COHOMOLOGY OF PROJECTIVE SYSTEMS ON RANKED POSETS. Introduction

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "COHOMOLOGY OF PROJECTIVE SYSTEMS ON RANKED POSETS. Introduction"

Transcript

1 COHOMOLOGY OF PROJECTIVE SYSTEMS ON RANKED POSETS ARNE B. SLETSJØE Abstract. We consider different cohomology theories for a ranked poset with a local orientation. Under certain condidtions on the poset we show that the cohomology theories coincide. Introduction In spline theory we consider piecewise polynomial functions on some space, which possesses a certain degree of smoothness in the subspaces where the polynomial pieces connect. The general framwork for this set-up is a partial ordered set Λ and a projective system F of abelian groups on Λ. The partial ordered set gives the combinatorial structure of a grid or a triangulation of the underlying space. The projective system is a system of polynomial functions of bounded degree, where smoothness is encoded algebraically in the restriction of the system to the connection subspaces. The problem of determine the space of piecewise polynomial functions with the given degree of smoothness, in particular the dimension of the space, has been discussed by several authors, by various methods. See e.g. [2], [3], [4], [5], [7], [8] and [9]. The idea of using cellular (co-)homology theory to determine the dimension of the space of picewise polynomial functions is not new, it was already introduced by Billera ([?, B2] in the late 80ś. Our approach to the problem is to use a general theory of limits of projective systems on partial ordered sets. This theory was thoroughly explored in an early paper by Laudal [6]. In his treatise he considers mainly constant projective systems. For our purpose more general projective systems is required. The partial ordered structures of grids or triangulations have an additional structure given by a rank function, corresponding to the geometrical dimension of the actual facet. Under certain conditions on the ranked partial ordered set, including the existence of a local orientation, we show that cellular (co-)homology of these abstract cell complexes coincide with the theory of inverse limits of projective systems developed in [6]. The correspondance between the cellular (co-)homology theory and the invers limit approach was also treated by Basak in [1], but limited to constant projective systems. The advantage of our approach is that the general theory of invers limits of projective systems provides us with usefull tools to attack more applied problems in e.g. spline theory. We will discuss the applied aspect in a forthcoming paper. 1. Ranked posets A ranked poset Λ is a finite, connected poset, equipped with a strict order-preserving dimension function d : Λ N 0. The maximum value d Λ of the dimension function is called the geometric dimension of the poset, and the minimum value is called the minimal rank of Λ, denoted m Λ. We say that Λ is of pure dimension if all maximal elements of Λ have the same dimension, and of pure minimal rank if all minimal elements have the same dimension. An element λ Λ of dimension q = d(λ) is called a q-cell of Λ, and the set Λ q Λ of all q-cells is the q-skeleton of Λ. If λ 1 < λ 2 we say that λ 1 is a facet of λ 2 of codimension d(λ 2 ) d(λ 1 ). A facet λ 1 < λ 2 of codimension 1 is called a face of λ 2. For any cell λ in Λ, λ denotes the set of faces of λ and for any subset S Λ, S = {τ σ for some σ S}. If λ 1 is a face of λ 2, 1

2 2 ARNE B. SLETSJØE then the pair λ 1 < λ 2 is called a cover in Λ, and the set of all covers in Λ is denoted Cov(Λ). The set of facets of codimension k is denoted k λ. Dually, a cell that have λ as one of its faces is called a co-face of λ. The set of cofaces is denoted λ. Definition 1.1. An abstract cell complex is a ranked poset satisfying the following condition: For any λ 1 2 λ 2, λ 2 λ 1 = {τ 1, τ 2 }, i.e. there exists exactly two elements in λ 2, τ 1 and τ 2, such that λ 1 < τ i < λ 2, i = 1, 2. An abstract cell complex does in general not have a geometrical realization. Consequently there is no natural orientation of the cell complex. In order to define (co-)homology on an abstract cell complex we need to impose a local orientation on Λ. Definition 1.2. A local orientation of an abstract cell complex Λ is a map ɛ : Cov(Λ) {±1} such that for λ 1 2 λ 2, with λ 2 λ 1 = {τ 1, τ 2 } we have where we use the notation ɛ λ<τ = ɛ(λ < τ). ɛ λ1<τ 1 ɛ τ1<λ 2 + ɛ λ1<τ 2 ɛ τ2<λ 2 = 0 Two local orientations ɛ, ɛ are equivalent if there exists a map µ : Λ {±1} such that ɛ λ<τ = µ(τ)µ(λ) 1 ɛ λ<τ. In general, the existence of a local orientation is a rather strict condition on the ranked poset. Notice also that if d(λ 2 ) = d(λ 1 ) + 2, there may not exist any λ 1 < τ < λ 2. In that case the condition of Definition 1.2 is vacuous. An abstract cell complex Λ of pure dimension n is called non-singular if each (n 1)-cell of Λ is a face of at most two maximal cells and dually, each 1-cell of Λ has at most two vertices. A local orientation of an non-singular abstract cell complex is an orientation of Λ if for any (n 1)-cell τ with τ = {σ 1, σ 2 }, ɛ τ<σ1 = ɛ τ<σ2, and for each 1-cell τ with τ = {γ 1, γ 2 }, ɛ γ1<τ = ɛ γ2<τ. The abstract cell complex is orientable if there exist an orientation. The dual poset Λ of a poset Λ has the same objects as Λ, but with reversed ordering. We use the notation λ Λ for the corresponding object of λ Λ in Λ. The dual S of a subset S Λ is the set S = {λ λ S} of dual elements. If Λ is ranked, there is also a natural ranking of Λ ; the dimension of the dual element λ is the codimension of λ, i.e. d(λ ) = d Λ d(λ), where d Λ is the geometric dimension of Λ. Thus the q-skeleton of Λ corresponds to the (d Λ q)-skeleton of Λ. Notice that for λ Λ p λ = {σ (Λ ) d p 1 λ < σ } = {σ Λ p 1 σ < λ} = ( λ) The dual complex Λ has geometrical dimension d Λ = d Λ m Λ and minimal rank m Λ = 0. There is an isomorphism Λ Λ, given by a dimension shift m Λ, with equality Λ = Λ if and only if Λ has minimal rank m Λ = 0. The order dimension r(λ) of a finite poset Λ is the maximum length of ordered chains of elements, i.e. r(λ) = max{p λ 0 < λ 1 < < λ p Λ} Since the dimension function of Λ is strict order-preserving, it follows that d Λ r(λ). For a poset Λ we denote by Λ (1) the induced order complex of Λ. It is a ranked poset of geometric dimension d Λ (1) = r(λ) and minimal rank m Λ (1) = 0. The p-skeleton of Λ (1) consists of sequences λ 0 < λ 1 < < λ p and the ordering is by inclusion. One can show that the order complex Λ (1) has the structure of a simplicial complex, i.e. a cell complex where every q-cell, q 1, has exactly q + 1 faces, λ = {τ 0, τ 1,..., τ q }, such that if q 2, τ i τ j is a (q 2)-cell for any pair i j. The order complex Λ (1) is equipped with the local orientation ɛ given by ɛ(λ 0 < ˆλ i < λ p λ 0 < < λ i < < λ p ) = ( 1) i

