Appendix. Appendix I. Details used in M-step of Section 4. and expect ultimately it will close to zero. αi =α (r 1) [δq(α i ; α (r 1)

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Appendix. Appendix I. Details used in M-step of Section 4. and expect ultimately it will close to zero. αi =α (r 1) [δq(α i ; α (r 1)"

Transcript

1 Appendx Appendx I. Detals used n M-step of Secton 4. Now wrte h (r) and expect ultmately t wll close to zero. and h (r) = [δq(α ; α (r) )/δα ] α =α (r 1) = [δq(α ; α (r) )/δα ] α =α (r 1) δ log L(α (r 1) )/δα [δq(α ; α (r 1) )/δα ] α =α (r 1) = [ψ(α ) ψ(α j ) + ψ(n j + α (r) j ) ψ(n + α (r) )] α =α (r 1) [ψ(α ) ψ(α j ) + ψ(n j + α (r 1) j ) ψ(n + α (r 1) )] α =α (r 1) = ψ(n j + α (r) j ) ψ(n + α (r) where B (0) matrx e (r) ) ψ(n j + α (r 1) j = α (r) v (r) c (r) α (r 1), error term = h (r) + B (r 1) e (r) ) + ψ(n + α (r 1) ) (A1) = 1/(v (r)t e (r) ) (A2) = I d, whch corresponds to ntal EM gradent step, and f the I c (α (r) ; n ) + B (r) fals to be postve defnte, then t s replaced by I c (α (r) ; n ) + ( 1 2 )m B (r), where m s the smallest postve nteger such that the above matrx s postve defnte. & B (r) = B (r 1) + c (r) v (r) v (r)t, for all = 1,, k (A3) Ideas of (A1), (A2) and (A3) are due to Davdon (1959). Appendx II. Program for smulaton of sample observatons for gven probabltes The smulaton() functon needs an argument. Value of n s the sample sze and p be the vector of probabltes. 1

2 smulaton<- functon(n, p) f(sum(p)!=1.0) stop( Probabltes are not properly gven ) k<- length(p) obs<- matrx(0, ncol=500, nrow= k) rowsum.obs<-c(rep(0,k)) for(j n 1:500) cumul.obs<- c(rep(0, k)) cumul.prob<- c(rep(0, k)) obs[1,j]<- rbnom(1, n, p[1]) cumul.obs[1]<- obs[1,j] cumul.prob[1]<- p[1] for( n 2:k) f((p[]/(1-cumul.prob[-1])) 1.0) obs[,j]<- rbnom(1, n-cumul.obs[-1], p[]/(1-cumul.prob[-1])) else obs<- n - cumul.obs[-1] cumul.obs[]<- cumul.obs[-1]+obs[,j] cumul.prob[]<- cumul.prob[-1]+p[] for( n 1:k) rowsum.obs[]<- sum(obs[, ])/500 return(round(rowsum.obs, dgts=0)) Program for calculaton of rsks for gven observatons and pror The rsk.est() functon needs an argument. Value of N s the sample sze and alpha be the vector of pror parameters. rsk.est<- functon(n, alpha) numer<- 0.0 denom<

3 rsk1<- 0.0 rsk2<- 0.0 rsk<- 0.0 numer<- sum(alpha)*sum(alpha)-sum(alpha*alpha) denom1<- sum(n)*sum(alpha)*(sum(alpha)+1) denom2<- (sum(n)+sum(alpha))*sum(alpha)*(sum(alpha)+1) rsk1<- numer/denom1 cat( Bayes rsk of unbased estmate ) prnt(rsk1) rsk2<- numer/denom2 cat( Bayes rsk of Bayes estmate ) prnt(rsk2) k<- length(alpha) f(length(n)!=k) stop( Gven vectors are not of same dmenson ) fsher.nf<- matrx(0,ncol=k,nrow=k) nv.fnf<- matrx(0,ncol=k,nrow=k) B0<- dag(k) B<- matrx(0,ncol=k,nrow=k) D<- matrx(0,ncol=k,nrow=k) S<- rep(0,k) d<- rep(0,k) v<- rep(0,k) h<- rep(0,k) hd<- matrx(0, 500, k) w<- rep(1,k) z<- numerc(0) g<- 0 m<- 0 u<- rep(0,k) eps< for(j n 1:k) D[j,j]<- trgamma(alpha[j])-trgamma(n[j]+alpha[j]) u[j]<- dgamma(alpha[j])-dgamma(n[j]+alpha[j]) hd[1,j]<- dgamma(n[j]+alpha[j])-dgamma(sum(n)+sum(alpha)) 3

