segoufin Abstract We consier regular languages of labele trees. We give an effective characterization of the regular languages over

More information

A simple model for the small-strain behaviour of soils

A simple model for the small-strain behaviour of soils A simple moel for the small-strain behaviour of soils José Jorge Naer Department of Structural an Geotechnical ngineering, Polytechnic School, University of São Paulo 05508-900, São Paulo, Brazil, e-mail:

More information

Lecture 2: Correlated Topic Model

Lecture 2: Correlated Topic Model Probabilistic Moels for Unsupervise Learning Spring 203 Lecture 2: Correlate Topic Moel Inference for Correlate Topic Moel Yuan Yuan First of all, let us make some claims about the parameters an variables

More information

Jointly continuous distributions and the multivariate Normal

Jointly continuous distributions and the multivariate Normal Jointly continuous istributions an the multivariate Normal Márton alázs an álint Tóth October 3, 04 This little write-up is part of important founations of probability that were left out of the unit Probability

More information

Generalized Tractability for Multivariate Problems

Generalized Tractability for Multivariate Problems Generalize Tractability for Multivariate Problems Part II: Linear Tensor Prouct Problems, Linear Information, an Unrestricte Tractability Michael Gnewuch Department of Computer Science, University of Kiel,

More information

Pseudo-Free Families of Finite Computational Elementary Abelian p-groups

Pseudo-Free Families of Finite Computational Elementary Abelian p-groups Pseuo-Free Families of Finite Computational Elementary Abelian p-groups Mikhail Anokhin Information Security Institute, Lomonosov University, Moscow, Russia anokhin@mccme.ru Abstract We initiate the stuy

More information

Logarithmic spurious regressions

Logarithmic spurious regressions Logarithmic spurious regressions Robert M. e Jong Michigan State University February 5, 22 Abstract Spurious regressions, i.e. regressions in which an integrate process is regresse on another integrate

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

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

Linear Algebra- Review And Beyond. Lecture 3

Linear Algebra- Review And Beyond. Lecture 3 Linear Algebra- Review An Beyon Lecture 3 This lecture gives a wie range of materials relate to matrix. Matrix is the core of linear algebra, an it s useful in many other fiels. 1 Matrix Matrix is the

More information

Symbolic integration with respect to the Haar measure on the unitary groups

Symbolic integration with respect to the Haar measure on the unitary groups BULLETIN OF THE POLISH ACADEMY OF SCIENCES TECHNICAL SCIENCES, Vol. 65, No., 207 DOI: 0.55/bpasts-207-0003 Symbolic integration with respect to the Haar measure on the unitary groups Z. PUCHAŁA* an J.A.

More information

Proof of SPNs as Mixture of Trees

Proof of SPNs as Mixture of Trees A Proof of SPNs as Mixture of Trees Theorem 1. If T is an inuce SPN from a complete an ecomposable SPN S, then T is a tree that is complete an ecomposable. Proof. Argue by contraiction that T is not a

More information

A Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential

A Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential Avances in Applie Mathematics an Mechanics Av. Appl. Math. Mech. Vol. 1 No. 4 pp. 573-580 DOI: 10.4208/aamm.09-m0946 August 2009 A Note on Exact Solutions to Linear Differential Equations by the Matrix

More information

arxiv: v2 [math.pr] 27 Nov 2018

arxiv: v2 [math.pr] 27 Nov 2018 Range an spee of rotor wals on trees arxiv:15.57v [math.pr] 7 Nov 1 Wilfrie Huss an Ecaterina Sava-Huss November, 1 Abstract We prove a law of large numbers for the range of rotor wals with ranom initial

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 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

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

ON THE DISTANCE BETWEEN SMOOTH NUMBERS

ON THE DISTANCE BETWEEN SMOOTH NUMBERS #A25 INTEGERS (20) ON THE DISTANCE BETWEEN SMOOTH NUMBERS Jean-Marie De Koninc Département e mathématiques et e statistique, Université Laval, Québec, Québec, Canaa jm@mat.ulaval.ca Nicolas Doyon Département

More information

A variance decomposition and a Central Limit Theorem for empirical losses associated with resampling designs

A variance decomposition and a Central Limit Theorem for empirical losses associated with resampling designs Mathias Fuchs, Norbert Krautenbacher A variance ecomposition an a Central Limit Theorem for empirical losses associate with resampling esigns Technical Report Number 173, 2014 Department of Statistics

More information

Analyzing Tensor Power Method Dynamics in Overcomplete Regime

Analyzing Tensor Power Method Dynamics in Overcomplete Regime Journal of Machine Learning Research 18 (2017) 1-40 Submitte 9/15; Revise 11/16; Publishe 4/17 Analyzing Tensor Power Metho Dynamics in Overcomplete Regime Animashree Ananumar Department of Electrical

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

REVERSIBILITY FOR DIFFUSIONS VIA QUASI-INVARIANCE. 1. Introduction We look at the problem of reversibility for operators of the form

REVERSIBILITY FOR DIFFUSIONS VIA QUASI-INVARIANCE. 1. Introduction We look at the problem of reversibility for operators of the form REVERSIBILITY FOR DIFFUSIONS VIA QUASI-INVARIANCE OMAR RIVASPLATA, JAN RYCHTÁŘ, AND BYRON SCHMULAND Abstract. Why is the rift coefficient b associate with a reversible iffusion on R given by a graient?

