Proof of Lemmas Lemma 1 Consider ξ nt = r

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Proof of Lemmas Lemma 1 Consider ξ nt = r"

Transcript

1 Supplemetary Material to "GMM Estimatio of Spatial Pael Data Models with Commo Factors ad Geeral Space-Time Filter" (Not for publicatio) Wei Wag & Lug-fei Lee April 207 Proof of Lemmas Lemma Cosider = r l= C,lV l + D e, where C,l s are matrices ad D is a square matrix of dimesio. Let E[V l,i V k,i ] = σ lk, E[V l,i V k,i V s,i ] = µ 3,lks, E[V l,i V k,i V s,i V w,i ] = µ 4,lksw, for l, k, s, w =,..., r, ad E[e 3,i ] = µ 3e, E[e 4,i ] = µ 4e. For ay -dimesioal square matrix A, let vec D (A) = (a,,...a, ) deote the colum vector formed with the diagoal elemets of A, The, for ay two square matrices A ad B of dimesio, ad r r r E( A ) = C,l vec D (C,kA C,s )µ 3,lks + D vec D (D A D )µ 3e l= k= s= = E( A B ) r r r r [(µ 4,lksw σ lk σ sw σ ls σ kw σ lw σ ks )vec D(C,lA C,k )vec D (C,sB C,w ) l= k= s= w= +σ 2 e0 l= +σ ls σ kw tr(c,la C,k C,sB C,w ) + σ lw σ ks tr(c,la C,k C,wB C,s ) +σ lk σ sw tr(c,la C,k )tr(c,sb C,w )] r [tr(c,la C,l )tr(d B D ) + tr(c,lb C,l )tr(d A D ) +tr(c,l C,lA D D B s ) + tr(d D A C,l C,lB s )] +(µ 4e 3σ 4 e0)vec D(D A D )vec D (D B D ) +σ 4 e0[tr(d A D D B s D ) + tr(d A D )tr(d B D )]. Proof: Note that V l s are ucorrelated with oe aother, ad are all idepedet of e. The the result is straightforward from expasios of A ad A B ad Lemma A.2 i Lee (2007). Q.E.D. Lemma 2 Uder Assumptios F, F2,, 3 ad 4, for ay ostochastic UB matrix A, (i) E( A ) = O(); (ii) V ar( A ) = O(); (iii) A = O p () ad A E( A ) = o p (); (iv) for the IV matrix Q, plim Q A = 0. Proof: (i) E( A ) = tr(a Σ ) = r l= tr[a ((f l (α 0 )f l (α 0)) I )]+σ 2 e0tr[a (J K J )], where (f l (α 0 )f l (α 0)) I ad (J K J ) are UB uder Assumptios F, F2, 3 ad 4. Thus E( A ) = O() by Lemma A.3 i Lee (2007).

2 (ii) From Lemma, V ar( A ) = E( A A ) E( A )E( A ) r r r r = {(µ 4,lksw σ lk σ sw σ ls σ kw σ lw σ ks ) l= k= s= w= vec D[(f l (α 0 ) I )A (f k (α 0 ) I )]vec D [(f s(α 0 ) I )A (f w (α 0 ) I )] + +σ ls σ kw tr[a (f l (α 0 )f k0(α 0 ) I )A (f s (α 0 )f w(α 0 ) I )] +σ lw σ ks tr[a (f l (α 0 )f k0(α 0 ) I )A (f w (α 0 )f s(α 0 ) I )]} r σ 2 e0tr[(f l (α 0 )f l (α 0 ) I )A (J K J )As l= +(J K J )A ((f l (α 0 )f l (α 0 ) I )A s ] +(µ 4e 3σ 4 e0)vec D[P J A J P ]vec D [P J A J P ] +σ 4 e0tr[a (J K J )As (J K J )], As J P, (f l (α 0 )f l (α 0)) I, for l =,..., r, ad J K J are UB uder Assumptios F, F2, 3 ad 4, V ar( A ) = O() follows from Lemma A.3 i Lee (2007). (iii) These immediately follow from (i) ad (ii). (iv) As = r l= f l(α 0 ) V l + (J P )e, we have Q A = Q A r l= [f l(α 0 ) I ]V l + Q A (J P )e. Uder Assumptios F, 3 ad 4, elemets of Q A [f l (α 0 ) I ] are bouded ad J P is UB. Therefore, by Assumptio 4, a law of large umbers ca apply to each row of Q A [f l (α 0 ) I ]V l s ad Q A (J P )e, which i tur, implies that plim Q A = 0. Q.E.D. Lemma 3 (CLT for a geeralized liear-quadratic form) Suppose that, for l, k =,..., m, {A,lk } is a sequece of symmetric ostochastic UB matrices ad B,l = (b,l,...b,l, ) is a -dimesioal vector such that sup (/) i= b i,l 2+η < for some η > 0. Let σ 2 Q be the variace of Q where Q = m m l= k= V,l A,lkV,k + m l= B,l V,l, ad V,l s are ucorrelated radom vectors whose elemets v i,l s are i.i.d. with zero mea ad fiite variace σ 2 l, ad E( v i,l 4+δ0 ) ad E( v i,l v i,k 2+δ0 ) for some δ 0 > 0 exist ad are uiformly bouded for all i, l ad k. Assume that the variace σ 2 Q is bouded away from zero at the rate. The (Q E(Q ))/σ 2 D Q N(0, ). Mai steps of the proof: Defie σ-fields F i, =< v,,..., v i,, v,2,..., v i,2,..., v,m,...v i,m > geerated by v,,..., v i,, v,2,..., v i,2,..., v,m,...v i,m. Because (v i,,..., v i,m ) for all i of V,l s are mutually idepedet, it is easily see that E(Z i, F i, ) = 0. Thus {(Z i,, F i, ) i } forms a martigale differece double array. Therefore, σ 2 Q = i= E(Z2 i, ). Defie ormalized variables Zi, = Z i,/σ Q. The {(Zi,, F i,) i } is a martigale differece double array ad (Q E(Q ))/σ 2 Q = i= Z i,. I order for the martigale cetral limit theorem to be applicable, we ca establish the followig two steps: Step. There exists δ > 0 such that i= E( Z i, 2+δ ) teds to approach zero as goes to ifiity. Step 2. i= E(Z 2 i, F i,) p. The detailed proof is available upo request, which is a rather log ad mechaical extesio of Kelejia ad Prucha (200) ad Qu ad Lee (202). Q.E.D. Lemma 4 Suppose that A (α 0 ) is a matrix, where α 0 is a parameter vector of fiite dimesio. Let α be ay possible value of α 0, ad α i is the i-th elemet of α, assume that {A (α)} ad 2