3 COHOMOLOGY OF PROJECTIVE SYSTEMS ON RANKED POSETS 3 2. Cellular (co-)homology Definition 2.1. Let Λ be a poset, and let A be the category of abelian groups (or any abelian category). A projective system with values in A on Λ is a contravariant functor F : Λ A, where Λ is considered as a category, i.e. for any λ Λ we associate an object F (λ), and for a relation λ < σ, a morphism F λ<σ : F (σ) F (λ) in A. Let Λ be a locally oriented ranked poset of geometric dimension d Λ, with local orientation ɛ, and let F be a projective system on Λ. We define a chain complex C p (Λ, F ) = λ Λ p F (λ)[λ] p 0 with differential δ : C p (Λ, F ) C p 1 (Λ, F ) given by δ(f σ [σ]) = ɛ λ<σ F λ<σ (f σ )[λ] for any f σ F (σ). By the local orientation property, δ 2 = 0. In fact, δ 2 (f σ [σ]) = ɛ λ<τ ɛ τ<σ F λ<σ (f σ )[λ] = ( ɛ λ<τ ɛ τ<σ ) F λ<σ (f σ )[λ] = 0 τ σ λ τ λ 2 σ λ<τ<σ Definition 2.2. The homology groups of the complex (C (Λ, F ), δ) H p (Λ, F ) = H p (C (Λ, F )), p 0 are called the cellular homology groups of the locally oriented ranked poset Λ with coefficients in the projective system F. Notice that equivalent local orientations give isomorphic cellular homology groups. Let F be a projective system of abelian groups on Λ. Define a cochain complex C p (Λ, F ) = λ Λ p F (λ ) with differential : C p (Λ, F ) C p+1 (Λ, F ) given by ξ(σ) = ɛ λ<σ Fσ <λ ξ(λ) Again we have 2 = 0 by the local orientation property. Definition 2.3. The cohomology groups of the complex (C (Λ, F ), ) H p (Λ, F ) = H p (C (Λ, F ), ), p 0 are called the cellular cohomology groups of the locally oriented ranked poset Λ with coefficients in the projective system F. A projective system F on Λ induces a projective system F = Hom k (F, k) on Λ by and Fσ <λ : F (λ ) F (σ ) given by F (λ ) = Hom k (F (λ), k) = F (λ) F σ <λ (φ(λ))(f σ) = φ(λ) F λ<σ (f σ ) where φ F, and φ(λ) : F (λ) k. Thus we have C p (Λ, F ) = F (λ ) = Hom k (F (λ), k) λ Λ p λ Λ p = Hom k ( λ Λ p F (λ), k) = Hom k (C p (Λ, F ), k) = C p (Λ, F )