4 z<- trgamma(sum(alpha))-trgamma(sum(n)+sum(alpha)) g<- dgamma(sum(alpha))-dgamma(sum(n)+sum(alpha)) fsher.nf<- D-z*(w%*%t(w)) nv.fnf<- solve(fsher.nf+b0) d<- nv.fnf%*%s alpha<- alpha + d f(any(abs(d) eps,na.rm=f)) break for(r n 2:500) f(any(alpha =0.0)) alpha=alpha-mn(alpha)+1 for(j n 1:k) D[j,j]<- trgamma(alpha[j])-trgamma(n[j]+alpha[j]) u[j]<- dgamma(alpha[j])-dgamma(n[j]+alpha[j]) hd[r,j]<- dgamma(n[j]+alpha[j])-dgamma(sum(n)+sum(alpha)) z<- trgamma(sum(alpha))-trgamma(sum(n)+sum(alpha)) g<- dgamma(sum(alpha))-dgamma(sum(n)+sum(alpha)) fsher.nf<- D-z*(w%*%t(w)) h<- hd[r, ]-hd[r-1, ] v<- h+b0%*%d m<- t(v)%*%d q<- matrx(m, ncol=k, nrow=k) P<- v%*%t(v) B<- B0+(P/q) nv.fnf<- solve(fsher.nf+b) d<- nv.fnf%*%s alpha -alpha+d f(any(abs(d) eps, na.rm=f)) break cat( Estmate of drchlet parameter ) prnt(alpha) numer<- sum(alpha)*sum(alpha)-sum(alpha*alpha) denom<-(sum(n)+sum(alpha))*sum(alpha)*(sum(alpha)+1) rsk<- numer/denom cat( Bayes rsk of emprcal Bayes estmate ) prnt(rsk) 4

5 Appendx III. Program for Emprcal Bayes estmator of transton probablty matrx when all states have dfferent pror (Drchlet) parameters usng EM algorthm. The embayes.est() functon needs an argument. Value of N s the sample transton matrx and alpha s the ntal value of the Drchlet parameters. embayes.est<- functon(n, alpha) f(ncol(n)!=nrow(n)) stop( Gven matrx s not a square one ) f(ncol(alpha)!=nrow(alpha)) stop( Gven parameter matrx s not asquare one ) f(ncol(n)!=ncol(alpha)) stop( Gven matrces are not of same dmenton ) k<-ncol(n) bayes.est<- matrx(0,ncol=k,nrow=k) embayes.est<- matrx(0,ncol=k,nrow=k) fsher.nf<- matrx(0,ncol=k,nrow=k) nv.fnf<- matrx(0,ncol=k,nrow=k) B0<- dag(k) B<- matrx(0,ncol=k,nrow=k) D<- matrx(0,ncol=k,nrow=k) P<- matrx(0,ncol=k,nrow=k) S<- rep(0,k) d<- rep(0,k) v<- rep(0,k) h<- rep(0,k) hd<- matrx(0,100,k) w<- rep(1,k) z<- 0 g<- 0 m<- 0 u<- rep(0,k) eps<

6 #Loop for Bayes estmate# for( n 1:k) for(j n 1:k) bayes.est[,j]=(n[,j]+alpha[,j])/(sum(n[,])+sum(alpha[,])) cat( Bayes estmate of transton pobablty matrx ) prnt(bayes.est) #To calculate Fsher nformaton matrx# for( n 1:k) for(j n 1:k) D[j,j]<- trgamma(alpha[,j])-trgamma(n[,j]+alpha[,j]) u[j]<- dgamma(alpha[,j])-dgamma(n[,j]+alpha[,j]) hd[1,j]<- dgamma(n[,j]+alpha[,j])-dgamma(sum(n[,])+sum(alpha[,])) z<- trgamma(sum(alpha[,]))-trgamma(sum(n[,])+sum(alpha[,])) g<- dgamma(sum(alpha[,]))-dgamma(sum(n[,])+sum(alpha[,])) fsher.nf<- D-z*(w%*%t(w)) nv.fnf<- solve(fsher.nf+b0) d<- nv.fnf%*%s alpha[,] -alpha[,]+d f(any(abs(d)<eps,na.rm=f)) break for(r n 2:100) f(any(alpha[, ]<=0.0)) alpha[, ]<- alpha[, ]-mn(alpha[,])+1 for(j n 1:k) D[j,j]<- trgamma(alpha[,j])-trgamma(n[,j]+alpha[,j]) u[j]<- dgamma(alpha[,j])-dgamma(n[,j]+alpha[,j]) hd[r,j]<- dgamma(n[,j]+alpha[,j])-dgamma(sum(n[,])+sum(alpha[,])) z<- trgamma(sum(alpha[,]))-trgamma(sum(n[,])+sum(alpha[,])) g<- dgamma(sum(alpha[,]))-dgamma(sum(n[,])+sum(alpha[,])) fsher.nf<- D-z*(w%*%t(w)) h<- hd[r, ]-hd[r-1, ] v<- h+b0%*%d 6

7 m<- t(v)%*%d q<- matrx(m, ncol=k, nrow=k) P<- v%*%t(v) B<- B0+P/q nv.fnf<- solve(fsher.nf+b) d<- nv.fnf%*%s alpha[,]<- alpha[,]+d f(any(abs(d)<eps, na.rm=f)) break cat( Estmate of Drchlet parameter. ) prnt(alpha) for( n 1:k) for(j n 1:k) embayes.est[, j]<- (N[, j]+alpha[, j])/(sum(n[, ])+sum(alpha[, ])) cat( Emprcal Bayes estmate of tranton probablty matrx. ) prnt(embayes.est) 7