3 { A (α)/ α i } are UB uiformly i α. If α is a cosistet estimator of α 0, the uder Assumptio 4, (i) [tr(a ( α)) tr(a (α 0 ))] = o p (), ad (ii) A ( α) A (α 0 ) = o p (). Proof: (i) By Taylor s expasio, [tr(a ( α)) tr(a (α 0 ))] = [ tr(a (α))/ α)]( α α 0 ), where α is a value betwee α ad α 0. As { A (α)/ α i } is UB uiformly i α, { A (α)/ α i } is UB. By Lemma A.3 i Lee (2007), tr( A (α)/ α i ) = O(). So tr(a (α))/ α i = tr( A (α)/ α i ) = O(). Because α α 0 = o p (), it follows that [ tr(a (α))/ α)]( α α 0 ) = o p (). (ii) Let e i be the idicator vector with the i-th elemet beig oe ad all other elemets beig zero. The A ( α) A (α 0 ) = max i j= e i [A ( α) A (α 0 )]e j. By the mea value theorem, e i [A ( α) A (α 0 )]e j = e i [ r k= max i ( ) A (α ij) α k A (α ij) α k ( α k α k0 )]e j, where α ij is a value betwee α ad α 0. Thus r A (α ij ) A ( α) A (α 0 ) = max i e i[ ( α k α k0 )]e j α j= k k= r ( ) A (α ij ) ( ) α k α k0 α k rc A (α ij ) α max i α k, j= k= where is the ij-th elemet of A (α ij) α ij k ad c α = max k { α k α k0 }. Because { A (α)/ α k } ( is UB uiformly i α, { A (α ij )/ α k } is UB so that max i A (α ij) j= α k is bouded. As α )ij ( α 0 = o p (), c α = o p (). Notig that r is fiite, rc α max i A (α ij) j= α k )ij = o p(). Therefore, A ( α) A (α 0 ) = o p (). Q.E.D. Lemma 5 Let θ ad θ be, respectively, the miimizers of F (θ) ad F (θ) i Θ. Suppose that (F (θ) F (θ)) coverges i probability to zero uiformly i θ Θ, where θ 0 is i the iterior of Θ, ad { F (θ)} satisfies the uiqueess idetificatio coditio at θ 0. If (F (θ) F (θ)) = o p () uiformly i θ Θ, the both θ ad θ coverge i probability to θ 0. I additio, suppose that 2 F (θ) ij coverges i probability to a well-defied limitig matrix, uiformly i θ Θ, which is osigular at θ 0, ad F (θ 0) = O p (). If F (θ 0) ( 2 F (θ) j= 2 F (θ) ) = o p () uiformly i θ Θ ad ( F (θ0) ) = o p (), the ( θ N θ 0 ) ad ( θ N θ 0 ) have the same limitig distributio. Proof: This is Lemma A.6 i Lee (2007), otig that T is fiite here. Q.E.D. Lemma 6 Suppose that z, ad z 2, are -dimesioal colum vectors of costats of which their elemets are uiformly bouded, the costat matrix A is uiformly bouded i colum sums i absolute value, ad the costat matrices B, ad B 2, are UB. Let θ be a -cosistet estimate of θ 0. Let C be either Σ, Σ (I T G j )Z π 0 or Σ (δ 0)/ δ l, where δ l is the l-th elemet of δ. Let Ĉ be the estimated couterparts of C. For these C matrices, C L represets its liear trasformed matrix that preserves UB property. The, uder Assumptios F, F2,, 3, 4 ad 6, (i) z, (Ĉ C )L z 2, = o p (); (ii) z, (Ĉ C )L A = o p (); (iii) B, (Ĉ C )L B 2, = o p (); (iv) (Ĉ C ) = o p (). Proof: Uder Assumptios F, F2,, 3, 4 ad 6, these results ca be obtaied from Lemmas 4 (ii) ad 8. Q.E.D. Lemma 7 Suppose that { W j } for j =,..., p ad { S }, where is a matrix orm, are bouded. The { S (λ) } is uiformly bouded i a eighborhood of λ0. 3 ij