4 4 ARNE B. SLETSJØE The differential : C p (Λ, F ) C p+1 (Λ, F ) of the cochain complex is induced by the differential δ : C p+1 (Λ, F ) C p (Λ, F ). In fact we have φ(σ)(f σ ) = ɛ λ<σ F σ <λ φ(λ)(f λ) = ( ) ɛ λ<σ φ(λ) Fλ<σ (fλ ) = φ ( for any σ Λ p+1. It follows that ɛ λ<σ F λ<σ ) (fλ [λ]) = φ(δ(f σ [σ]) H q (Λ, F ) H q (Λ, F ), q 0 For the constant projective system F = Z on Λ we write H p (Λ, Z) = H p (Λ) (resp. H p (Λ, Z ) = H p (Λ)). Notice also that for finite Λ and a projective system F on Λ we have an isomorphism C p (Λ, F ) = β F (λ) F (λ)[λ] = C d p (Λ, F ) λ (Λ ) p λ Λ d p given by β(ξ) = It is easily seen that β (ξ) = δβ(ξ). Thus we have, λ Λ d p ξ(λ )[λ] Proposition 2.4. Let Λ be a locally oriented finite poset, and F a projective system of abelian groups on Λ. Then there are natural isomorphisms where d = d Λ is the geometric dimension of Λ. H p (Λ, F ) H d p (Λ, F ), p 0 3. Limits of projective systems Let Λ be a finite poset, and Λ 1 Λ a closed subposet. Let C Λ be the abelian category of projective systems on Λ with values in the category A of abelian groups. The category C Λ has enough injectives and projectives. As in [6] we define a covariant functor lim : C Λ A as follows; for any projective system F, the projective limit lim F is an abelian group, together with a family of group homomorphisms Π λ : lim F F (λ). It is unique, up to isomorphism, and universal with the above property. The homomorphisms define a natural transformation lim F F, of the constant projective system lim F into F. For all λ Λ 1, we have Π λ = 0. One can show that the limit exist and that the functor is left exact. If Λ 1 =, we set lim = lim. Λ Λ/ Denote by Z Λ/Λ1 the projective system on Λ given by Z Λ/Λ1 (λ) = Z if λ Λ 1 and Z Λ/Λ1 (λ) = 0 if λ Λ 1. Then we have [6] lim ( ) F = R lim F Ext C Λ (Z Λ/Λ1, F ) The functor lim is left-exact, thus an exact sequence 0 F F F 0

5 COHOMOLOGY OF PROJECTIVE SYSTEMS ON RANKED POSETS 5 of projective systems of abelian groups on Λ induces a long-exact sequence of abelian groups for j 0. lim (j) F lim (j) F lim (j) F lim (j+1) F In [6] it is shown that the complex D p (Λ, F ) = λ 0<λ 1< <λ p Λ with differential δ : D p (Λ, F ) D p+1 (Λ, F ) given by F (λ 0 ) p+1 δξ(λ 0 < < λ p+1 ) = F λ0<λ 1 ξ(λ 1 < < λ p+1 ) + ( 1) i ξ(λ 0 < ˆλ i < λ p+1 ) is a resolving complex for the inverse limit functor, i.e. we have i=1 H p (D (Λ, F )) = lim Λ (p) F, p 0 There is also a relative version of the D-complex. Let Λ 1 Λ be a closed subposet. Define In this case we have D p (Λ, Λ 1, F ) = {ξ D p (Λ, F ) ξ(λ 0 < λ 1 < < λ p ) = 0 if λ p Λ 1 } H p (D (Λ, Λ 1, F )) = lim (p) F p 0 A projective system F on Λ induces a projective system F on the dual of the order complex, (Λ (1) ), given by F (λ 0 < < λ p ) = F (λ 0 ) and F (λ 0 < ˆλ i < λ p λ 0 < < λ p ) = { Fλ0<λ 1 if i = 0 Id F (λ0) if i 0 By similarity of the definitions we have D p (Λ, F ) = C p (Λ (1), F ). Denote by D p (F ), for p 0, the projective system on Λ given by D p (F )(λ) = C p (ˆλ (1), F ) = F (λ 0 ) λ 0<λ 1< <λ p λ where, for λ < σ, D p (F )(σ) D p (F )(λ) is the projection. The differential δ : D p (F )(λ) D p+1 (F )(λ) is given by p+1 δξ(λ 0 < < λ p+1 λ) = F λ0<λ 1 ξ(λ 1 < < λ p+1 λ)+ ( 1) i ξ(λ 0 < ˆλ i < λ p+1 λ) In fact, (D (F ), δ) defines a projective system of cochain complexes on Λ and we have D (Λ, F ) = lim Λ D (F ) i=1 We define a double complex by considering the projective system D (F ) as a projective system on Λ Λ. The double complex is given by C p,q = C p (Λ, D q (F )) The differential δ : C p,q C p,q+1 is the differential of the complex D (ˆλ, F ), for any λ Λ and : C p,q C p+1,q is the differential of the cell complex. It is obvious that the two differentials commute, i.e. δ = δ. The total differential of the double complex D = + ( 1) p δ satisfies D 2 = 0. It is a first quadrant double complex, and the two spectral sequences 2 = H p (Λ (q), lim F ) ˆλ E p,q