One and two particle density matrices for single determinant HF wavefunctions. (1) = φ 2. )β(1) ( ) ) + β(1)β * β. (1)ρ RHF

One and two particle density matrices for single determinant HF wavefunctions. (1) = φ 2. )β(1) ( ) ) + β(1)β * β. (1)ρ RHF One and two partcle densty matrces for sngle determnant HF wavefunctons One partcle densty matrx Gven the Hartree-Fock wavefuncton ψ (,,3,!, = Âϕ (ϕ (ϕ (3!ϕ ( 3 The electronc energy s ψ H ψ = ϕ ( f ( ϕ

Διαβάστε περισσότερα

Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών. ΗΥ-570: Στατιστική Επεξεργασία Σήµατος. ιδάσκων : Α. Μουχτάρης. εύτερη Σειρά Ασκήσεων.

Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών. ΗΥ-570: Στατιστική Επεξεργασία Σήµατος. ιδάσκων : Α. Μουχτάρης. εύτερη Σειρά Ασκήσεων. Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 2015 ιδάσκων : Α. Μουχτάρης εύτερη Σειρά Ασκήσεων Λύσεις Ασκηση 1. 1. Consder the gven expresson for R 1/2 : R 1/2

Διαβάστε περισσότερα

α & β spatial orbitals in

α & β spatial orbitals in The atrx Hartree-Fock equatons The most common method of solvng the Hartree-Fock equatons f the spatal btals s to expand them n terms of known functons, { χ µ } µ= consder the spn-unrestrcted case. We

Διαβάστε περισσότερα

8.1 The Nature of Heteroskedasticity 8.2 Using the Least Squares Estimator 8.3 The Generalized Least Squares Estimator 8.

8.1 The Nature of Heteroskedasticity 8.2 Using the Least Squares Estimator 8.3 The Generalized Least Squares Estimator 8. 8.1 The Nature of Heteroskedastcty 8. Usng the Least Squares Estmator 8.3 The Generalzed Least Squares Estmator 8.4 Detectng Heteroskedastcty E( y) = β+β 1 x e = y E( y ) = y β β x 1 y = β+β x + e 1 Fgure

Διαβάστε περισσότερα

Multi-dimensional Central Limit Theorem

Multi-dimensional Central Limit Theorem Mult-dmensonal Central Lmt heorem Outlne () () () t as () + () + + () () () Consder a sequence of ndependent random proceses t, t, dentcal to some ( t). Assume t 0. Defne the sum process t t t t () t tme

Διαβάστε περισσότερα

Multi-dimensional Central Limit Theorem

Multi-dimensional Central Limit Theorem Mult-dmensonal Central Lmt heorem Outlne () () () t as () + () + + () () () Consder a sequence of ndependent random proceses t, t, dentcal to some ( t). Assume t 0. Defne the sum process t t t t () t ();

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

8. ΕΠΕΞΕΡΓΑΣΊΑ ΣΗΜΆΤΩΝ. ICA: συναρτήσεις κόστους & εφαρμογές

8. ΕΠΕΞΕΡΓΑΣΊΑ ΣΗΜΆΤΩΝ. ICA: συναρτήσεις κόστους & εφαρμογές 8. ΕΠΕΞΕΡΓΑΣΊΑ ΣΗΜΆΤΩΝ ICA: συναρτήσεις κόστους & εφαρμογές ΚΎΡΤΩΣΗ (KUROSIS) Αθροιστικό (cumulant) 4 ης τάξεως μίας τ.μ. x με μέσο όρο 0: kurt 4 [ x] = E[ x ] 3( E[ y ]) Υποθέτουμε διασπορά=: kurt[ x]

Διαβάστε περισσότερα

Exam Statistics 6 th September 2017 Solution

Exam Statistics 6 th September 2017 Solution Exam Statstcs 6 th September 17 Soluto Maura Mezzett Exercse 1 Let (X 1,..., X be a raom sample of... raom varables. Let f θ (x be the esty fucto. Let ˆθ be the MLE of θ, θ be the true parameter, L(θ be

Διαβάστε περισσότερα

Math221: HW# 1 solutions

Math221: HW# 1 solutions Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin

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

Variance of Trait in an Inbred Population. Variance of Trait in an Inbred Population

Variance of Trait in an Inbred Population. Variance of Trait in an Inbred Population Varance of Trat n an Inbred Populaton Varance of Trat n an Inbred Populaton Varance of Trat n an Inbred Populaton Revew of Mean Trat Value n Inbred Populatons We showed n the last lecture that for a populaton

Διαβάστε περισσότερα

Solution Series 9. i=1 x i and i=1 x i.

