Accepted Manuscript. Guillaume Marrelec, Habib Benali. S (08)00059-X DOI: /j.spl Reference: STAPRO 4923.

Size: px
Start display at page:

Download "Accepted Manuscript. Guillaume Marrelec, Habib Benali. S (08)00059-X DOI: /j.spl Reference: STAPRO 4923."

Transcription

1 Accepted Manuscrpt Condtonal ndependence between two varables gven any condtonng subset mples block dagonal covarance matrx for multvarate Gaussan dstrbutons Gullaume Marrelec Habb Benal PII: S (8)59-X DOI: 1116/spl2816 Reference: STAPRO 4923 To appear n: Statstcs and Probablty Letters Receved date: 23 Aprl 27 Revsed date: 3 July 27 Accepted date: 9 January 28 Please cte ths artcle as: Marrelec G Benal H Condtonal ndependence between two varables gven any condtonng subset mples block dagonal covarance matrx for multvarate Gaussan dstrbutons Statstcs and Probablty Letters (28) do:1116/spl2816 Ths s a PDF fle of an unedted manuscrpt that has been accepted for publcaton As a servce to our customers we are provdng ths early verson of the manuscrpt The manuscrpt wll undergo copyedtng typesettng and revew of the resultng proof before t s publshed n ts fnal form Please note that durng the producton process errors may be dscovered whch could affect the content and all legal dsclamers that apply to the ournal pertan

2 Condtonal Independence Between Two Varables Gven Any Condtonng Subset Imples Block Dagonal Covarance Matrx for Multvarate Gaussan Dstrbutons Gullaume Marrelec ab Habb Benal ab a Inserm U678 Pars F-7513 France b Unversté Perre et Mare Cure Faculté de médecne Pté-Salpêtrère Pars F-7513 France Abstract Let x = (x ) be a multvarate Gaussan varable wth covarance matrx Σ For and n we show that f the condtonal covarance between x and x gven any condtonng set \ { } s equal to zero then Σ s block dagonal and and belong to two dfferent blocks Key words: multvarate Gaussan varables condtonal ndependence block dagonal covarance matrx 1 Introducton As ponted out by Dawd (1998) the concept of condtonal ndependence s beleved to be fundamental knowledge n the process of scentfc nference For multvarate Gaussan varables condtonal ndependence s quantfed by condtonal covarance Investgaton of such coeffcents have led to a better characterzaton of nteractons between varables n partcular through the use of condtonal ndependence graphs (Whttaker 199; Laurtzen 1996; Edwards 2) Margnal correlaton coeffcents have also been examned through covarance graphs (Kauermann 1996; Edwards 2) It would be nterestng Correspondng author Address: CHU Pté-Salpêtrère 91 boulevard de l Hôptal Pars Cedex 13 France Emal address: marrelec@medusseufr (Gullaume Marrelec) Preprnt submtted to Elsever Scence 3 July 27

3 to generalze these approaches by smultaneously consderng all possble condtonal covarances for a gven par of varables For nstance consder the case of a three dmensonal Gaussan varable x = (x 1 x 2 x 3 ) wth covarance matrx Σ If Corr [x 1 x 2 x 3 ] = then Corr [x 1 x 2 ] = Corr [x 1 x 3 ] Corr [x 2 x 3 ] (Wermuth 1976; Whttaker 199) If one furthermore has Corr [x 1 x 2 ] = t drectly comes out that ether Corr [x 1 x 3 ] = or Corr [x 2 x 3 ] = In other words the followng yelds: { Corr [x1 x 2 ] = and Corr [x 1 x 2 x 3 ] = } Σ s block dagonal To our knowledge no generalzaton of such a result has been shown yet Ths paper s a frst step n ths drecton We prove a result that demonstrates how ths approach can nform us regardng the global pattern of nteracton and shed lght nto the structure of the varables 2 Man theorem Let be a fnte set and x = (x ) be a multvarate Gaussan varable ndexed on wth covarance matrx Σ Theorem 1 Let and be two elements of and further assume that x and x are condtonally ndependent gven any set of remanng varables e \ { } Cov [x x x ] = (1) Then Σ s block dagonal and and belong to two dfferent blocks Sole consderaton of margnal and/or partal covarance s not suffcent to provde ths result for there exst covarance matrces that are not block dagonal whle ncludng varables for whch Cov [x x ] = and/or Cov [ x x x \{ı}] = Ths result can be establshed by successve examnaton of condtonal ndependence constrants (see Fg 1 for a graphcal sketch of proof) Frst Corr[x x ] = and hence Σ = We also have Cov[x x x k ] = for any k \ { } Snce Σ = ths covarance coeffcent s equal to (Anderson 1958) Cov[x x x k ] = Σ kσ k Σ kk For Cov[x x x k ] to be equal to zero we must then have Σ k Σ k = e ether Σ k = or Σ k = Ths lne of reasonng beng vald for any k { } t s possble to separate \ { } nto three sets: 1 such that Σ k and Σ k = for k 1; 1 such that Σ k = and Σ k for k 1; and 1 2