6 6 ARNE B. SLETSJØE and E p,q 2 = H q (H p (Λ, D (F ))) both converge to the cohomology of the total complex. Lemma 3.1. For any λ Λ we have { (q) F (λ) if q = 0 lim F = 0 if q 0 ˆλ Proof. We define a contracting cochain homotopy s : C q+1 (ˆλ (1), F ) C q (ˆλ (1), F ) by { 0 if λq = λ sξ(λ 0 < < λ q λ) = ξ(λ 0 < < λ q < λ λ) else For λ q λ, we have ( s s )ξ(λ 0 < < λ q λ) = F λ0<λ 1 (ξ(λ 1 < < λ q < λ λ)) + F λ0<λ 1 (ξ(λ 1 < < λ q < λ)) q ( 1) i ξ(λ 0 < ˆλ i < λ q < λ λ) i=1 q ( 1) i ξ(λ 0 < ˆλ i < λ q < λ λ) ( 1) q+1 ξ(λ 0 < < λ q λ) = ( 1) q ξ(λ 0 < < λ q λ) i=1 For λ q = λ we have ( s s )ξ(λ 0 < < λ q λ) = ( 1) q ξ(λ 0 < < λ q 1 < λ q λ) It follows that the first spectral sequences degenerates and we have, { 2 = H p (Λ (q) H, lim F p (Λ, F ) for q = 0 ) = 0 for q 0 E p,q ˆλ Denote by F j the projective system on (Λ (1) ) given by F j (λ 0 < < λ q ) = C j ( ˆλ q, F (λ 0 )) where F (λ 0 ) denotes the constant projective system on ˆλ q. An inclusion of sequences λ 0 < ˆλ i < λ q λ 0 < < λ q gives rise to a map F j (λ 0 < ˆλ i < λ q ) F j (λ 0 < < λ q ) which is the projection for i = q, the map F (λ 1 ) F (λ 0 ) for i = 0, and the identity for 0 < i < q. Let ξ C p (Λ, D q (F )). For a q-cell λ 0 < < λ q of Λ (1) define ξ [λ0,...,λ q] C p ( ˆλ q, F (λ 0 )) by for λ ( ˆλ q) p. ξ [λ0,...,λ q](λ ) = ξ(λ )(λ 0 < < λ q λ) Proposition 3.2. Fix q 0. The map ξ ξ induces an isomorphism of cochain complexes C p (Λ, D q (F )) C p ( ˆλ q, F (λ 0 )) λ 0< <λ q

7 COHOMOLOGY OF PROJECTIVE SYSTEMS ON RANKED POSETS 7 Proof. We have an isomorphism of cochain groups C p (Λ, D q (F )) = F (λ 0 ) = λ (Λ ) p λ 0< <λ q<λ = λ 0< <λ q C p ( ˆλ q, F (λ 0 )) λ 0< <λ q λ <λ q λ (Λ )p F (λ 0 ) where F (λ 0 ) is the constant projective system. For σ ˆλ q, i.e. for λ q σ we have and ξ [λ0...λ q](σ ) = ξ(σ )(λ 0 < < λ q σ) = λ σ ɛ σ<λ D q (F ) σ<λ ξ(λ )(λ 0 < < λ q σ) = λ σ ɛ σ<λ ξ(λ )(λ 0 < < λ q λ) ξ [λ0...λ q](σ ) = ɛ σ<λ ξ [λ0...λ q](λ ) λ σ = λ σ ɛ σ<λ ξ(λ )(λ 0 < < λ q λ) which shows that the map is a map of cochains. Thus, for the second spectral sequence we have E p,q 2 = H q (H p (C (Λ, D (F )))) = H q (H p ( = H q ( λ 0< <λ H p Thus, we have proved the following theorem, λ 0< <λ C ( ˆλ, F (λ 0 )))) ( ) ) ( ) ˆλ, F (λ 0 ) = lim (q) H p ˆλ Λ, F (λ 0 ) Theorem 3.3. There is a first quadrant spectral sequence converging to cellular cohomology H n (Λ, F ) E p,q 2 = lim Λ (q) H p ( ˆλ, F (λ 0 )) If Λ has acyclic closed cells, i.e. H p ( ˆλ, F (λ 0 )) = { F (λ0 ) for p = 0 0 for p 0 the spectral sequence degenerates, and we obtain the main result, Corollary 3.4. Let Λ be a locally oriented combinatorial cell complex of geometrical dimension d, such that Λ has acyclic closed cells, and let F be projective system of A-modules on Λ. Then we have H p (Λ, F ) = lim Λ (d p) F, p 0 where d is the geometric dimension of Λ. Proof. In case of acyclic closed cells, the two spectral sequences degenerate. Combining this with Proposition 2.4 the result follows.