Solution Series 9. i=1 x i and i=1 x i. Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x

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

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

Numerical Analysis FMN011

Numerical Analysis FMN011 Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =

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

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

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

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

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

ΠΤΥΧΙΑΚΗ/ ΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ

ΠΤΥΧΙΑΚΗ/ ΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ ΑΡΙΣΤΟΤΕΛΕΙΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΘΕΣΣΑΛΟΝΙΚΗΣ ΣΧΟΛΗ ΘΕΤΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΤΜΗΜΑ ΠΛΗΡΟΦΟΡΙΚΗΣ ΠΤΥΧΙΑΚΗ/ ΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ «ΚΛΑ ΕΜΑ ΟΜΑ ΑΣ ΚΑΤΑ ΠΕΡΙΠΤΩΣΗ ΜΕΣΩ ΤΑΞΙΝΟΜΗΣΗΣ ΠΟΛΛΑΠΛΩΝ ΕΤΙΚΕΤΩΝ» (Instance-Based Ensemble

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

Estimators when the Correlation Coefficient. is Negative

Estimators when the Correlation Coefficient. is Negative It J Cotemp Math Sceces, Vol 5, 00, o 3, 45-50 Estmators whe the Correlato Coeffcet s Negatve Sad Al Al-Hadhram College of Appled Sceces, Nzwa, Oma abur97@ahoocouk Abstract Rato estmators for the mea of

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

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

ΗΥ537: Έλεγχος Πόρων και Επίδοση σε Ευρυζωνικά Δίκτυα,

ΗΥ537: Έλεγχος Πόρων και Επίδοση σε Ευρυζωνικά Δίκτυα, ΗΥ537: Έλεγχος Πόρων και Επίδοση σε Ευρυζωνικά Δίκτυα Βασίλειος Σύρης Τμήμα Επιστήμης Υπολογιστών Πανεπιστήμιο Κρήτης Εαρινό εξάμηνο 2008 Economcs Contents The contet The basc model user utlty, rces and

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

Symplecticity of the Störmer-Verlet algorithm for coupling between the shallow water equations and horizontal vehicle motion

Symplecticity of the Störmer-Verlet algorithm for coupling between the shallow water equations and horizontal vehicle motion Symplectcty of the Störmer-Verlet algorthm for couplng between the shallow water equatons and horzontal vehcle moton by H. Alem Ardakan & T. J. Brdges Department of Mathematcs, Unversty of Surrey, Guldford

Διαβάστε περισσότερα

MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)

MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3) 1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations

Διαβάστε περισσότερα

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων Εξάμηνο 7 ο Procedures and Functions Stored procedures and functions are named blocks of code that enable you to group and organize a series of SQL and PL/SQL

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

( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a)

( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a) hapter 5 xercise Problems X5. α β α 0.980 For α 0.980, β 49 0.980 0.995 For α 0.995, β 99 0.995 So 49 β 99 X5. O 00 O or n 3 O 40.5 β 0 X5.3 6.5 μ A 00 β ( 0)( 6.5 μa) 8 ma 5 ( 8)( 4 ) or.88 P on + 0.0065

Διαβάστε περισσότερα

Πρόβλημα 1: Αναζήτηση Ελάχιστης/Μέγιστης Τιμής

Πρόβλημα 1: Αναζήτηση Ελάχιστης/Μέγιστης Τιμής Πρόβλημα 1: Αναζήτηση Ελάχιστης/Μέγιστης Τιμής Να γραφεί πρόγραμμα το οποίο δέχεται ως είσοδο μια ακολουθία S από n (n 40) ακέραιους αριθμούς και επιστρέφει ως έξοδο δύο ακολουθίες από θετικούς ακέραιους

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

130907_A_fasi_PE70 ΑΑ ΕΠΩΝΥΜΟ ΟΝΟΜΑ ΠΑΤΡΩΝΥΜΟ ΜΗΤΡΩΝΥΜΟ ΚΛΑΔΟΣ ΤΡΙΤΕΚΝΟ ΠΙΝΑΚΑΣ Σ ΔΙΕΥΘΥΝΣΗ ΕΚΠ/ΣΗΣ ΠΙΝΑΚΑ ΠΙΝΑΚΑ ΤΟΠΟΘΕΤΗΣΗΣ

130907_A_fasi_PE70 ΑΑ ΕΠΩΝΥΜΟ ΟΝΟΜΑ ΠΑΤΡΩΝΥΜΟ ΜΗΤΡΩΝΥΜΟ ΚΛΑΔΟΣ ΤΡΙΤΕΚΝΟ ΠΙΝΑΚΑΣ Σ ΔΙΕΥΘΥΝΣΗ ΕΚΠ/ΣΗΣ ΠΙΝΑΚΑ ΠΙΝΑΚΑ ΤΟΠΟΘΕΤΗΣΗΣ ΑΑ ΕΠΩΝΥΜΟ ΟΝΟΜΑ ΠΑΤΡΩΝΥΜΟ ΜΗΤΡΩΝΥΜΟ ΚΛΑΔΟ ΤΡΙΤΕΚΝΟ ΕΙΡΑ ΜΟΡΙΑ ΠΕΡΙΟΧΗ ΠΙΝΑΚΑ ΠΙΝΑΚΑ ΠΙΝΑΚΑ ΤΟΠΟΘΕΤΗΗ ΔΙΕΥΘΥΝΗ ΕΚΠ/Η 1 ΜΙΧΟΥΔΗ ΔΗΜΗΤΡΙΟ ΙΩΑΝΝΗ ΔΕΠΟΙΝΑ ΠΕ70 ΟΧΙ Β 2 9,5 Ηράκλειο ΔΙΕΥΘΥΝΗ Π.Ε. ΗΡΑΚΛΕΙΟΥ