More information

0.1 Differentiation Rules

0.1 Differentiation Rules 0.1 Differentiation Rules From our previous work we ve seen tat it can be quite a task to calculate te erivative of an arbitrary function. Just working wit a secon-orer polynomial tings get pretty complicate

More information

Binary Discrimination Methods for High Dimensional Data with a. Geometric Representation

Binary Discrimination Methods for High Dimensional Data with a. Geometric Representation Binary Discrimination Methos for High Dimensional Data with a Geometric Representation Ay Bolivar-Cime, Luis Miguel Corova-Roriguez Universia Juárez Autónoma e Tabasco, División Acaémica e Ciencias Básicas

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

THE GENUINE OMEGA-REGULAR UNITARY DUAL OF THE METAPLECTIC GROUP

THE GENUINE OMEGA-REGULAR UNITARY DUAL OF THE METAPLECTIC GROUP THE GENUINE OMEGA-REGULAR UNITARY DUAL OF THE METAPLECTIC GROUP ALESSANDRA PANTANO, ANNEGRET PAUL, AND SUSANA A. SALAMANCA-RIBA Abstract. We classify all genuine unitary representations of the metaplectic

More information

Applications of the Wronskian to ordinary linear differential equations

Applications of the Wronskian to ordinary linear differential equations Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.

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

Year 11 Matrices Semester 2. Yuk

Year 11 Matrices Semester 2. Yuk Year 11 Matrices Semester 2 Chapter 5A input/output Yuk 1 Chapter 5B Gaussian Elimination an Systems of Linear Equations This is an extension of solving simultaneous equations. What oes a System of Linear

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

3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes

3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes Fin these erivatives of these functions: y.7 Implicit Differentiation -- A Brief Introuction -- Stuent Notes tan y sin tan = sin y e = e = Write the inverses of these functions: y tan y sin How woul we

More information

The Non-abelian Hodge Correspondence for Non-Compact Curves

The Non-abelian Hodge Correspondence for Non-Compact Curves 1 Section 1 Setup The Non-abelian Hoge Corresponence for Non-Compact Curves Chris Elliott May 8, 2011 1 Setup In this talk I will escribe the non-abelian Hoge theory of a non-compact curve. This was worke

More information

arxiv: v1 [math-ph] 5 May 2014

arxiv: v1 [math-ph] 5 May 2014 DIFFERENTIAL-ALGEBRAIC SOLUTIONS OF THE HEAT EQUATION VICTOR M. BUCHSTABER, ELENA YU. NETAY arxiv:1405.0926v1 [math-ph] 5 May 2014 Abstract. In this work we introuce the notion of ifferential-algebraic

More information

Relative Entropy and Score Function: New Information Estimation Relationships through Arbitrary Additive Perturbation

Relative Entropy and Score Function: New Information Estimation Relationships through Arbitrary Additive Perturbation Relative Entropy an Score Function: New Information Estimation Relationships through Arbitrary Aitive Perturbation Dongning Guo Department of Electrical Engineering & Computer Science Northwestern University

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

Systems & Control Letters

Systems & Control Letters Systems & ontrol Letters ( ) ontents lists available at ScienceDirect Systems & ontrol Letters journal homepage: www.elsevier.com/locate/sysconle A converse to the eterministic separation principle Jochen

More information

ON BEAUVILLE STRUCTURES FOR PSL(2, q)

ON BEAUVILLE STRUCTURES FOR PSL(2, q) ON BEAUVILLE STRUCTURES FOR PSL(, q) SHELLY GARION Abstract. We characterize Beauville surfaces of unmixe type with group either PSL(, p e ) or PGL(, p e ), thus extening previous results of Bauer, Catanese

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

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

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

Interconnected Systems of Fliess Operators

Interconnected Systems of Fliess Operators Interconnecte Systems of Fliess Operators W. Steven Gray Yaqin Li Department of Electrical an Computer Engineering Ol Dominion University Norfolk, Virginia 23529 USA Abstract Given two analytic nonlinear

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

arxiv:math/ v1 [math.pr] 19 Apr 2001

arxiv:math/ v1 [math.pr] 19 Apr 2001 Conitional Expectation as Quantile Derivative arxiv:math/00490v math.pr 9 Apr 200 Dirk Tasche November 3, 2000 Abstract For a linear combination u j X j of ranom variables, we are intereste in the partial

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