4 Proof: This is Lemma C8 i Lee ad Liu (200). Q.E.D. Lemma 8 Uder Assumptios F, F2,, 3, 4 ad 6, {Σ (δ)}, { Σ (δ)/ δ l }, { Σ (δ)/ δ l}, ad { 2 Σ (δ)/ δ2 l } are UB uiformly i δ, where δ l is the l-th elemet of δ. Proof: The UB of {Σ (δ)} ad { Σ (δ)/ δ l } are directly from their expressios ad Assumptios F, F2,, 3, ad 4. As Σ (δ)/ δ l = Σ (δ) Σ (δ) δ l Σ (δ), from the expressio of Σ (δ)/ δ l ad Assumptios F, F2,, 3, 4 ad 6, its UB follows. Similarly, the UB of { 2 Σ (δ)/ δ2 l } ca be derived from its expressio ad the assumptios metioed above. Q.E.D. Proofs of Propositios 4 ad 5 Proof of Propositio 4: We shall show that F (θ) = ĝ (θ) Ω ĝ (θ) ad F (θ) = g (θ)ω will satisfy the coditios i Lemma 5. If so, the GMM estimator from the miimizatio of F (θ) will have the same limitig distributio as that of the miimizer of F (θ). The differece of F (θ) ad F (θ) ad its derivatives ivolve the differece of ĝ (θ) ad g (θ) ad their derivatives. Furthermore, oe has to cosider the differece of Ω ad Ω. First, cosider N (ĝ N (θ) g N (θ)). Let m = p + h + 2q + 2. Explicitly, (ĝ (θ) g (θ)) = { (ϑ)( Q Q ), [ (ϑ)( P, P, ) (ϑ) tr(( P, P, )Σ (δ))],..., [ (ϑ)( P m, P m, ) (ϑ) tr(( P m, P m, )Σ (δ))]}. g (θ) The (ϑ) is related to as (ϑ) = d (ϑ) + [I T S (λ)s ], where d (ϑ) = Z (π 0 π) + p j= (λ j0 λ j )(I T G j )Z π 0. To prove (ϑ)( Q Q ) = o p() uiformly i θ Θ, we eed to cosider each compoet i Q Q ad its product with (ϑ), otig that Q = Σ [Z, (I T G )Z π 0,..., (I T G p )Z π 0 ]. For j =,..., p, (ϑ)[ Σ (I T Ĝj)Z π Σ (I T G j )Z π 0 ] = (ϑ)[ Σ (I T Ĝj) Σ (I T G j )]Z π + (ϑ)σ (I T G j )Z ( π π 0 ) = [Z (π 0 π) + (λ j0 λ j )(I T G j )Z π 0 ] [ Σ (I T Ĝj) Σ (I T G j )]Z π j= + [I T S (λ)s ] [ Σ (I T Ĝj) Σ (I T G j )]Z π + [Z (π 0 π) + (λ j0 λ j )(I T G j )Z π 0 ] Σ (I T G j )Z ( π π 0 ) j= + [I T S (λ)s ] Σ (I T G j )Z ( π π 0 ). () The last three terms o the right had side of () are o p () uiformly i θ Θ by Assumptios 2-4 ad 4