Διαβάστε περισσότερα

Exercises to Statistics of Material Fatigue No. 5

Exercises to Statistics of Material Fatigue No. 5 Prof. Dr. Christine Müller Dipl.-Math. Christoph Kustosz Eercises to Statistics of Material Fatigue No. 5 E. 9 (5 a Show, that a Fisher information matri for a two dimensional parameter θ (θ,θ 2 R 2, can

Διαβάστε περισσότερα

Vidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a

Vidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a Per -.(D).() Vdymndr lsses Solutons to evson est Seres - / EG / JEE - (Mthemtcs) Let nd re dmetrcl ends of crcle Let nd D re dmetrcl ends of crcle Hence mnmum dstnce s. y + 4 + 4 6 Let verte (h, k) then

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

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 11/3/2006

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 11/3/2006 ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 11/3/26 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα μικρότεροι το 1 εκτός αν ορίζεται διαφορετικά στη διατύπωση

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

8.324 Relativistic Quantum Field Theory II

8.324 Relativistic Quantum Field Theory II Lecture 8.3 Relatvstc Quantum Feld Theory II Fall 00 8.3 Relatvstc Quantum Feld Theory II MIT OpenCourseWare Lecture Notes Hon Lu, Fall 00 Lecture 5.: RENORMALIZATION GROUP FLOW Consder the bare acton

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

LECTURE 4 : ARMA PROCESSES

LECTURE 4 : ARMA PROCESSES LECTURE 4 : ARMA PROCESSES Movng-Average Processes The MA(q) process, s defned by (53) y(t) =µ ε(t)+µ 1 ε(t 1) + +µ q ε(t q) =µ(l)ε(t), where µ(l) =µ +µ 1 L+ +µ q L q and where ε(t) s whte nose An MA model

Διαβάστε περισσότερα

Solutions to Exercise Sheet 5

Solutions to Exercise Sheet 5 Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X

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

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

F19MC2 Solutions 9 Complex Analysis

F19MC2 Solutions 9 Complex Analysis F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at

Διαβάστε περισσότερα

ΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ

ΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ ΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ ΕΛΕΝΑ ΦΛΟΚΑ Επίκουρος Καθηγήτρια Τµήµα Φυσικής, Τοµέας Φυσικής Περιβάλλοντος- Μετεωρολογίας ΓΕΝΙΚΟΙ ΟΡΙΣΜΟΙ Πληθυσµός Σύνολο ατόµων ή αντικειµένων στα οποία αναφέρονται

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

arxiv: v1 [stat.me] 20 Jun 2015

arxiv: v1 [stat.me] 20 Jun 2015 Combnng cluster sampg and k-tracng sampg to estmate the sze of a hdden populaton: asymptotc propertes of the estmators arxv:56.69v stat.me 2 Jun 25 Martín H. Fél Medna Techncal report Number: FCFM-UAS-25-

Διαβάστε περισσότερα

ΑΠΟΤΕΛΕΣΜΑΤΑ ΕΞΕΤΑΣΕΩΝ ΣΕΜΙΝΑΡΙΟΥ ΠΙΣΤΟΠΟΙΗΣΗΣ ΤΥΠΟΣ ΠΙΣΤΟΠ.

ΑΠΟΤΕΛΕΣΜΑΤΑ ΕΞΕΤΑΣΕΩΝ ΣΕΜΙΝΑΡΙΟΥ ΠΙΣΤΟΠΟΙΗΣΗΣ ΤΥΠΟΣ ΠΙΣΤΟΠ. 1 ΛΥΣΣΑΝΔΡΗ ΣΟΦΙΑ ΧΑΜΠΗΣ Α1 108400011 ΑΠΟΤΥΧΩΝ/ΟΥΣΑ ΑΠΟΤΥΧΩΝ/ΟΥΣΑ _ 2 ΓΙΑΝΝΙΟΣ ΝΙΚΟΛΑΟΣ ΜΙΧΑΗΛ Α1 108400021 ΑΠΟΤΥΧΩΝ/ΟΥΣΑ ΕΠΙΤΥΧΩΝ/ΟΥΣΑ _ 3 ΤΣΙΜΠΛΑΚΟΥ ΕΛΕΝΗ ΠΑΝΑΓΙΩΤΗΣ Α1 108400031 ΕΠΙΤΥΧΩΝ/ΟΥΣΑ ΕΠΙΤΥΧΩΝ/ΟΥΣΑ

Διαβάστε περισσότερα

Overview. Transition Semantics. Configurations and the transition relation. Executions and computation

Overview. Transition Semantics. Configurations and the transition relation. Executions and computation Overview Transition Semantics Configurations and the transition relation Executions and computation Inference rules for small-step structural operational semantics for the simple imperative language Transition

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 24/3/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 24/3/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Όλοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα μικρότεροι του 10000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Αν κάπου κάνετε κάποιες υποθέσεις

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

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

Supporting information for: Functional Mixed Effects Model for Small Area Estimation