8 8 ARNE B. SLETSJØE An important tool in computations of inverse limits is the use of κ-functors. Let Γ and Λ be two posets. A order-preserving map κ : Γ Λ (1) such that κ(γ) Λ (1) is closed for all γ Γ is called a κ-functor of Γ in Λ. For a projective system F on Λ we define a projective system on Γ by γ limf Denote by im κ = γ Γ κ(γ) Λ. Then for any γ Γ there is a canonical homomorphism κ(γ) limf limf im κ κ(γ) and this family of homomorphisms define a canonical homomorphism limf lim limf Γ im κ Theorem 3.5. Let κ : Γ Λ (1) be a κ-functor with im κ = Λ, and such tht if γ 1, γ 2 Γ, and λ κ(γ 1 ) κ(γ 2 ), then there exixts γ < γ 1, γ 2 such that λ κ(γ). Then there is a spectral sequence E p,q 2 = lim (p) lim (q) Γ F converging to lim ( ) F Λ κ(γ) κ(γ) Proof. See [6] for a proof. References [1] Basak, Tathagata: Combinatorial cell complexes and Poincaré duality, Geom. Dedicata 147 (2010) pp: [2] Billera, Louis J.: Homology of smooth splines: generic triangulations and a conjecture of Strang, Trans. Amer. Math. Soc. 310 (1988), no. 1, pp: [3] Deng, Jiansong, Chen, Falai, Feng, YuYu: Dimensions of spline spaces over??-meshes, J. Comput. Appl. Math. 194 (2006), no. 2, pp: [4] Deng, Jiansong, Chen, Falai, Jin, Liangbing: Dimensions of biquadratic spline spaces over T-meshes, J. Comput. Appl. Math. 238 (2013), pp: [5] Dokken, Tor, Lyche, Tom, Pettersen, Kjell Fredrik: Polynomial splines over locally refined box-partitions, Comput. Aided Geom. Design 30 (2013), no. 3, pp: [6] Laudal, Olav Arnfinn: Sur les limites projectives et inductives, Ann. sci. de l École Normale Supérieure 82.2 (1965) pp: [7] Mourrain, Bernard: On the dimension of spline spaces on planar T-meshes, Math. Comp. 83 (2014), pp: [8] Mourrain, Bernard, Villamizar, Nelly: Homological techniques for the analysis of the dimension of triangular spline spaces Journal of Symbolic Computation 50, (2013) pp: [9] Schenck, Hal: A Spectral Sequence for Splines Adv. in Appl. Math. 19, (1997) pp: Matematisk institutt, University of Oslo, Pb. 1053, Blindern, N-0316 Oslo, Norway address: arnebs@math.uio.no

2 Composition. Invertible Mappings

2 Composition. Invertible Mappings Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,

Διαβάστε περισσότερα

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal

Διαβάστε περισσότερα

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that

Διαβάστε περισσότερα

EE512: Error Control Coding

EE512: Error Control Coding EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3

Διαβάστε περισσότερα

Congruence Classes of Invertible Matrices of Order 3 over F 2

Congruence Classes of Invertible Matrices of Order 3 over F 2 International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and

Διαβάστε περισσότερα

Homomorphism in Intuitionistic Fuzzy Automata

Homomorphism in Intuitionistic Fuzzy Automata International Journal of Fuzzy Mathematics Systems. ISSN 2248-9940 Volume 3, Number 1 (2013), pp. 39-45 Research India Publications http://www.ripublication.com/ijfms.htm Homomorphism in Intuitionistic

Διαβάστε περισσότερα

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all

Διαβάστε περισσότερα

Example Sheet 3 Solutions

Example Sheet 3 Solutions Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note

Διαβάστε περισσότερα

Statistical Inference I Locally most powerful tests

Statistical Inference I Locally most powerful tests Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided

Διαβάστε περισσότερα

de Rham Theorem May 10, 2016

de Rham Theorem May 10, 2016 de Rham Theorem May 10, 2016 Stokes formula and the integration morphism: Let M = σ Σ σ be a smooth triangulated manifold. Fact: Stokes formula σ ω = σ dω holds, e.g. for simplices. It can be used to define

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: linear functions Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U

Διαβάστε περισσότερα

Every set of first-order formulas is equivalent to an independent set

Every set of first-order formulas is equivalent to an independent set Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent

Διαβάστε περισσότερα

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018 Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals

Διαβάστε περισσότερα

Fractional Colorings and Zykov Products of graphs

Fractional Colorings and Zykov Products of graphs Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is

Διαβάστε περισσότερα

Uniform Convergence of Fourier Series Michael Taylor

Uniform Convergence of Fourier Series Michael Taylor Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula

Διαβάστε περισσότερα

Chapter 3: Ordinal Numbers

Chapter 3: Ordinal Numbers Chapter 3: Ordinal Numbers There are two kinds of number.. Ordinal numbers (0th), st, 2nd, 3rd, 4th, 5th,..., ω, ω +,... ω2, ω2+,... ω 2... answers to the question What position is... in a sequence? What

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS

MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS FUMIE NAKAOKA AND NOBUYUKI ODA Received 20 December 2005; Revised 28 May 2006; Accepted 6 August 2006 Some properties of minimal closed sets and maximal closed

Διαβάστε περισσότερα

Lecture 15 - Root System Axiomatics

Lecture 15 - Root System Axiomatics Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the

Διαβάστε περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 Autoregressive Moving Average Model ARMA(1,1) 84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this

Διαβάστε περισσότερα

SOME PROPERTIES OF FUZZY REAL NUMBERS

SOME PROPERTIES OF FUZZY REAL NUMBERS Sahand Communications in Mathematical Analysis (SCMA) Vol. 3 No. 1 (2016), 21-27 http://scma.maragheh.ac.ir SOME PROPERTIES OF FUZZY REAL NUMBERS BAYAZ DARABY 1 AND JAVAD JAFARI 2 Abstract. In the mathematical

Διαβάστε περισσότερα

A Note on Intuitionistic Fuzzy. Equivalence Relation

A Note on Intuitionistic Fuzzy. Equivalence Relation International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com

Διαβάστε περισσότερα

Problem Set 3: Solutions

Problem Set 3: Solutions CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C

Διαβάστε περισσότερα

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p) Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok

Διαβάστε περισσότερα

ORDINAL ARITHMETIC JULIAN J. SCHLÖDER

ORDINAL ARITHMETIC JULIAN J. SCHLÖDER ORDINAL ARITHMETIC JULIAN J. SCHLÖDER Abstract. We define ordinal arithmetic and show laws of Left- Monotonicity, Associativity, Distributivity, some minor related properties and the Cantor Normal Form.