4 such that Σ k = and Σ k = for k 1 Let then be = {k l} wth k 1 and l 1 Cov[x x x ] s gven by (see Eq (A1)) ab ( 1) pos (a)+pos (b) det [ Σ \{b} \{a} (Σ ) a det [Σ ] ] (Σ ) b where pos (a) stands for the poston of a n Snce k 1 and l 1 we have Σ l = Σ k = Drect calculaton then shows that Cov[x x x ] s equal to Cov[x x x ] = Σ kσ kl Σ l Σ kk Σ ll Σ 2 kk Snce we must also have Cov[x x x ] = accordng to our hypothess ths equaton leads to Σ kl = gven that Σ k and Σ l are dfferent from zero Elements of 1 (resp 1) have hence a zero margnal correlaton to both (resp ) and all elements of 1 (resp 1) We then proceed by nducton Assume that there exst 2(N + 1) subsets and n wth n = N and one set N of such that = {} and = {}; { N N N} s a partton of nonzero margnal correlatons can only be found between between n 1 and n or between N and { N N} all margnal correlatons between n 1 and n as well as between and n are dfferent from zero n 1 and n n n 1 Snce we proved that Σ = Σ l = for l 1 Σ k = for k 1 Σ kl = for (k l) 1 1 and constructed 1 and 1 so that Σ k for k 1 and Σ l for l 1 the assumpton holds for N = 1 We now assume that t also holds for a gven N 1 If N s empty then the process stops Otherwse the frst step conssts of settng = {k 1 l 1 k N l N m} wth (k n l n ) n n for n = 1 N and m N Gven the assumpton of ndependence between x and x we must have Cov[x x x ] = Ths condtonal covarance coeffcent s equal to (cf Eq (A2)) Σ k1 Σ l1 [ n=1n 1 Σ knk n+1 Σ lnl n+1 ] ΣkN mσ ln m det [Σ ] and s equal to zero f and only f Σ kn mσ ln m = snce by constructon all Σ knk n+1 and Σ lnl n+1 are dfferent from zero It s then possble to separate N nto three sets: N+1 such that Σ kn m and Σ ln m = for all m N+1; N+1 such that Σ kn m = and Σ ln m for all m N+1; and N+1 such that Σ kn m = Σ ln m = for all m N+1 It now remans to prove that we have Σ kl = for (k l) N+1 N+1 To ths am set = {k 1 l 1 k N+1 l N+1 } wth (k n l n ) n n for n = 1 N +1 Snce 3

5 x and x are ndependent we must have Cov[x x x ] = Ths quantty beng equal to (see Eq (A3)) Cov [x x x ] = Σ [ ] k 1 Σ l1 n=1n Σ knk n+1σ lnl n+1 ΣkN+1l N+1 det [Σ ] t s equal to zero f and only f Σ kn+1 l N+1 = The assumpton s therefore also vald for N + 1 The sequence ( N) s of decreasng cardnal beng a fnte set there exsts a step N for whch N s empty: the process ends there Set = {V N } and = { N } { } s hence a partton of for whch there exsts no margnal correlaton between an element of and an element of Consequently the covarance matrx of x has the followng structural form: Σ Σ thereby provng the theorem 3 Dscusson and perspectves In ths paper we consdered x = (x ) a multvarate Gaussan varable wth covarance matrx Σ For and n we showed that f the condtonal covarance between x and x gven any condtonng set \ { } was equal to zero then Σ was block dagonal and and belonged to two dfferent blocks Note that the converse of ths theorem s straghtforward Indeed f one consders that the covarance matrx Σ s block dagonal then any condtonal covarance between varables belongng to two dfferent blocks s equal to zero accordng to Eq (A1) Theorem 1 shows that for multvarate Gaussan varables there s a clear separaton between two varables x and x that are ndependent wth regard to any condtonng subset and that ths separaton also apples to all other varables whch are ether wth x or wth x Consequently ther effect can be analyzed ndependently n one block of varables or the other Interestngly ths result ncely relates two dstnct propertes of Gaussan dstrbutons The block dagonal property of the covarance matrx s clearly a global feature of Gaussan probablty dstrbutons By contrast the relatonshp of complete ndependence (e condtoned on all subsets) s rather a local descrpton and characterzaton of the nteracton structure between varables snce the defnton gves a partcular role to x and x Ths perspectve dffers from the common approach where one usually sets a level 4

6 of condtonng (margnal for covarance graphs partal for condtonal ndependence graphs) and then vares the two varables on whch correlaton s calculated In ths dual approach the defnton does not so much depend on the condtonng set than on the varables whose condtonal covarance we examne We manly focus on the ndependence pattern that can be exhbted wth a sngle par of varables and ts potental mplcatons onto the global structure We beleve that there s much to gan by analyzng varables from ths perspectve and hope to be able to provde further results along the same lnes n the near future 4 Acknowledgments We are n debt to an anonymous referee for pontng out that the result exposed here s well-known for three dmensonal Gaussan varables A Calculaton of Cov [x x x ] The condtonal covarance between and gven reads (Anderson 1958) Cov[x x x ] = Σ ab (Σ ) a [ (Σ ) 1] ab (Σ ) b Calculatng (Σ ) 1 from the adont matrx (Horn and Johnson 1999) yelds for Cov[x x x ]: Σ ab ( 1) pos (a)+pos (b) det [ Σ \{b} \{a} (Σ ) a det [Σ ] ] (Σ ) b (A1) where pos (a) stands for the poston of a n From now on we also assume that there exst 2(N +1)+1 subsets of namely n n wth n = N and N respectng the condtons detaled on page 3 Frst for N 1 set = {k 1 l 1 k N l N m} k n n and l n n for n = 1 N and m N By constructon only elements n 1 (resp 1) have nonzero margnal covarance wth (resp ) Consequently the sum n Equaton (A1) can be smplfed nto ] ( 1) pos (a)+pos (b) det [ Σ \{l 1 } \{k 1 } Σ k1 Σ l1 det [Σ ] Gven the defnton of Σ Σ \{l 1 } \{k 1 } and the determnant of the latter matrx respectvely read 5

7 wth Σ = Σ \{l 1 } \{k 1 } = Σ k1 k 1 Σ k1 k 2 Σ l1 l 1 Σ l1 l 2 Σ k1 k 2 Σ k2 k 2 Σ k2 k 3 Σ l1 l 2 Σ l2 l 2 Σ l2 l 3 Σ ln 1 l N Σ ln 1 l N 1 Σ ln 1 l N 1 Σ kn 1 k Σ N kn k Σ N kn m Σ ln 1 l N Σ ln l N Σ ln m Σ kn m Σ ln m Σ mm Σ k1 k 2 Σ k2 k 2 Σ k2 k 3 Σ l1 l 2 Σ l2 l 2 Σ l2 l 3 Σ k2 k 3 Σ k3 k 3 Σ k3 k 4 Σ ln 1 l N Σ ln 1 l N 1 Σ ln 1 l N 1 Σ kn 1 k Σ N kn k Σ N kn m Σ ln 1 l N Σ ln l N Σ ln m Σ kn m Σ ln m Σ mm det [ Σ \{l 1 } \{k 1 }] = Σk1 k 2 det ( Σ \{l 1 k 1 } \{k 1 k 2 }) Σ \{l 1 k 1 } \{k 1 k 2 } = and hence Ths leads to Σ k2 k 3 Σ l1 l 2 Σ l2 l 2 Σ l2 l 3 Σ k3 k 3 Σ k3 k 4 Σ l2 l 3 Σ l3 l 3 Σ l3 l 4 Σ ln 1 l N Σ ln 1 l N 1 Σ ln 1 l N 1 Σ kn 1 k Σ N kn k Σ N kn m Σ ln 1 l N Σ ln l N Σ ln m Σ kn m Σ ln m Σ mm det ( Σ \{l 1 k 1 } \{k 1 k 2 }) = Σl1 l 2 det ( Σ \{l 1 k 1 l 2 } \{k 1 l 1 k 2 }) det [ Σ \{l 1 } \{k 1 }] = Σk1 k 2 Σ l1 l 2 det ( Σ \{l 1 k 1 l 2 } \{k 1 l 1 k 2 }) 6