Supporting information for: Functional Mixed Effects Model for Small Area Estimation Supportng nformaton for: Functonal Mxed Effects Model for Small Area Estmaton Tapabrata Mat 1, Samran Snha 2 and Png-Shou Zhong 1 1 Department of Statstcs & Probablty, Mchgan State Unversty, East Lansng,

Διαβάστε περισσότερα

Calculating the propagation delay of coaxial cable

Calculating the propagation delay of coaxial cable Your source for quality GNSS Networking Solutions and Design Services! Page 1 of 5 Calculating the propagation delay of coaxial cable The delay of a cable or velocity factor is determined by the dielectric

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

1 Complete Set of Grassmann States

1 Complete Set of Grassmann States Physcs 610 Homework 8 Solutons 1 Complete Set of Grassmann States For Θ, Θ, Θ, Θ each ndependent n-member sets of Grassmann varables, and usng the summaton conventon ΘΘ Θ Θ Θ Θ, prove the dentty e ΘΘ dθ

Διαβάστε περισσότερα

THE SECOND WEIGHTED MOMENT OF ζ. S. Bettin & J.B. Conrey

THE SECOND WEIGHTED MOMENT OF ζ. S. Bettin & J.B. Conrey THE SECOND WEIGHTED MOMENT OF ζ by S. Bettn & J.B. Conrey Abstract. We gve an explct formula for the second weghted moment of ζs) on the crtcal lne talored for fast computatons wth any desred accuracy.

Διαβάστε περισσότερα

The ε-pseudospectrum of a Matrix

The ε-pseudospectrum of a Matrix The ε-pseudospectrum of a Matrix Feb 16, 2015 () The ε-pseudospectrum of a Matrix Feb 16, 2015 1 / 18 1 Preliminaries 2 Definitions 3 Basic Properties 4 Computation of Pseudospectrum of 2 2 5 Problems

Διαβάστε περισσότερα

Notes on the Open Economy

Notes on the Open Economy Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.

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

Suppose Mr. Bump observes the selling price and sales volume of milk gallons for 10 randomly selected weeks as follows

Suppose Mr. Bump observes the selling price and sales volume of milk gallons for 10 randomly selected weeks as follows Albert Ludwgs Unverst Freburg Department of Emprcal Research and Econometrcs Appled Econometrcs Dr Kestel ummer 9 EXAMPLE IMPLE LINEAR REGREION ANALYI uppose Mr Bump observes the sellng prce and sales

Διαβάστε περισσότερα

Generalized Linear Model [GLM]

Generalized Linear Model [GLM] Generalzed Lnear Model [GLM]. ก. ก Emal: nkom@kku.ac.th A Lttle Hstory Multple lnear regresson normal dstrbuton & dentty lnk (Legendre, Guass: early 19th century). ANOVA normal dstrbuton & dentty lnk (Fsher:

Διαβάστε περισσότερα

SUPPLEMENT TO SEQUENTIAL ESTIMATION OF STRUCTURAL MODELS WITH A FIXED POINT CONSTRAINT (Econometrica, Vol. 80, No. 5, September 2012, )

SUPPLEMENT TO SEQUENTIAL ESTIMATION OF STRUCTURAL MODELS WITH A FIXED POINT CONSTRAINT (Econometrica, Vol. 80, No. 5, September 2012, ) Econometrca Supplementary Materal SULEMENT TO SEQUENTIAL ESTIMATION OF STRUCTURAL MODELS WITH A FIXED OINT CONSTRAINT (Econometrca, Vol. 80, No. 5, September 2012, 2303 2319) BY HIROYUKI KASAHARA AND KATSUMI

Διαβάστε περισσότερα

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3

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

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

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

Supplementary materials for Statistical Estimation and Testing via the Sorted l 1 Norm

Supplementary materials for Statistical Estimation and Testing via the Sorted l 1 Norm Sulementary materals for Statstcal Estmaton and Testng va the Sorted l Norm Małgorzata Bogdan * Ewout van den Berg Weje Su Emmanuel J. Candès October 03 Abstract In ths note we gve a roof showng that even

Διαβάστε περισσότερα

A Two Sample Test for Mean Vectors with Unequal Covariance Matrices

A Two Sample Test for Mean Vectors with Unequal Covariance Matrices A Two Sample Test for Mean Vectors wth Unequal Covarance Matrces Tamae Kawasak 1 and Takash Seo 2 1 Department of Mathematcal Informaton Scence Graduate School of Scence, Tokyo Unversty of Scence, Tokyo,

Διαβάστε περισσότερα

arxiv: v1 [math.na] 16 Apr 2017

arxiv: v1 [math.na] 16 Apr 2017 Energy estmates for two-dmensonal space-resz fractonal wave equaton Mnghua Chen, Wenshan Yu arxv:17.716v1 math.na 16 Apr 17 School of Mathematcs and Statstcs, Gansu Key Laboratory of Appled Mathematcs

Διαβάστε περισσότερα

Variational Wavefunction for the Helium Atom

Variational Wavefunction for the Helium Atom Technische Universität Graz Institut für Festkörperphysik Student project Variational Wavefunction for the Helium Atom Molecular and Solid State Physics 53. submitted on: 3. November 9 by: Markus Krammer