Διαβάστε περισσότερα

5. Choice under Uncertainty

5. Choice under Uncertainty 5. Choice under Uncertainty Daisuke Oyama Microeconomics I May 23, 2018 Formulations von Neumann-Morgenstern (1944/1947) X: Set of prizes Π: Set of probability distributions on X : Preference relation

Διαβάστε περισσότερα

On a four-dimensional hyperbolic manifold with finite volume

On a four-dimensional hyperbolic manifold with finite volume BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In

Διαβάστε περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.S. 430 Assignment 6, Sample Solutions C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order

Διαβάστε περισσότερα

12. Radon-Nikodym Theorem

12. Radon-Nikodym Theorem Tutorial 12: Radon-Nikodym Theorem 1 12. Radon-Nikodym Theorem In the following, (Ω, F) is an arbitrary measurable space. Definition 96 Let μ and ν be two (possibly complex) measures on (Ω, F). We say

Διαβάστε περισσότερα

DIRECT PRODUCT AND WREATH PRODUCT OF TRANSFORMATION SEMIGROUPS

DIRECT PRODUCT AND WREATH PRODUCT OF TRANSFORMATION SEMIGROUPS GANIT J. Bangladesh Math. oc. IN 606-694) 0) -7 DIRECT PRODUCT AND WREATH PRODUCT OF TRANFORMATION EMIGROUP ubrata Majumdar, * Kalyan Kumar Dey and Mohd. Altab Hossain Department of Mathematics University

Διαβάστε περισσότερα

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =

Διαβάστε περισσότερα

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ. Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action

Διαβάστε περισσότερα

Commutative Monoids in Intuitionistic Fuzzy Sets

Commutative Monoids in Intuitionistic Fuzzy Sets Commutative Monoids in Intuitionistic Fuzzy Sets S K Mala #1, Dr. MM Shanmugapriya *2 1 PhD Scholar in Mathematics, Karpagam University, Coimbatore, Tamilnadu- 641021 Assistant Professor of Mathematics,

Διαβάστε περισσότερα

Homomorphism of Intuitionistic Fuzzy Groups

Homomorphism of Intuitionistic Fuzzy Groups International Mathematical Forum, Vol. 6, 20, no. 64, 369-378 Homomorphism o Intuitionistic Fuzz Groups P. K. Sharma Department o Mathematics, D..V. College Jalandhar Cit, Punjab, India pksharma@davjalandhar.com

Διαβάστε περισσότερα

Cyclic or elementary abelian Covers of K 4

Cyclic or elementary abelian Covers of K 4 Cyclic or elementary abelian Covers of K 4 Yan-Quan Feng Mathematics, Beijing Jiaotong University Beijing 100044, P.R. China Summer School, Rogla, Slovenian 2011-06 Outline 1 Question 2 Main results 3

Διαβάστε περισσότερα

Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.

Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X. Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:

Διαβάστε περισσότερα

Tridiagonal matrices. Gérard MEURANT. October, 2008

Tridiagonal matrices. Gérard MEURANT. October, 2008 Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,

Διαβάστε περισσότερα

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Partial Differential Equations in Biology The boundary element method. March 26, 2013 The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

Section 8.3 Trigonometric Equations

Section 8.3 Trigonometric Equations 99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.

Διαβάστε περισσότερα

Concrete Mathematics Exercises from 30 September 2016

Concrete Mathematics Exercises from 30 September 2016 Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)

Διαβάστε περισσότερα

Finite Field Problems: Solutions

Finite Field Problems: Solutions Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The

Διαβάστε περισσότερα

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)

Διαβάστε περισσότερα

derivation of the Laplacian from rectangular to spherical coordinates

derivation of the Laplacian from rectangular to spherical coordinates derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used

Διαβάστε περισσότερα

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required) Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts

Διαβάστε περισσότερα

ST5224: Advanced Statistical Theory II

ST5224: Advanced Statistical Theory II ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known

Διαβάστε περισσότερα

Differential forms and the de Rham cohomology - Part I

Differential forms and the de Rham cohomology - Part I Differential forms and the de Rham cohomology - Part I Paul Harrison University of Toronto October 30, 2009 I. Review Triangulation of Manifolds M = smooth, compact, oriented n-manifold. Can triangulate

Διαβάστε περισσότερα

Abstract Storage Devices

Abstract Storage Devices Abstract Storage Devices Robert König Ueli Maurer Stefano Tessaro SOFSEM 2009 January 27, 2009 Outline 1. Motivation: Storage Devices 2. Abstract Storage Devices (ASD s) 3. Reducibility 4. Factoring ASD

Διαβάστε περισσότερα

Matrices and Determinants

Matrices and Determinants Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z

Διαβάστε περισσότερα

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch: HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying

Διαβάστε περισσότερα

Intuitionistic Fuzzy Ideals of Near Rings

Intuitionistic Fuzzy Ideals of Near Rings International Mathematical Forum, Vol. 7, 202, no. 6, 769-776 Intuitionistic Fuzzy Ideals of Near Rings P. K. Sharma P.G. Department of Mathematics D.A.V. College Jalandhar city, Punjab, India pksharma@davjalandhar.com

Διαβάστε περισσότερα

1. Introduction and Preliminaries.

1. Introduction and Preliminaries. Faculty of Sciences and Mathematics, University of Niš, Serbia Available at: http://www.pmf.ni.ac.yu/filomat Filomat 22:1 (2008), 97 106 ON δ SETS IN γ SPACES V. Renuka Devi and D. Sivaraj Abstract We

Διαβάστε περισσότερα

ω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω

ω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω 0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +

Διαβάστε περισσότερα

New bounds for spherical two-distance sets and equiangular lines

New bounds for spherical two-distance sets and equiangular lines New bounds for spherical two-distance sets and equiangular lines Michigan State University Oct 8-31, 016 Anhui University Definition If X = {x 1, x,, x N } S n 1 (unit sphere in R n ) and x i, x j = a

Διαβάστε περισσότερα

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other Test Constructions: Likelihood Ratio & Bayes Tests Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :

Διαβάστε περισσότερα

The Probabilistic Method - Probabilistic Techniques. Lecture 7: The Janson Inequality

The Probabilistic Method - Probabilistic Techniques. Lecture 7: The Janson Inequality The Probabilistic Method - Probabilistic Techniques Lecture 7: The Janson Inequality Sotiris Nikoletseas Associate Professor Computer Engineering and Informatics Department 2014-2015 Sotiris Nikoletseas,

Διαβάστε περισσότερα

Homework 3 Solutions

Homework 3 Solutions Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For

Διαβάστε περισσότερα

Section 7.6 Double and Half Angle Formulas

Section 7.6 Double and Half Angle Formulas 09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)

Διαβάστε περισσότερα

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β 3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

Second Order Partial Differential Equations

Second Order Partial Differential Equations Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y

Διαβάστε περισσότερα

The challenges of non-stable predicates

The challenges of non-stable predicates The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates

Διαβάστε περισσότερα

Bounding Nonsplitting Enumeration Degrees

Bounding Nonsplitting Enumeration Degrees Bounding Nonsplitting Enumeration Degrees Thomas F. Kent Andrea Sorbi Università degli Studi di Siena Italia July 18, 2007 Goal: Introduce a form of Σ 0 2-permitting for the enumeration degrees. Till now,

Διαβάστε περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)

Διαβάστε περισσότερα

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. Dirac Equation. Hamiltonian. Dirac Eq. 6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2

Διαβάστε περισσότερα

w o = R 1 p. (1) R = p =. = 1

w o = R 1 p. (1) R = p =. = 1 Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:

Διαβάστε περισσότερα

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R + Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b

Διαβάστε περισσότερα

THE SECOND ISOMORPHISM THEOREM ON ORDERED SET UNDER ANTIORDERS. Daniel A. Romano

THE SECOND ISOMORPHISM THEOREM ON ORDERED SET UNDER ANTIORDERS. Daniel A. Romano 235 Kragujevac J. Math. 30 (2007) 235 242. THE SECOND ISOMORPHISM THEOREM ON ORDERED SET UNDER ANTIORDERS Daniel A. Romano Department of Mathematics and Informatics, Banja Luka University, Mladena Stojanovića

Διαβάστε περισσότερα

Generating Set of the Complete Semigroups of Binary Relations

Generating Set of the Complete Semigroups of Binary Relations Applied Mathematics 06 7 98-07 Published Online January 06 in SciRes http://wwwscirporg/journal/am http://dxdoiorg/036/am067009 Generating Set of the Complete Semigroups of Binary Relations Yasha iasamidze

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max

Διαβάστε περισσότερα

Local Approximation with Kernels

Local Approximation with Kernels Local Approximation with Kernels Thomas Hangelbroek University of Hawaii at Manoa 5th International Conference Approximation Theory, 26 work supported by: NSF DMS-43726 A cubic spline example Consider

Διαβάστε περισσότερα

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8  questions or comments to Dan Fetter 1 Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test

Διαβάστε περισσότερα

Coefficient Inequalities for a New Subclass of K-uniformly Convex Functions

Coefficient Inequalities for a New Subclass of K-uniformly Convex Functions International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for

Διαβάστε περισσότερα

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =? Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least

Διαβάστε περισσότερα

Lecture 34 Bootstrap confidence intervals

Lecture 34 Bootstrap confidence intervals Lecture 34 Bootstrap confidence intervals Confidence Intervals θ: an unknown parameter of interest We want to find limits θ and θ such that Gt = P nˆθ θ t If G 1 1 α is known, then P θ θ = P θ θ = 1 α

Διαβάστε περισσότερα

Approximation of distance between locations on earth given by latitude and longitude

Approximation of distance between locations on earth given by latitude and longitude Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth

Διαβάστε περισσότερα

The Simply Typed Lambda Calculus

The Simply Typed Lambda Calculus Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and