8 wth Σ \{l 1 k 1 l 2 } \{k 1 k 2 l 1 } = Σ k2 k 3 Σ k3 k 3 Σ k3 k 4 Σ l2 l 3 Σ l3 l 3 Σ l3 l 4 Σ l3 l 4 Σ k4 k 4 Σ k4 k 5 Σ ln 1 l N Σ ln 1 l N 1 Σ ln 1 l N 1 Σ kn 1 k Σ N kn k Σ N kn m Σ ln 1 l N Σ ln l N Σ ln m Σ kn m Σ ln m Σ mm whch s of the same form as Σ \{l 1 } \{k 1 } Consequently a smlar calculaton shows that det ( Σ \{l 1 k 1 l 2 } \{k 1 l 1 k 2 }) = Σk2 k 3 Σ l2 l 3 det ( Σ \{l 1 k 1 l 2 k 2 l 3 } \{k 1 l 1 k 2 l 2 k 3 }) and by nducton one can hence easly show that for all n 2 det ( Σ \{l 1 k 1 l n 1 k n 1 l n} \{k 1 l 1 k n 1 l n 1 k n}) = Σ knk n+1 Σ lnl n+1 det ( Σ \{l 1 k 1 l nk nl n+1 } \{k 1 l 1 k nl nk n+1 l n}) We hence obtan that det [ Σ \{l 1 } \{k 1 }] = det ( Σ \{l 1 k 1 k N 2 l N 2 l N 1 } \{k 1 l 1 k N 2 l N 2 k N 1 } where the matrx of the rght-hand sde s equal to Σ {kn 1 k N l nm}{l N 1 k N l N m} = Σ kn 1 k N Σ kn k N Σ kn m Σ ln 1 l N Σ ln l N Σ ln m Σ kn m Σ ln m Σ mm ) The determnant of ths matrx can be obtaned by a smlar argument as prevously developed: det ( ) Σ kn m Σ {kn 1 k N l nm}{l N 1 k N l N m} = ΣkN 1k Σ ln 1 l Σ N N ln l Σ N ln m We fnally have det [ Σ \{l 1 } \{k 1 }] = ΣkN mσ ln m Σ ln m Σ mm Σ = Σ kn 1 k N Σ kn m ln 1 l N Σ ln m Σ mm = Σ kn 1 k N Σ ln 1 l N Σ kn mσ ln m 7 n=1n 1 Σ knk n+1 Σ lnl n+1 n=1n 2 Σ knk n+1 Σ lnl n+1

9 and n concluson for = {k 1 l 1 k N l N m} we obtan for Cov [x x x ] [ ] [ ] Σ k1 n=1n 1 Σ knk n+1 ΣkN m Σ l1 n=1n 1 Σ lnl n+1 ΣlN m (A2) det [Σ ] The second case s rather smlar to the frst one Set = {k 1 l 1 k N+1 l N+1 } wth N 1 k n n and l n n for n = 1 N +1 The prevous lne of reasonng can be appled n ths case too except that Σ \{l 1 k 1 l N 1 } \{k 1 l 1 k N 1 } reads Σ {kn 1 k N l N k N+1 l N+1 }{l N 1 k N l N k N+1 l N+1 } = Σ kn 1 k N Σ kn k N Σ kn k N+1 Σ ln 1 l N Σ ln l N Σ ln l N+1 Σ kn k N+1 Σ kn+1 k N+1 Σ kn+1 l N+1 Σ ln l N+1 Σ kn+1 l N+1 Σ ln l N leadng to a determnant of Σ \{l 1 k 1 l N 1 } \{k 1 l 1 k N 1 } equal to Σ kn k N+1 Σ = Σ ln 1 l Σ kn 1 k N N ln l Σ N ln l N+1 Σ kn+1 k Σ N+1 kn+1 l N+1 Σ ln l Σ N+1 ln l N Σ kn k N+1 = Σ kn 1 k N Σ ln 1 Σ l N kn+1 k Σ N+1 kn+1 l N+1 Σ ln l Σ N+1 ln l N Σ kn+1 l N+1 = Σ kn 1 k N Σ ln 1 l N Σ kn k N+1 Σ ln l N+1 Σ ln l N = Σ kn 1 k N Σ ln 1 l N Σ kn k N+1 Σ ln l N+1 Σ kn+1 l N+1 Fnally Cov [x x x ] reads [ ] [ ] Σ k1 n=1n Σ knk n+1 Σl1 n=1n Σ lnl n+1 ΣkN+1 l N+1 (A3) det [Σ ] References Anderson T W 1958 An Introducton to Multvarate Statstcal Analyss Wley Publcatons n Statstcs John Wley and Sons New York Dawd A P 1998 Condtonal ndependence In: Kotz S Read C B Banks D L (Eds) Encyclopeda of Statstcal Scences Vol 2 Wley pp Edwards D 2 Introducton to Graphcal Modellng 2nd Edton Sprnger Texts n Statstcs Sprnger New York 8

10 Horn R A Johnson C R 1999 Matrx Analyss Cambrdge Unversty Press Kauermann G 1996 On a dualzaton of graphcal Gaussan models Scand J Statst Laurtzen S L 1996 Graphcal Models Oxford Unversty Press Oxford Wermuth N 1976 Analoges between multplcatve models n contgency tables and covarance selecton Bometrcs Whttaker J 199 Graphcal Models n Appled Multvarate Statstcs J Wley and Sons Chchester 9