5 Lemma 2 (iv) because θ p θ0. Note that S ( λ ) S = S ( λ )[S S ( λ )]S = ( λ ) ( λ j, λ j0 )W j S S ( λ ) S j= λ j, λ j0 Wj S = o p (), j= by Assumptio 3 ad Lemma 7 because λ p λ0, ad therefore, (I T Ĝj) (I T G j ) = I T (Ĝj G j ) = Ĝj G j (2) = W j S ( λ ) W j S S W j ( λ ) S = o p (). Moreover, by Lemmas 4 (ii) ad 8, Σ Σ = o p (). Thus, Σ (I T Ĝj) Σ (I T G j ) (3) = Σ [(I T Ĝj) (I T G j )] + ( Σ Σ )(I T G j ) Σ (I T Ĝj) (I T G j ) + Σ I T G j = o p (), which i tur implies that [Z (π 0 π) + Σ (λ j0 λ j )(I T G j )Z π 0 ] [ Σ (I T Ĝj) Σ (I T G j )]Z π = o p (). j= Therefore, (ϑ)[ Σ (I T Ĝj)Z π Σ (I T G j )Z π 0 ] = o p () for j =,..., p. Ad (ϑ)( Σ Z Σ Z ) = (ϑ)( Σ Σ )Z = o p () also follows from the above results. Thus, we coclude that (ϑ)( Q Q ) = o p() uiformly i θ Θ. Similarly, by expadig (ϑ) = d (ϑ) + [I T S (λ)s ], we have for l =,..., m, [ (ϑ)( P l, P l, ) (ϑ) tr(( P l, P l, )Σ (δ))] (4) = [ [I T S (λ)s ] ( P l, Pl, )[I T S (λ)s ] tr(( P l, Pl, )Σ (δ))] + 2 [ [I T S (λ)s ] ( P l, Pl, )[Z (π 0 π) + (λ j0 λ j )(I T G j )Z π 0 ] + [Z (π 0 π) + [Z (π 0 π) + j= (λ j0 λ j )(I T G j )Z π 0 ] ( P l, Pl, ) j= (λ j0 λ j )(I T G j )Z π 0 ]. j= The secod term o the right had side of (4) is o p () uiformly i θ Θ by Assumptios F, F2, ad -4 ad Lemma 2 (iv). Notig that Pl, Σ is δ l, Lemmas 4 (ii) ad 8 lead to the result that P l, P l, = 5

6 o p (). So the first ad last terms o the right had side of (4) are also o p () uiformly i θ Θ by Assumptios F, F2, ad -4. Therefore, [ (ϑ)( P l, P l, ) (ϑ) tr(( P l, P l, )Σ (δ))] = o p () uiformly i θ Θ for l =,..., m. We coclude that (ĝ (θ) g (θ)) = o p() uiformly i θ Θ. Cosider ext the derivatives of ĝ (θ) ad g (θ). We have ad, for j =,..., k, 2 g (θ) j = g (θ) = (ϑ)p s, Q (ϑ) (ϑ)pm s (ϑ), (ϑ) tr(p s, Σ (δ))/. tr(pm s, Σ (δ))/ Q 2 (ϑ) j (ϑ) j P, s (ϑ) + (ϑ)p,. 2 (ϑ) j (ϑ) j Pm s (ϑ), + (ϑ)pm 2 (ϑ), j where θ j is the j-th elemet of θ. The first order derivatives of (ϑ) are, 2 tr(p s, Σ (δ)) j 2 tr(p s m, Σ (δ)) j (ϑ) = [Z, (I T W )]Y,..., (I T W p )]Y, 0,..., 0], where Y = (I T S )Z π 0 + (I T S ). The secod order derivatives of (ϑ) are 2 (ϑ) λ π = 0, 2 (ϑ) δ l = 0, where δ l is the l-th elemet of δ. It follows from Lemmas 4 ad 6 that ( ĝ (θ) g (θ) ) = o p () ad ( 2 ĝ (θ) j 2 g (θ) j ) = o p () for j =,..., k, uiformly i θ Θ. with Cosider ( Ω Ω ), where m m = Ω N = ( Q Σ ) Q 0 0, m m tr(p, Σ P, s Σ N) tr(p, Σ Pm s, Σ )..... tr(p m, Σ P s, Σ ) tr(p m, Σ P s m, Σ ) Cosider the block matrix m m. That tr( P i, Σ s P Σ j, ) tr(p i, Σ Pj, s Σ ) = o p () for i, j =,..., m follows from Lemma 4. Next, cosider the block Q Σ Q. Lemma 6 implies that Therefore, ( Q Σ Q Q Σ Q ) = [ Q Σ ( Q Q ) + ( Q Q ) Σ Q ] = o p (). ( Q Σ Q Q Σ Q ) = ( Q Σ Q Q Σ Q ) + (Q Σ Q Q Σ Q ) = Q ( Σ Σ )Q + o p () = o p (),., 6