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

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

Phasor Diagram of an RC Circuit V R

Phasor Diagram of an RC Circuit V R ESE Lecture 3 Phasor Dagram of an rcut VtV m snt V t V o t urrent s a reference n seres crcut KVL: V m V + V V ϕ I m V V m ESE Lecture 3 Phasor Dagram of an L rcut VtV m snt V t V t L V o t KVL: V m V

Διαβάστε περισσότερα

Dynamic types, Lambda calculus machines Section and Practice Problems Apr 21 22, 2016

Dynamic types, Lambda calculus machines Section and Practice Problems Apr 21 22, 2016 Harvard School of Engineering and Applied Sciences CS 152: Programming Languages Dynamic types, Lambda calculus machines Apr 21 22, 2016 1 Dynamic types and contracts (a) To make sure you understand the

Διαβάστε περισσότερα

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1)

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1) HW 3 Solutions a) I use the autoarima R function to search over models using AIC and decide on an ARMA3,) b) I compare the ARMA3,) to ARMA,0) ARMA3,) does better in all three criteria c) The plot of the

Διαβάστε περισσότερα

m4.3 Chris Parrish June 16, 2016

m4.3 Chris Parrish June 16, 2016 m4.3 Chris Parrish June 16, 2016 Contents!Kung model 1 data..................................................... 1 scatterplot with ggplot2....................................... 2 model....................................................

Διαβάστε περισσότερα

Srednicki Chapter 55

Srednicki Chapter 55 Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third

Διαβάστε περισσότερα

An Inventory of Continuous Distributions

An Inventory of Continuous Distributions Appendi A An Inventory of Continuous Distributions A.1 Introduction The incomplete gamma function is given by Also, define Γ(α; ) = 1 with = G(α; ) = Z 0 Z 0 Z t α 1 e t dt, α > 0, >0 t α 1 e t dt, α >

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

Αναγνώριση Προτύπων (Pattern Recognition) Μπεϋζιανή Θεωρία Αποφάσεων (Bayesian Decision Theory) Π. Τσακαλίδης

Αναγνώριση Προτύπων (Pattern Recognition) Μπεϋζιανή Θεωρία Αποφάσεων (Bayesian Decision Theory) Π. Τσακαλίδης Αναγνώριση Προτύπων (Pattern Recognton Μπεϋζιανή Θεωρία Αποφάσεων (Bayesan Decson Theory Π. Τσακαλίδης ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ ΤΜΗΜΑ ΕΠΙΣΤΗΜΗΣ ΥΠΟΛΟΓΙΣΤΩΝ Μπεϋζιανή Θεωρία Αποφάσεων (Bayes Decson theory Στατιστικά

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

1η εργασία για το μάθημα «Αναγνώριση προτύπων»

1η εργασία για το μάθημα «Αναγνώριση προτύπων» 1η εργασία για το μάθημα «Αναγνώριση προτύπων» Σημειώσεις: 1. Η παρούσα εργασία είναι η πρώτη από 2 συνολικά εργασίες, η κάθε μια από τις οποίες θα βαθμολογηθεί με 0.4 μονάδες του τελικού βαθμού του μαθήματος.

Διαβάστε περισσότερα

ΜΕΡΟΣ ΙΙI ΜΟΡΙΑΚΟ ΒΑΡΟΣ ΠΟΛΥΜΕΡΩΝ

ΜΕΡΟΣ ΙΙI ΜΟΡΙΑΚΟ ΒΑΡΟΣ ΠΟΛΥΜΕΡΩΝ ΜΕΡΟΣ ΙΙI ΜΟΡΙΑΚΟ ΒΑΡΟΣ ΠΟΛΥΜΕΡΩΝ ΓΕΝΙΚΕΣ ΠΑΡΑΤΗΡΗΣΕΙΣ ΕΠΙ ΡΑΣΗ Μ.Β ΣΤΙΣ Ι ΙΟΤΗΤΕΣ ΠΟΛΥΜΕΡΩΝ ΜΑΘΗΜΑΤΙΚΗ ΠΕΡΙΓΡΑΦΗ ΤΗΣ ΚΑΤΑΝΟΜΗΣ ΜΟΡΙΑΚΟΥ ΒΑΡΟΥΣ ΣΥΝΑΡΤΗΣΗ ΠΙΘΑΝΟΤΗΤΟΣ ( ΙΑΦΟΡΙΚΗ) Probablty Densty Functon

Διαβάστε περισσότερα

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Harvard College Statistics 104: Quantitative Methods for Economics Formula and Theorem Review Tommy MacWilliam, 13 tmacwilliam@college.harvard.edu March 10, 2011 Contents 1 Introduction to Data 5 1.1 Sample

Διαβάστε περισσότερα

Μαθητές που εισήχθησαν στην Τριτοβάθμια Εκπαίδευση με τις Πανελλαδικές Εξετάσεις 2013. Όνομα Πατέρα. Μητέρας