11 1 (a) Fg 1 Sketch of proof From an orgnal parttonng of nto { N that for all elements of N there can be no margnal covarance wth both N and covarate wth N (gathered n N+1 ) elements that covarate wth (gathered n (gathered n N+1) (b) Last we show that elements of N+1 and (b) N N+1 N N N+1 N } (a) we We then p ) and elem must have zero margnal co

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

Composite Hypotheses testing

Composite Hypotheses testing Composte ypotheses testng In many hypothess testng problems there are many possble dstrbutons that can occur under each of the hypotheses. The output of the source s a set of parameters (ponts n a parameter

More information

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4)

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4) I. Classcal Assumptons Econ7 Appled Econometrcs Topc 3: Classcal Model (Studenmund, Chapter 4) We have defned OLS and studed some algebrac propertes of OLS. In ths topc we wll study statstcal propertes

More information

ISQS 6348 Final Open notes, no books. Points out of 100 in parentheses. Y 1 ε 2

ISQS 6348 Final Open notes, no books. Points out of 100 in parentheses. Y 1 ε 2 ISQS 6348 Fnal Open notes, no books. Ponts out of 100 n parentheses. 1. The followng path dagram s gven: ε 1 Y 1 ε F Y 1.A. (10) Wrte down the usual model and assumptons that are mpled by ths dagram. Soluton:

More information

Volume 18 Figure 1. Notation 1. Notation 2. Observation 1. Remark 1. Remark 2. Remark 3. Remark 4. Remark 5. Remark 6. Theorem A [2]. Theorem B [2].

Volume 18 Figure 1. Notation 1. Notation 2. Observation 1. Remark 1. Remark 2. Remark 3. Remark 4. Remark 5. Remark 6. Theorem A [2]. Theorem B [2]. Bulletn of Mathematcal Scences and Applcatons Submtted: 016-04-07 ISSN: 78-9634, Vol. 18, pp 1-10 Revsed: 016-09-08 do:10.1805/www.scpress.com/bmsa.18.1 Accepted: 016-10-13 017 ScPress Ltd., Swtzerland

More information

An (almost) unbiased estimator for the S-Gini index

An (almost) unbiased estimator for the S-Gini index An (almost unbased estmator for the S-Gn ndex Thomas Demuynck February 25, 2009 Abstract Ths note provdes an unbased estmator for the absolute S-Gn and an almost unbased estmator for the relatve S-Gn for

More information

ANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U)

ANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U) Econ 413 Exam 13 H ANSWERS Settet er nndelt 9 deloppgaver, A,B,C, som alle anbefales å telle lkt for å gøre det ltt lettere å stå. Svar er gtt . Unfortunately, there s a prntng error n the hnt of

More information

Self-complementing permutations of k-uniform hypergraphs

Self-complementing permutations of k-uniform hypergraphs Dscrete Mathematcs Theoretcal Computer Scence DMTCS vol. 11:1, 2009, 117 124 Self-complementng permutatons of k-unform hypergraphs Artur Szymańsk A. Paweł Wojda Faculty of Appled Mathematcs, AGH Unversty

More information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

Remarks on the Properties of a Quasi-Fibonacci-like Polynomial Sequence

Remarks on the Properties of a Quasi-Fibonacci-like Polynomial Sequence Remarks on the Propertes of a Quas-Fbonacc-lke Polynomal Sequence Brce Merwne LIU Brooklyn Ilan Wenschelbaum Wesleyan Unversty Abstract Consder the Quas-Fbonacc-lke Polynomal Sequence gven by F 0 = 1,

More information

2.3 Nilpotent endomorphisms

2.3 Nilpotent endomorphisms s a block dagonal matrx, wth A Mat dm U (C) In fact, we can assume that B = B 1 B k, wth B an ordered bass of U, and that A = [f U ] B, where f U : U U s the restrcton of f to U 40 23 Nlpotent endomorphsms

More information

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family IOSR Journal of Mathematcs IOSR-JM) ISSN: 2278-5728. Volume 3, Issue 3 Sep-Oct. 202), PP 44-48 www.osrjournals.org Usng T.O.M to Estmate Parameter of dstrbutons that have not Sngle Exponental Famly Jubran

More information

j) = 1 (note sigma notation) ii. Continuous random variable (e.g. Normal distribution) 1. density function: f ( x) 0 and f ( x) dx = 1

j) = 1 (note sigma notation) ii. Continuous random variable (e.g. Normal distribution) 1. density function: f ( x) 0 and f ( x) dx = 1 Random varables Measure of central tendences and varablty (means and varances) Jont densty functons and ndependence Measures of assocaton (covarance and correlaton) Interestng result Condtonal dstrbutons

More information

More metrics on cartesian products

More metrics on cartesian products More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of

More information

Inductance Calculation for Conductors of Arbitrary Shape

Inductance Calculation for Conductors of Arbitrary Shape CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors

More information

Applied Mathematics Letters

Applied Mathematics Letters Appled Matheatcs Letters 2 (2) 46 5 Contents lsts avalable at ScenceDrect Appled Matheatcs Letters journal hoepage: wwwelseverco/locate/al Calculaton of coeffcents of a cardnal B-splne Gradr V Mlovanovć

More information

EPR Paradox and the Physical Meaning of an Experiment in Quantum Mechanics. Vesselin C. Noninski

EPR Paradox and the Physical Meaning of an Experiment in Quantum Mechanics. Vesselin C. Noninski EPR Paradox and the Physcal Meanng of an Experment n Quantum Mechancs Vesseln C Nonnsk vesselnnonnsk@verzonnet Abstract It s shown that there s one purely determnstc outcome when measurement s made on

More information

The Exact Formulation of the Inverse of the Tridiagonal Matrix for Solving the 1D Poisson Equation with the Finite Difference Method

The Exact Formulation of the Inverse of the Tridiagonal Matrix for Solving the 1D Poisson Equation with the Finite Difference Method Journal of Electromagnetc Analyss and Applcatons, 04, 6, 0-08 Publshed Onlne September 04 n ScRes. http://www.scrp.org/journal/jemaa http://dx.do.org/0.46/jemaa.04.6000 The Exact Formulaton of the Inverse