7 by Lemmas 4 ad 8. I coclusio, ( Ω Ω ) = o p(). As the limit of Ω exists ad is a osigular matrix, it follows that ( Ω ) ( Ω ) = o p () by the cotiuous mappig theorem. Furthermore, because (ĝ (θ) g (θ)) = o p(), ad [g (θ) E(g (θ)] = o p() uiformly i θ Θ, ad sup θ Θ E(g (θ) = O() (see the proof of Propositio 2), hece g (θ) ad ĝ (θ) are O p(), g uiformly i θ Θ. Similarly, (θ) ĝ, (θ), 2 g (θ) j ad 2 ĝ (θ) j for j =,..., k, are O p (), uiformly i θ Θ. With the uiform covergece i probability ad uiformly stochastic boudedess properties, the differece of F (θ) ad F (θ) ca be ivestigated. By expasio, (F (θ) F (θ)) = ĝ (θ) Ω (ĝ (θ) g (θ)) + g (θ)( Ω Ω )ĝ (θ) + g (θ)ω (ĝ (θ) g (θ)) = o p (), uiformly i θ Θ. Similarly, for each compoet θ j of θ, F ( 2 (θ) j 2 F (θ) j ) = 2 [ ĝ (θ) j Fially, because ( ĝ limit theorem i Lemma 3, (θ0) ( F (θ 0) (θ 0) = 2{ ĝ = 2 ĝ (θ 0) Ω g (θ0) ĝ Ω (θ) + ĝ ( g (θ) Ω g (θ) j + g = o p (), (θ) Ω (θ)ω 2 ĝ (θ) j 2 g (θ) j )] Ω ) = o p() as above, ad g (θ 0) = O p () by the cetral F (θ 0 ) ) Ω [ĝ (θ 0 ) g (θ 0 )] + [ ĝ (θ 0) ( Ω ) [ĝ (θ 0 ) g (θ 0 )] + o p (). Ω g (θ 0) Ω ] gn(θ 0 )} As [ĝ (θ 0) g (θ 0)] = o p () by Lemma 6, ( F (θ0) F (θ 0) ) = o p (). The desired result follows from Lemma 5. Q.E.D. Proof of Propositio 5: The ML estimator θ ml is characterized by the equatios (2)-(4) i the mai text, which are Z Σ (δ) (ϑ) = 0, (δ)(i T W j S (λ))z π] (ϑ)+ (ϑ)σ (δ)(i T W j S (λ)) (ϑ) tr[σ (δ)(i T W j S (λ))σ (δ)] = 0, [Σ ad (ϑ) Σ (δ) δ (ϑ) tr[ Σ (δ) Σ (δ)] = 0. l δ l 7

8 for j =,..., p ad l =,..., h + 2q + 2. Obviously, θ ml is the solutio of a ĝ ml, (θ) = 0, with a = I k x+t (k x+k z) I p I p 0, I h+2q+2 ad ĝ ml, (θ) = { (ϑ)σ ( δ ml )[Z, (I T W S ( λ ml ))Z π ml,..., (I T W p S ( λ ml ))Z π ml ], (ϑ)σ ( δ ml )(I T W S ( λ ml )) (ϑ) tr[σ ( δ ml )(I T W S ( λ ml ))Σ (δ)],..., (ϑ)σ ( δ ml )(I T W p S ( λ ml )) (ϑ) tr[σ ( δ ml )(I T W p S ( λ ml ))Σ (δ)], (ϑ) Σ ( δ ml ) α (ϑ) tr[ Σ ( δ ml ) Σ (δ)],..., (ϑ) Σ ( δ ml ) α α (ϑ) tr[ Σ ( δ ml ) Σ (δ)], h α h (ϑ) Σ ( δ ml ) γ (ϑ) tr[ Σ ( δ ml ) Σ (δ)],..., (ϑ) Σ ( δ ml ) γ γ (ϑ) tr[ Σ ( δ ml ) Σ (δ)], q γ q (ϑ) Σ ( δ ml ) η (ϑ) tr[ Σ ( δ ml ) Σ (δ)],..., (ϑ) Σ ( δ ml ) η η (ϑ) tr[ Σ ( δ ml ) Σ (δ)], q η q (ϑ) Σ ( δ ml ) ρ (ϑ) tr[ Σ ( δ ml ) Σ (δ)], (ϑ) Σ ( δ ml ) ρ (ϑ) tr[ Σ ( δ ml ) Σ (δ)]}. Ad it follows by similar argumets as i the proof of Propositio 4 that a ĝ ml, (θ) = 0 is asymptotically equivalet to a g ml, (θ) = 0 i the sese that their cosistet roots have the same limitig distributio, where g ml, (θ) = { (ϑ)σ [Z, (I T W S )Z π 0,..., (I T W p S )Z π 0 ], (ϑ)σ (I T W S ) (ϑ) tr[σ (I T W S )Σ (δ)],..., (ϑ)σ (I T W p S ) (ϑ) tr[σ (I T W p S )Σ (δ)], (ϑ) Σ α (ϑ) Σ γ (ϑ) Σ η (ϑ) Σ ρ (ϑ) tr[ Σ α (ϑ) tr[ Σ γ (ϑ) tr[ Σ η (ϑ) tr[ Σ ρ σ 2 e Σ (δ)],..., (ϑ) Σ Σ (δ)],..., (ϑ) Σ γ q Σ (δ)],..., (ϑ) Σ η q Σ (δ)], (ϑ) Σ σ 2 e σ 2 e α (ϑ) tr[ Σ Σ (δ)], h α h (ϑ) tr[ Σ Σ (δ)], γ q (ϑ) tr[ Σ Σ (δ)], η q (ϑ) tr[ Σ σ 2 Σ (δ)]}, e The vector of empirical momets g ml, (θ) cosists of liear ad quadratic fuctios of (ϑ), hece the correspodig optimal GMM estimator derived from mi g ml, (θ)ω g ml, (θ) is i the class of M. As the BGMM estimator is the most effi ciet estimator i M, the BGMM estimator is effi ciet relative to the ML estimator. O the other had, the ML estimator attais the lower boud of Fisher Iformatio uder ormality, it is the most asymptotic effi ciet estimator. Hece, we coclude that the BGMM estimator is asymptotically effi ciet as the ML estimator uder ormality. Q.E.D. 8