Μαθητές που εισήχθησαν στην Τριτοβάθμια Εκπαίδευση με τις Πανελλαδικές Εξετάσεις 2013. Όνομα Πατέρα. Μητέρας Μαθητές που εισήχθησαν στην Τριτοβάθμια Εκπαίδευση με τις Πανελλαδικές Εξετάσεις 2013 α/α Επώνυμο Όνομα Όνομα Πατέρα Όνομα Μητέρας Σχολή Επιτυχίας 1 ΑΔΑΜΟΥ ΚΑΛΛΙΟΠΗ ΓΕΩΡΓΙΟΣ ΦΙΛΟΣΟΦΙΚΗ 2 ΛΛΕΣΙ ΝΤΕΝΙΣ ΑΓΚΡΟΝ

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

ΠΡΟΓΡΑΜΜΑ ΣΠΟΥΔΩΝ: "ΤΡΑΠΕΖΙΚΗ" ( ΤΡΑ ) ΚΑΤΗΓΟΡΙΑ Α' Α/Α EΠΩΝΥΜΟ ΟΝΟΜΑ ΟΝΟΜΑ ΠΑΤΕΡΑ ΣΕΙΡΑ ΕΠΙΤΥΧΙΑΣ

ΠΡΟΓΡΑΜΜΑ ΣΠΟΥΔΩΝ: ΤΡΑΠΕΖΙΚΗ ( ΤΡΑ ) ΚΑΤΗΓΟΡΙΑ Α' Α/Α EΠΩΝΥΜΟ ΟΝΟΜΑ ΟΝΟΜΑ ΠΑΤΕΡΑ ΣΕΙΡΑ ΕΠΙΤΥΧΙΑΣ ΠΡΟΓΡΑΜΜΑ ΣΠΟΥΔΩΝ: "ΤΡΑΠΕΖΙΚΗ" ( ΤΡΑ ) ΚΑΤΗΓΟΡΙΑ Α' Α/Α EΠΩΝΥΜΟ ΟΝΟΜΑ ΟΝΟΜΑ ΠΑΤΕΡΑ ΣΕΙΡΑ ΕΠΙΤΥΧΙΑΣ 1 ΠΑΡΑΣΚΕΥΟΠΟΥΛΟΥ ΣΤΥΛΙΑΝΗ ΣΩΤΗΡΙΟΣ 1 2 ΠΛΑΣΤΗΡΑΣ ΝΙΚΟΛΑΟΣ ΒΑΣΙΛΕΙΟΣ 3 3 GJINI VILMA ΧΡΟΝΗΣ 5 4 ΣΟΥΝΙΤΗ

Διαβάστε περισσότερα

Differential equations

Differential equations Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential

Διαβάστε περισσότερα

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0. DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec

Διαβάστε περισσότερα

Mean-Variance Analysis

Mean-Variance Analysis Mean-Variance Analysis Jan Schneider McCombs School of Business University of Texas at Austin Jan Schneider Mean-Variance Analysis Beta Representation of the Risk Premium risk premium E t [Rt t+τ ] R1

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

ΤΜΗΜΑ ΛΟΓΙΣΤΙΚΗΣ & ΧΡΗΜΑΤΟΟΙΚΟΝΟΜΙΚΗΣ

ΤΜΗΜΑ ΛΟΓΙΣΤΙΚΗΣ & ΧΡΗΜΑΤΟΟΙΚΟΝΟΜΙΚΗΣ ΤΕΧΝΟΛΟΓΙΚΟ ΕΚΠΑΙΔΕΥΤΙΚΟ ΙΔΡΥΜΑ ΠΕΛΟΠΟΝΝΗΣΟΥ ΣΧΟΛΗ ΔΙΟΙΚΗΣΗΣ & ΟΙΚΟΝΟΜΙΑΣ ΤΜΗΜΑ ΛΟΓΙΣΤΙΚΗΣ & ΧΡΗΜΑΤΟΟΙΚΟΝΟΜΙΚΗΣ ΠΤΥΧΙΑΚΗ ΕΡΓΑΣΙΑ ΟΙ ΦΟΡΟΛΟΓΙΚΕΣ ΥΠΟΧΡΕΩΣΕΙΣ ΤΩΝ ΞΕΝΟΔΟΧΕΙΑΚΩΝ ΑΝΩΝΥΜΩΝ ΕΠΙΧΕΙΡΗΣΕΩΝ ΠΑΝΑΓΙΩΤΗΣ

Διαβάστε περισσότερα

Neutralino contributions to Dark Matter, LHC and future Linear Collider searches

Neutralino contributions to Dark Matter, LHC and future Linear Collider searches Neutralno contrbutons to Dark Matter, LHC and future Lnear Collder searches G.J. Gounars Unversty of Thessalonk, Collaboraton wth J. Layssac, P.I. Porfyrads, F.M. Renard and wth Th. Dakonds for the γz

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

Testing for Indeterminacy: An Application to U.S. Monetary Policy. Technical Appendix

Testing for Indeterminacy: An Application to U.S. Monetary Policy. Technical Appendix Testing for Indeterminacy: An Application to U.S. Monetary Policy Technical Appendix Thomas A. Lubik Department of Economics Johns Hopkins University Frank Schorfheide Department of Economics University

Διαβάστε περισσότερα