More information

Comparison of Regression Lines

Comparison of Regression Lines STATGRAPHICS Rev. 9/13/2013 Comparson of Regresson Lnes Summary... 1 Data Input... 3 Analyss Summary... 4 Plot of Ftted Model... 6 Condtonal Sums of Squares... 6 Analyss Optons... 7 Forecasts... 8 Confdence

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

APPROXIMATE PRICES OF BASKET AND ASIAN OPTIONS DUPONT OLIVIER. Premia 14

APPROXIMATE PRICES OF BASKET AND ASIAN OPTIONS DUPONT OLIVIER. Premia 14 APPROXIMAE PRICES OF BASKE AND ASIAN OPIONS DUPON OLIVIER Prema 14 Contents Introducton 1 1. Framewor 1 1.1. Baset optons 1.. Asan optons. Computng the prce 3. Lower bound 3.1. Closed formula for the prce

More information

Christian Aebi Collège Calvin, Geneva, Switzerland

Christian Aebi Collège Calvin, Geneva, Switzerland #A7 INTEGERS 12 (2012) A PROPERTY OF TWIN PRIMES Chrstan Aeb Collège Calvn, Geneva, Swtzerland chrstan.aeb@edu.ge.ch Grant Carns Department of Mathematcs, La Trobe Unversty, Melbourne, Australa G.Carns@latrobe.edu.au

More information

The Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices

The Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan

More information

On Finite Rank Perturbation of Diagonalizable Operators

On Finite Rank Perturbation of Diagonalizable Operators Functonal Analyss, Approxmaton and Computaton 6 (1) (2014), 49 53 Publshed by Faculty of Scences and Mathematcs, Unversty of Nš, Serba Avalable at: http://wwwpmfnacrs/faac On Fnte Rank Perturbaton of Dagonalzable

More information

On the correction of the h-index for career length

On the correction of the h-index for career length 1 On the correcton of the h-ndex for career length by L. Egghe Unverstet Hasselt (UHasselt), Campus Depenbeek, Agoralaan, B-3590 Depenbeek, Belgum 1 and Unverstet Antwerpen (UA), IBW, Stadscampus, Venusstraat

More information

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 3, Issue 1, July 2013

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 3, Issue 1, July 2013 ISSN: 2277-375 Constructon of Trend Free Run Orders for Orthogonal rrays Usng Codes bstract: Sometmes when the expermental runs are carred out n a tme order sequence, the response can depend on the run

More information

Computation of Higher Order Moments from Two Multinomial Overdispersion Likelihood Models

Computation of Higher Order Moments from Two Multinomial Overdispersion Likelihood Models Computaton of Hgher Order Moments from Two Multnomal Overdsperson Lkelhood Models BY J. T. NEWCOMER, N. K. NEERCHAL Department of Mathematcs and Statstcs, Unversty of Maryland, Baltmore County, Baltmore,

More information

Randić Energy and Randić Estrada Index of a Graph

Randić Energy and Randić Estrada Index of a Graph EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 5, No., 202, 88-96 ISSN 307-5543 www.ejpam.com SPECIAL ISSUE FOR THE INTERNATIONAL CONFERENCE ON APPLIED ANALYSIS AND ALGEBRA 29 JUNE -02JULY 20, ISTANBUL

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009 College of Computer & Informaton Scence Fall 2009 Northeastern Unversty 20 October 2009 CS7880: Algorthmc Power Tools Scrbe: Jan Wen and Laura Poplawsk Lecture Outlne: Prmal-dual schema Network Desgn:

More information

Lecture 3 Stat102, Spring 2007

Lecture 3 Stat102, Spring 2007 Lecture 3 Stat0, Sprng 007 Chapter 3. 3.: Introducton to regresson analyss Lnear regresson as a descrptve technque The least-squares equatons Chapter 3.3 Samplng dstrbuton of b 0, b. Contnued n net lecture

More information

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2 Salmon: Lectures on partal dfferental equatons 5. Classfcaton of second-order equatons There are general methods for classfyng hgher-order partal dfferental equatons. One s very general (applyng even to

More information

Discussion 11 Summary 11/20/2018

Discussion 11 Summary 11/20/2018 Dscusson 11 Summary 11/20/2018 1 Quz 8 1. Prove for any sets A, B that A = A B ff B A. Soluton: There are two drectons we need to prove: (a) A = A B B A, (b) B A A = A B. (a) Frst, we prove A = A B B A.

More information

A new construction of 3-separable matrices via an improved decoding of Macula s construction

A new construction of 3-separable matrices via an improved decoding of Macula s construction Dscrete Optmzaton 5 008 700 704 Contents lsts avalable at ScenceDrect Dscrete Optmzaton journal homepage: wwwelsevercom/locate/dsopt A new constructon of 3-separable matrces va an mproved decodng of Macula

More information

Chat eld, C. and A.J.Collins, Introduction to multivariate analysis. Chapman & Hall, 1980

Chat eld, C. and A.J.Collins, Introduction to multivariate analysis. Chapman & Hall, 1980 MT07: Multvarate Statstcal Methods Mke Tso: emal mke.tso@manchester.ac.uk Webpage for notes: http://www.maths.manchester.ac.uk/~mkt/new_teachng.htm. Introducton to multvarate data. Books Chat eld, C. and

More information

Perron Vectors of an Irreducible Nonnegative Interval Matrix

Perron Vectors of an Irreducible Nonnegative Interval Matrix Perron Vectors of an Irreducble Nonnegatve Interval Matrx Jr Rohn August 4 2005 Abstract As s well known an rreducble nonnegatve matrx possesses a unquely determned Perron vector. As the man result of

More information

Hidden Markov Models & The Multivariate Gaussian (10/26/04)

Hidden Markov Models & The Multivariate Gaussian (10/26/04) CS281A/Stat241A: Statstcal Learnng Theory Hdden Markov Models & The Multvarate Gaussan (10/26/04) Lecturer: Mchael I. Jordan Scrbes: Jonathan W. Hu 1 Hdden Markov Models As a bref revew, hdden Markov models

More information

Here is the rationale: If X and y have a strong positive relationship to one another, then ( x x) will tend to be positive when ( y y)

Here is the rationale: If X and y have a strong positive relationship to one another, then ( x x) will tend to be positive when ( y y) Secton 1.5 Correlaton In the prevous sectons, we looked at regresson and the value r was a measurement of how much of the varaton n y can be attrbuted to the lnear relatonshp between y and x. In ths secton,