Διαβάστε περισσότερα

Second Order RLC Filters

Second Order RLC Filters ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor

Διαβάστε περισσότερα

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1. Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given

Διαβάστε περισσότερα

On the Galois Group of Linear Difference-Differential Equations

On the Galois Group of Linear Difference-Differential Equations On the Galois Group of Linear Difference-Differential Equations Ruyong Feng KLMM, Chinese Academy of Sciences, China Ruyong Feng (KLMM, CAS) Galois Group 1 / 19 Contents 1 Basic Notations and Concepts

Διαβάστε περισσότερα

Lecture 21: Properties and robustness of LSE

Lecture 21: Properties and robustness of LSE Lecture 21: Properties and robustness of LSE BLUE: Robustness of LSE against normality We now study properties of l τ β and σ 2 under assumption A2, i.e., without the normality assumption on ε. From Theorem

Διαβάστε περισσότερα

Chapter 2. Ordinals, well-founded relations.

Chapter 2. Ordinals, well-founded relations. Chapter 2. Ordinals, well-founded relations. 2.1. Well-founded Relations. We start with some definitions and rapidly reach the notion of a well-ordered set. Definition. For any X and any binary relation

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013 Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή

Διαβάστε περισσότερα

Some new generalized topologies via hereditary classes. Key Words:hereditary generalized topological space, A κ(h,µ)-sets, κµ -topology.

Some new generalized topologies via hereditary classes. Key Words:hereditary generalized topological space, A κ(h,µ)-sets, κµ -topology. Bol. Soc. Paran. Mat. (3s.) v. 30 2 (2012): 71 77. c SPM ISSN-2175-1188 on line ISSN-00378712 in press SPM: www.spm.uem.br/bspm doi:10.5269/bspm.v30i2.13793 Some new generalized topologies via hereditary

Διαβάστε περισσότερα

Sequent Calculi for the Modal µ-calculus over S5. Luca Alberucci, University of Berne. Logic Colloquium Berne, July 4th 2008

Sequent Calculi for the Modal µ-calculus over S5. Luca Alberucci, University of Berne. Logic Colloquium Berne, July 4th 2008 Sequent Calculi for the Modal µ-calculus over S5 Luca Alberucci, University of Berne Logic Colloquium Berne, July 4th 2008 Introduction Koz: Axiomatisation for the modal µ-calculus over K Axioms: All classical

Διαβάστε περισσότερα

6.3 Forecasting ARMA processes

6.3 Forecasting ARMA processes 122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear

Διαβάστε περισσότερα

Heisenberg Uniqueness pairs

Heisenberg Uniqueness pairs Heisenberg Uniqueness pairs Philippe Jaming Bordeaux Fourier Workshop 2013, Renyi Institute Joint work with K. Kellay Heisenberg Uniqueness Pairs µ : finite measure on R 2 µ(x, y) = R 2 e i(sx+ty) dµ(s,

Διαβάστε περισσότερα

Iterated trilinear fourier integrals with arbitrary symbols

Iterated trilinear fourier integrals with arbitrary symbols Cornell University ICM 04, Satellite Conference in Harmonic Analysis, Chosun University, Gwangju, Korea August 6, 04 Motivation the Coifman-Meyer theorem with classical paraproduct(979) B(f, f )(x) :=

Διαβάστε περισσότερα

Homework 8 Model Solution Section

Homework 8 Model Solution Section MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx

Διαβάστε περισσότερα

Affine Weyl Groups. Gabriele Nebe. Summerschool GRK 1632, September Lehrstuhl D für Mathematik

Affine Weyl Groups. Gabriele Nebe. Summerschool GRK 1632, September Lehrstuhl D für Mathematik Affine Weyl Groups Gabriele Nebe Lehrstuhl D für Mathematik Summerschool GRK 1632, September 2015 Crystallographic root systems. Definition A crystallographic root system Φ is a finite set of non zero

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr (T t N n) Pr (max (X 1,..., X N ) t N n) Pr (max

Διαβάστε περισσότερα

Lecture 2. Soundness and completeness of propositional logic

Lecture 2. Soundness and completeness of propositional logic Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness

Διαβάστε περισσότερα

D Alembert s Solution to the Wave Equation

D Alembert s Solution to the Wave Equation D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique

Διαβάστε περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- ----------------- Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin

Διαβάστε περισσότερα

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1 Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the

Διαβάστε περισσότερα

UNIT - I LINEAR ALGEBRA. , such that αν V satisfying following condition

UNIT - I LINEAR ALGEBRA. , such that αν V satisfying following condition UNIT - I LINEAR ALGEBRA Definition Vector Space : A non-empty set V is said to be vector space over the field F. If V is an abelian group under addition and if for every α, β F, ν, ν 2 V, such that αν

Διαβάστε περισσότερα

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ. Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +

Διαβάστε περισσότερα

Higher Derivative Gravity Theories

Higher Derivative Gravity Theories Higher Derivative Gravity Theories Black Holes in AdS space-times James Mashiyane Supervisor: Prof Kevin Goldstein University of the Witwatersrand Second Mandelstam, 20 January 2018 James Mashiyane WITS)

Διαβάστε περισσότερα