Homework for 1/27 Due 2/5

Homework for 1/27 Due 2/5 Name: ID: Homework for /7 Due /5. [ 8-3] I Example D of Sectio 8.4, the pdf of the populatio distributio is + αx x f(x α) =, α, otherwise ad the method of momets estimate was foud to be ˆα = 3X (where

Διαβάστε περισσότερα

Lecture 17: Minimum Variance Unbiased (MVUB) Estimators

Lecture 17: Minimum Variance Unbiased (MVUB) Estimators ECE 830 Fall 2011 Statistical Sigal Processig istructor: R. Nowak, scribe: Iseok Heo Lecture 17: Miimum Variace Ubiased (MVUB Estimators Ultimately, we would like to be able to argue that a give estimator

Διαβάστε περισσότερα

Ψηφιακή Επεξεργασία Εικόνας

Ψηφιακή Επεξεργασία Εικόνας ΠΑΝΕΠΙΣΤΗΜΙΟ ΙΩΑΝΝΙΝΩΝ ΑΝΟΙΚΤΑ ΑΚΑΔΗΜΑΪΚΑ ΜΑΘΗΜΑΤΑ Ψηφιακή Επεξεργασία Εικόνας Φιλτράρισμα στο πεδίο των συχνοτήτων Διδάσκων : Αναπληρωτής Καθηγητής Νίκου Χριστόφορος Άδειες Χρήσης Το παρόν εκπαιδευτικό

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

Solutions: Homework 3

Solutions: Homework 3 Solutios: Homework 3 Suppose that the radom variables Y,, Y satisfy Y i = βx i + ε i : i,, where x,, x R are fixed values ad ε,, ε Normal0, σ ) with σ R + kow Fid ˆβ = MLEβ) IND Solutio: Observe that Y

Διαβάστε περισσότερα

1. For each of the following power series, find the interval of convergence and the radius of convergence:

1. For each of the following power series, find the interval of convergence and the radius of convergence: Math 6 Practice Problems Solutios Power Series ad Taylor Series 1. For each of the followig power series, fid the iterval of covergece ad the radius of covergece: (a ( 1 x Notice that = ( 1 +1 ( x +1.

Διαβάστε περισσότερα

1. Matrix Algebra and Linear Economic Models

1. Matrix Algebra and Linear Economic Models Matrix Algebra ad Liear Ecoomic Models Refereces Ch 3 (Turkigto); Ch 4 5 (Klei) [] Motivatio Oe market equilibrium Model Assume perfectly competitive market: Both buyers ad sellers are price-takers Demad:

Διαβάστε περισσότερα

SUPPLEMENT TO ROBUSTNESS, INFINITESIMAL NEIGHBORHOODS, AND MOMENT RESTRICTIONS (Econometrica, Vol. 81, No. 3, May 2013, )

SUPPLEMENT TO ROBUSTNESS, INFINITESIMAL NEIGHBORHOODS, AND MOMENT RESTRICTIONS (Econometrica, Vol. 81, No. 3, May 2013, ) Ecoometrica Supplemetary Material SUPPLEMENT TO ROBUSTNESS, INFINITESIMAL NEIGHBORHOODS, AND MOMENT RESTRICTIONS (Ecoometrica, Vol. 81, No. 3, May 213, 1185 121) BY YUICHI KITAMURA,TAISUKE OTSU, ANDKIRILL

Διαβάστε περισσότερα

Three Classical Tests; Wald, LM(Score), and LR tests

Three Classical Tests; Wald, LM(Score), and LR tests Eco 60 Three Classical Tests; Wald, MScore, ad R tests Suppose that we have the desity l y; θ of a model with the ull hypothesis of the form H 0 ; θ θ 0. et θ be the lo-likelihood fuctio of the model ad

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

L.K.Gupta (Mathematic Classes) www.pioeermathematics.com MOBILE: 985577, 4677 + {JEE Mai 04} Sept 0 Name: Batch (Day) Phoe No. IT IS NOT ENOUGH TO HAVE A GOOD MIND, THE MAIN THING IS TO USE IT WELL Marks:

Διαβάστε περισσότερα

Introduction of Numerical Analysis #03 TAGAMI, Daisuke (IMI, Kyushu University)

Introduction of Numerical Analysis #03 TAGAMI, Daisuke (IMI, Kyushu University) Itroductio of Numerical Aalysis #03 TAGAMI, Daisuke (IMI, Kyushu Uiversity) web page of the lecture: http://www2.imi.kyushu-u.ac.jp/~tagami/lec/ Strategy of Numerical Simulatios Pheomea Error modelize

Διαβάστε περισσότερα

LAD Estimation for Time Series Models With Finite and Infinite Variance

LAD Estimation for Time Series Models With Finite and Infinite Variance LAD Estimatio for Time Series Moels With Fiite a Ifiite Variace Richar A. Davis Colorao State Uiversity William Dusmuir Uiversity of New South Wales 1 LAD Estimatio for ARMA Moels fiite variace ifiite