More information

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens THE CHINESE REMAINDER THEOREM KEITH CONRAD We should thank the Chnese for ther wonderful remander theorem. Glenn Stevens 1. Introducton The Chnese remander theorem says we can unquely solve any par of

More information

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP C O L L O Q U I U M M A T H E M A T I C U M VOL. 80 1999 NO. 1 FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP BY FLORIAN K A I N R A T H (GRAZ) Abstract. Let H be a Krull monod wth nfnte class

More information

On Graphs with Same Distance Distribution

On Graphs with Same Distance Distribution Appled Mathematcs, 07, 8, 799-807 http://wwwscrporg/journal/am ISSN Onlne: 5-7393 ISSN Prnt: 5-7385 On Graphs wth Same Dstance Dstrbuton Xulang Qu, Xaofeng Guo,3 Chengy Unversty College, Jme Unversty,

More information

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:

More information

Convexity preserving interpolation by splines of arbitrary degree

Convexity preserving interpolation by splines of arbitrary degree Computer Scence Journal of Moldova, vol.18, no.1(52), 2010 Convexty preservng nterpolaton by splnes of arbtrary degree Igor Verlan Abstract In the present paper an algorthm of C 2 nterpolaton of dscrete

More information

Chapter 11: Simple Linear Regression and Correlation

Chapter 11: Simple Linear Regression and Correlation Chapter 11: Smple Lnear Regresson and Correlaton 11-1 Emprcal Models 11-2 Smple Lnear Regresson 11-3 Propertes of the Least Squares Estmators 11-4 Hypothess Test n Smple Lnear Regresson 11-4.1 Use of t-tests

More information

Maximizing the number of nonnegative subsets

Maximizing the number of nonnegative subsets Maxmzng the number of nonnegatve subsets Noga Alon Hao Huang December 1, 213 Abstract Gven a set of n real numbers, f the sum of elements of every subset of sze larger than k s negatve, what s the maxmum

More information

SL n (F ) Equals its Own Derived Group

SL n (F ) Equals its Own Derived Group Internatonal Journal of Algebra, Vol. 2, 2008, no. 12, 585-594 SL n (F ) Equals ts Own Derved Group Jorge Macel BMCC-The Cty Unversty of New York, CUNY 199 Chambers street, New York, NY 10007, USA macel@cms.nyu.edu

More information

Learning Theory: Lecture Notes

Learning Theory: Lecture Notes Learnng Theory: Lecture Notes Lecturer: Kamalka Chaudhur Scrbe: Qush Wang October 27, 2012 1 The Agnostc PAC Model Recall that one of the constrants of the PAC model s that the data dstrbuton has to be

More information

Chapter 8 Indicator Variables

Chapter 8 Indicator Variables Chapter 8 Indcator Varables In general, e explanatory varables n any regresson analyss are assumed to be quanttatve n nature. For example, e varables lke temperature, dstance, age etc. are quanttatve n

More information

The exponential map of GL(N)

The exponential map of GL(N) The exponental map of GLN arxv:hep-th/9604049v 9 Apr 996 Alexander Laufer Department of physcs Unversty of Konstanz P.O. 5560 M 678 78434 KONSTANZ Aprl 9, 996 Abstract A fnte expanson of the exponental

More information

Lecture 16 Statistical Analysis in Biomaterials Research (Part II)

Lecture 16 Statistical Analysis in Biomaterials Research (Part II) 3.051J/0.340J 1 Lecture 16 Statstcal Analyss n Bomaterals Research (Part II) C. F Dstrbuton Allows comparson of varablty of behavor between populatons usng test of hypothess: σ x = σ x amed for Brtsh statstcan

More information

Expected Value and Variance

Expected Value and Variance MATH 38 Expected Value and Varance Dr. Neal, WKU We now shall dscuss how to fnd the average and standard devaton of a random varable X. Expected Value Defnton. The expected value (or average value, or

More information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

STAT 511 FINAL EXAM NAME Spring 2001

STAT 511 FINAL EXAM NAME Spring 2001 STAT 5 FINAL EXAM NAME Sprng Instructons: Ths s a closed book exam. No notes or books are allowed. ou may use a calculator but you are not allowed to store notes or formulas n the calculator. Please wrte

More information

A combinatorial problem associated with nonograms

A combinatorial problem associated with nonograms A combnatoral problem assocated wth nonograms Jessca Benton Ron Snow Nolan Wallach March 21, 2005 1 Introducton. Ths work was motvated by a queston posed by the second named author to the frst named author

More information

A Bayes Algorithm for the Multitask Pattern Recognition Problem Direct Approach

A Bayes Algorithm for the Multitask Pattern Recognition Problem Direct Approach A Bayes Algorthm for the Multtask Pattern Recognton Problem Drect Approach Edward Puchala Wroclaw Unversty of Technology, Char of Systems and Computer etworks, Wybrzeze Wyspanskego 7, 50-370 Wroclaw, Poland

More information

Finding Dense Subgraphs in G(n, 1/2)

Finding Dense Subgraphs in G(n, 1/2) Fndng Dense Subgraphs n Gn, 1/ Atsh Das Sarma 1, Amt Deshpande, and Rav Kannan 1 Georga Insttute of Technology,atsh@cc.gatech.edu Mcrosoft Research-Bangalore,amtdesh,annan@mcrosoft.com Abstract. Fndng

More information

Asymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation

Asymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation Nonl. Analyss and Dfferental Equatons, ol., 4, no., 5 - HIKARI Ltd, www.m-har.com http://dx.do.org/.988/nade.4.456 Asymptotcs of the Soluton of a Boundary alue Problem for One-Characterstc Dfferental Equaton

More information

The Geometry of Logit and Probit

The Geometry of Logit and Probit The Geometry of Logt and Probt Ths short note s meant as a supplement to Chapters and 3 of Spatal Models of Parlamentary Votng and the notaton and reference to fgures n the text below s to those two chapters.