Διαβάστε περισσότερα

n r f ( n-r ) () x g () r () x (1.1) = Σ g() x = Σ n f < -n+ r> g () r -n + r dx r dx n + ( -n,m) dx -n n+1 1 -n -1 + ( -n,n+1)

n r f ( n-r ) () x g () r () x (1.1) = Σ g() x = Σ n f < -n+ r> g () r -n + r dx r dx n + ( -n,m) dx -n n+1 1 -n -1 + ( -n,n+1) 8 Higher Derivative of the Product of Two Fuctios 8. Leibiz Rule about the Higher Order Differetiatio Theorem 8.. (Leibiz) Whe fuctios f ad g f g are times differetiable, the followig epressio holds. r

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

IIT JEE (2013) (Trigonomtery 1) Solutions

IIT JEE (2013) (Trigonomtery 1) Solutions L.K. Gupta (Mathematic Classes) www.pioeermathematics.com MOBILE: 985577, 677 (+) PAPER B IIT JEE (0) (Trigoomtery ) Solutios TOWARDS IIT JEE IS NOT A JOURNEY, IT S A BATTLE, ONLY THE TOUGHEST WILL SURVIVE

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

Other Test Constructions: Likelihood Ratio & Bayes Tests

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

Διαβάστε περισσότερα

The Heisenberg Uncertainty Principle

The Heisenberg Uncertainty Principle Chemistry 460 Sprig 015 Dr. Jea M. Stadard March, 015 The Heiseberg Ucertaity Priciple A policema pulls Werer Heiseberg over o the Autobah for speedig. Policema: Sir, do you kow how fast you were goig?

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

Bessel function for complex variable

Bessel function for complex variable Besse fuctio for compex variabe Kauhito Miuyama May 4, 7 Besse fuctio The Besse fuctio Z ν () is the fuctio wich satisfies + ) ( + ν Z ν () =. () Three kids of the soutios of this equatio are give by {

Διαβάστε περισσότερα

Supplemental Material: Scaling Up Sparse Support Vector Machines by Simultaneous Feature and Sample Reduction

Supplemental Material: Scaling Up Sparse Support Vector Machines by Simultaneous Feature and Sample Reduction Supplemetal Material: Scalig Up Sparse Support Vector Machies by Simultaeous Feature ad Sample Reductio Weizhog Zhag * 2 Bi Hog * 3 Wei Liu 2 Jiepig Ye 3 Deg Cai Xiaofei He Jie Wag 3 State Key Lab of CAD&CG,

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

A study on generalized absolute summability factors for a triangular matrix

A study on generalized absolute summability factors for a triangular matrix Proceedigs of the Estoia Acadey of Scieces, 20, 60, 2, 5 20 doi: 0.376/proc.20.2.06 Available olie at www.eap.ee/proceedigs A study o geeralized absolute suability factors for a triagular atrix Ere Savaş

Διαβάστε περισσότερα

Lecture 3: Asymptotic Normality of M-estimators

Lecture 3: Asymptotic Normality of M-estimators Lecture 3: Asymptotic Istructor: Departmet of Ecoomics Staford Uiversity Prepared by Webo Zhou, Remi Uiversity Refereces Takeshi Amemiya, 1985, Advaced Ecoometrics, Harvard Uiversity Press Newey ad McFadde,

Διαβάστε περισσότερα

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

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

Διαβάστε περισσότερα

Στα επόμενα θεωρούμε ότι όλα συμβαίνουν σε ένα χώρο πιθανότητας ( Ω,,P) Modes of convergence: Οι τρόποι σύγκλισης μιας ακολουθίας τ.μ.

Στα επόμενα θεωρούμε ότι όλα συμβαίνουν σε ένα χώρο πιθανότητας ( Ω,,P) Modes of convergence: Οι τρόποι σύγκλισης μιας ακολουθίας τ.μ. Στα πόμνα θωρούμ ότι όλα συμβαίνουν σ ένα χώρο πιθανότητας ( Ω,,). Modes of covergece: Οι τρόποι σύγκλισης μιας ακολουθίας τ.μ. { } ίναι οι ξής: σ μια τ.μ.. Ισχυρή σύγκλιση strog covergece { } lim = =.

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

Presentation of complex number in Cartesian and polar coordinate system

Presentation of complex number in Cartesian and polar coordinate system 1 a + bi, aεr, bεr i = 1 z = a + bi a = Re(z), b = Im(z) give z = a + bi & w = c + di, a + bi = c + di a = c & b = d The complex cojugate of z = a + bi is z = a bi The sum of complex cojugates is real:

Διαβάστε περισσότερα

Example Sheet 3 Solutions

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

Διαβάστε περισσότερα

Statistical Inference I Locally most powerful tests

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

Διαβάστε περισσότερα

Biorthogonal Wavelets and Filter Banks via PFFS. Multiresolution Analysis (MRA) subspaces V j, and wavelet subspaces W j. f X n f, τ n φ τ n φ.