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

Power law and dimension of the maximum value for belief distribution with the max Deng entropy

Power law and dimension of the maximum value for belief distribution with the max Deng entropy Power law and dmenson of the maxmum value for belef dstrbuton wth the max Deng entropy Bngy Kang a, a College of Informaton Engneerng, Northwest A&F Unversty, Yanglng, Shaanx, 712100, Chna. Abstract Deng

More information

Every planar graph is 4-colourable a proof without computer

Every planar graph is 4-colourable a proof without computer Peter Dörre Department of Informatcs and Natural Scences Fachhochschule Südwestfalen (Unversty of Appled Scences) Frauenstuhlweg 31, D-58644 Iserlohn, Germany Emal: doerre(at)fh-swf.de Mathematcs Subject

More information

Assortment Optimization under MNL

Assortment Optimization under MNL Assortment Optmzaton under MNL Haotan Song Aprl 30, 2017 1 Introducton The assortment optmzaton problem ams to fnd the revenue-maxmzng assortment of products to offer when the prces of products are fxed.

More information

On the set of natural numbers

On the set of natural numbers On the set of natural numbers by Jalton C. Ferrera Copyrght 2001 Jalton da Costa Ferrera Introducton The natural numbers have been understood as fnte numbers, ths wor tres to show that the natural numbers

More information

Lecture 10: May 6, 2013

Lecture 10: May 6, 2013 TTIC/CMSC 31150 Mathematcal Toolkt Sprng 013 Madhur Tulsan Lecture 10: May 6, 013 Scrbe: Wenje Luo In today s lecture, we manly talked about random walk on graphs and ntroduce the concept of graph expander,

More information

A Robust Method for Calculating the Correlation Coefficient

A Robust Method for Calculating the Correlation Coefficient A Robust Method for Calculatng the Correlaton Coeffcent E.B. Nven and C. V. Deutsch Relatonshps between prmary and secondary data are frequently quantfed usng the correlaton coeffcent; however, the tradtonal

More information

Linear Regression Analysis: Terminology and Notation

Linear Regression Analysis: Terminology and Notation ECON 35* -- Secton : Basc Concepts of Regresson Analyss (Page ) Lnear Regresson Analyss: Termnology and Notaton Consder the generc verson of the smple (two-varable) lnear regresson model. It s represented

More information

A Hybrid Variational Iteration Method for Blasius Equation

A Hybrid Variational Iteration Method for Blasius Equation Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method

More information

Min Cut, Fast Cut, Polynomial Identities

Min Cut, Fast Cut, Polynomial Identities Randomzed Algorthms, Summer 016 Mn Cut, Fast Cut, Polynomal Identtes Instructor: Thomas Kesselhem and Kurt Mehlhorn 1 Mn Cuts n Graphs Lecture (5 pages) Throughout ths secton, G = (V, E) s a mult-graph.

More information

Difference Equations

Difference Equations Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1

More information

Solution Thermodynamics

Solution Thermodynamics Soluton hermodynamcs usng Wagner Notaton by Stanley. Howard Department of aterals and etallurgcal Engneerng South Dakota School of nes and echnology Rapd Cty, SD 57701 January 7, 001 Soluton hermodynamcs

More information

/ n ) are compared. The logic is: if the two

/ n ) are compared. The logic is: if the two STAT C141, Sprng 2005 Lecture 13 Two sample tests One sample tests: examples of goodness of ft tests, where we are testng whether our data supports predctons. Two sample tests: called as tests of ndependence

More information

Norm Bounds for a Transformed Activity Level. Vector in Sraffian Systems: A Dual Exercise

Norm Bounds for a Transformed Activity Level. Vector in Sraffian Systems: A Dual Exercise ppled Mathematcal Scences, Vol. 4, 200, no. 60, 2955-296 Norm Bounds for a ransformed ctvty Level Vector n Sraffan Systems: Dual Exercse Nkolaos Rodousaks Department of Publc dmnstraton, Panteon Unversty

More information

Case Study of Markov Chains Ray-Knight Compactification

Case Study of Markov Chains Ray-Knight Compactification Internatonal Journal of Contemporary Mathematcal Scences Vol. 9, 24, no. 6, 753-76 HIKAI Ltd, www.m-har.com http://dx.do.org/.2988/cms.24.46 Case Study of Marov Chans ay-knght Compactfcaton HaXa Du and

More information

SUCCESSIVE MINIMA AND LATTICE POINTS (AFTER HENK, GILLET AND SOULÉ) M(B) := # ( B Z N)

SUCCESSIVE MINIMA AND LATTICE POINTS (AFTER HENK, GILLET AND SOULÉ) M(B) := # ( B Z N) SUCCESSIVE MINIMA AND LATTICE POINTS (AFTER HENK, GILLET AND SOULÉ) S.BOUCKSOM Abstract. The goal of ths note s to present a remarably smple proof, due to Hen, of a result prevously obtaned by Gllet-Soulé,

More information

Foundations of Arithmetic

Foundations of Arithmetic Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an

More information

Distribution of subgraphs of random regular graphs

Distribution of subgraphs of random regular graphs Dstrbuton of subgraphs of random regular graphs Zhcheng Gao Faculty of Busness Admnstraton Unversty of Macau Macau Chna zcgao@umac.mo N. C. Wormald Department of Combnatorcs and Optmzaton Unversty of Waterloo

More information

Linear Algebra and its Applications

Linear Algebra and its Applications Lnear Algebra and ts Applcatons 4 (00) 5 56 Contents lsts avalable at ScenceDrect Lnear Algebra and ts Applcatons journal homepage: wwwelsevercom/locate/laa Notes on Hlbert and Cauchy matrces Mroslav Fedler

More information

However, since P is a symmetric idempotent matrix, of P are either 0 or 1 [Eigen-values

However, since P is a symmetric idempotent matrix, of P are either 0 or 1 [Eigen-values Fall 007 Soluton to Mdterm Examnaton STAT 7 Dr. Goel. [0 ponts] For the general lnear model = X + ε, wth uncorrelated errors havng mean zero and varance σ, suppose that the desgn matrx X s not necessarly

More information

Number of cases Number of factors Number of covariates Number of levels of factor i. Value of the dependent variable for case k

Number of cases Number of factors Number of covariates Number of levels of factor i. Value of the dependent variable for case k ANOVA Model and Matrx Computatons Notaton The followng notaton s used throughout ths chapter unless otherwse stated: N F CN Y Z j w W Number of cases Number of factors Number of covarates Number of levels

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,

More information

Department of Quantitative Methods & Information Systems. Time Series and Their Components QMIS 320. Chapter 6

Department of Quantitative Methods & Information Systems. Time Series and Their Components QMIS 320. Chapter 6 Department of Quanttatve Methods & Informaton Systems Tme Seres and Ther Components QMIS 30 Chapter 6 Fall 00 Dr. Mohammad Zanal These sldes were modfed from ther orgnal source for educatonal purpose only.

More information

Probability Theory. The nth coefficient of the Taylor series of f(k), expanded around k = 0, gives the nth moment of x as ( ik) n n!

Probability Theory. The nth coefficient of the Taylor series of f(k), expanded around k = 0, gives the nth moment of x as ( ik) n n! 8333: Statstcal Mechancs I Problem Set # 3 Solutons Fall 3 Characterstc Functons: Probablty Theory The characterstc functon s defned by fk ep k = ep kpd The nth coeffcent of the Taylor seres of fk epanded

More information

Time-Varying Systems and Computations Lecture 6

Time-Varying Systems and Computations Lecture 6 Tme-Varyng Systems and Computatons Lecture 6 Klaus Depold 14. Januar 2014 The Kalman Flter The Kalman estmaton flter attempts to estmate the actual state of an unknown dscrete dynamcal system, gven nosy

More information

A CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS

A CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS Journal of Mathematcal Scences: Advances and Applcatons Volume 25, 2014, Pages 1-12 A CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS JIA JI, WEN ZHANG and XIAOFEI QI Department of Mathematcs

More information

Random Partitions of Samples

Random Partitions of Samples Random Parttons of Samples Klaus Th. Hess Insttut für Mathematsche Stochastk Technsche Unverstät Dresden Abstract In the present paper we construct a decomposton of a sample nto a fnte number of subsamples

More information

Appendix B. Criterion of Riemann-Stieltjes Integrability

Appendix B. Criterion of Riemann-Stieltjes Integrability Appendx B. Crteron of Remann-Steltes Integrablty Ths note s complementary to [R, Ch. 6] and [T, Sec. 3.5]. The man result of ths note s Theorem B.3, whch provdes the necessary and suffcent condtons for

More information

The optimal delay of the second test is therefore approximately 210 hours earlier than =2.

The optimal delay of the second test is therefore approximately 210 hours earlier than =2. THE IEC 61508 FORMULAS 223 The optmal delay of the second test s therefore approxmately 210 hours earler than =2. 8.4 The IEC 61508 Formulas IEC 61508-6 provdes approxmaton formulas for the PF for smple

More information

UNIVERSITY OF TORONTO Faculty of Arts and Science. December 2005 Examinations STA437H1F/STA1005HF. Duration - 3 hours

UNIVERSITY OF TORONTO Faculty of Arts and Science. December 2005 Examinations STA437H1F/STA1005HF. Duration - 3 hours UNIVERSITY OF TORONTO Faculty of Arts and Scence December 005 Examnatons STA47HF/STA005HF Duraton - hours AIDS ALLOWED: (to be suppled by the student) Non-programmable calculator One handwrtten 8.5'' x

More information

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS SECTION 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS 493 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS All the vector spaces you have studed thus far n the text are real vector spaces because the scalars

More information

APPENDIX A Some Linear Algebra

APPENDIX A Some Linear Algebra APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,

More information

20. Mon, Oct. 13 What we have done so far corresponds roughly to Chapters 2 & 3 of Lee. Now we turn to Chapter 4. The first idea is connectedness.

20. Mon, Oct. 13 What we have done so far corresponds roughly to Chapters 2 & 3 of Lee. Now we turn to Chapter 4. The first idea is connectedness. 20. Mon, Oct. 13 What we have done so far corresponds roughly to Chapters 2 & 3 of Lee. Now we turn to Chapter 4. The frst dea s connectedness. Essentally, we want to say that a space cannot be decomposed

More information

x = , so that calculated

x = , so that calculated Stat 4, secton Sngle Factor ANOVA notes by Tm Plachowsk n chapter 8 we conducted hypothess tests n whch we compared a sngle sample s mean or proporton to some hypotheszed value Chapter 9 expanded ths to

More information

Anti-van der Waerden numbers of 3-term arithmetic progressions.

Anti-van der Waerden numbers of 3-term arithmetic progressions. Ant-van der Waerden numbers of 3-term arthmetc progressons. Zhanar Berkkyzy, Alex Schulte, and Mchael Young Aprl 24, 2016 Abstract The ant-van der Waerden number, denoted by aw([n], k), s the smallest

More information

Homework Notes Week 7

Homework Notes Week 7 Homework Notes Week 7 Math 4 Sprng 4 #4 (a Complete the proof n example 5 that s an nner product (the Frobenus nner product on M n n (F In the example propertes (a and (d have already been verfed so we

More information

2016 Wiley. Study Session 2: Ethical and Professional Standards Application

2016 Wiley. Study Session 2: Ethical and Professional Standards Application 6 Wley Study Sesson : Ethcal and Professonal Standards Applcaton LESSON : CORRECTION ANALYSIS Readng 9: Correlaton and Regresson LOS 9a: Calculate and nterpret a sample covarance and a sample correlaton

More information

Graph Reconstruction by Permutations

Graph Reconstruction by Permutations Graph Reconstructon by Permutatons Perre Ille and Wllam Kocay* Insttut de Mathémathques de Lumny CNRS UMR 6206 163 avenue de Lumny, Case 907 13288 Marselle Cedex 9, France e-mal: lle@ml.unv-mrs.fr Computer

More information

Lecture 17 : Stochastic Processes II

Lecture 17 : Stochastic Processes II : Stochastc Processes II 1 Contnuous-tme stochastc process So far we have studed dscrete-tme stochastc processes. We studed the concept of Makov chans and martngales, tme seres analyss, and regresson analyss

More information

2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification

2E Pattern Recognition Solutions to Introduction to Pattern Recognition, Chapter 2: Bayesian pattern classification E395 - Pattern Recognton Solutons to Introducton to Pattern Recognton, Chapter : Bayesan pattern classfcaton Preface Ths document s a soluton manual for selected exercses from Introducton to Pattern Recognton

More information