Biorthogonal Wavelets and Filter Banks via PFFS. Multiresolution Analysis (MRA) subspaces V j, and wavelet subspaces W j. f X n f, τ n φ τ n φ. Chapter 3. Biorthogoal Wavelets ad Filter Baks via PFFS 3.0 PFFS applied to shift-ivariat subspaces Defiitio: X is a shift-ivariat subspace if h X h( ) τ h X. Ex: Multiresolutio Aalysis (MRA) subspaces

Διαβάστε περισσότερα

Fractional Colorings and Zykov Products of graphs

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

Διαβάστε περισσότερα

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

Lecture 21: Properties and robustness of LSE

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

Διαβάστε περισσότερα

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

Last Lecture. Biostatistics Statistical Inference Lecture 19 Likelihood Ratio Test. Example of Hypothesis Testing.

Last Lecture. Biostatistics Statistical Inference Lecture 19 Likelihood Ratio Test. Example of Hypothesis Testing. Last Lecture Biostatistics 602 - Statistical Iferece Lecture 19 Likelihood Ratio Test Hyu Mi Kag March 26th, 2013 Describe the followig cocepts i your ow words Hypothesis Null Hypothesis Alterative Hypothesis

Διαβάστε περισσότερα

Supplementary Material For Testing Homogeneity of. High-dimensional Covariance Matrices

Supplementary Material For Testing Homogeneity of. High-dimensional Covariance Matrices Supplementary Material For Testing Homogeneity of High-dimensional Covariance Matrices Shurong Zheng, Ruitao Lin, Jianhua Guo, and Guosheng Yin 3 School of Mathematics & Statistics and KLAS, Northeast

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

SUPERPOSITION, MEASUREMENT, NORMALIZATION, EXPECTATION VALUES. Reading: QM course packet Ch 5 up to 5.6

SUPERPOSITION, MEASUREMENT, NORMALIZATION, EXPECTATION VALUES. Reading: QM course packet Ch 5 up to 5.6 SUPERPOSITION, MEASUREMENT, NORMALIZATION, EXPECTATION VALUES Readig: QM course packet Ch 5 up to 5. 1 ϕ (x) = E = π m( a) =1,,3,4,5 for xa (x) = πx si L L * = πx L si L.5 ϕ' -.5 z 1 (x) = L si

Διαβάστε περισσότερα

α β

α β 6. Eerg, Mometum coefficiets for differet velocit distributios Rehbock obtaied ) For Liear Velocit Distributio α + ε Vmax { } Vmax ε β +, i which ε v V o Give: α + ε > ε ( α ) Liear velocit distributio

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

derivation of the Laplacian from rectangular to spherical coordinates

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

Διαβάστε περισσότερα

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

A Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering

A Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering Electronic Companion A Two-Sie Laplace Inversion Algorithm with Computable Error Bouns an Its Applications in Financial Engineering Ning Cai, S. G. Kou, Zongjian Liu HKUST an Columbia University Appenix

Διαβάστε περισσότερα

Second Order RLC Filters

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

Διαβάστε περισσότερα

On Certain Subclass of λ-bazilevič Functions of Type α + iµ

On Certain Subclass of λ-bazilevič Functions of Type α + iµ Tamsui Oxford Joural of Mathematical Scieces 23(2 (27 141-153 Aletheia Uiversity O Certai Subclass of λ-bailevič Fuctios of Type α + iµ Zhi-Gag Wag, Chu-Yi Gao, ad Shao-Mou Yua College of Mathematics ad

Διαβάστε περισσότερα

A Note on Intuitionistic Fuzzy. Equivalence Relation

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

Διαβάστε περισσότερα

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

Tridiagonal matrices. Gérard MEURANT. October, 2008

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

Διαβάστε περισσότερα

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

Solve the difference equation

Solve the difference equation Solve the differece equatio Solutio: y + 3 3y + + y 0 give tat y 0 4, y 0 ad y 8. Let Z{y()} F() Taig Z-trasform o both sides i (), we get y + 3 3y + + y 0 () Z y + 3 3y + + y Z 0 Z y + 3 3Z y + + Z y

Διαβάστε περισσότερα

On Generating Relations of Some Triple. Hypergeometric Functions

On Generating Relations of Some Triple. Hypergeometric Functions It. Joural of Math. Aalysis, Vol. 5,, o., 5 - O Geeratig Relatios of Some Triple Hypergeometric Fuctios Fadhle B. F. Mohse ad Gamal A. Qashash Departmet of Mathematics, Faculty of Educatio Zigibar Ade

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

Uniform Convergence of Fourier Series Michael Taylor

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

Διαβάστε περισσότερα

Estimation for ARMA Processes with Stable Noise. Matt Calder & Richard A. Davis Colorado State University

Estimation for ARMA Processes with Stable Noise. Matt Calder & Richard A. Davis Colorado State University Estimation for ARMA Processes with Stable Noise Matt Calder & Richard A. Davis Colorado State University rdavis@stat.colostate.edu 1 ARMA processes with stable noise Review of M-estimation Examples of

Διαβάστε περισσότερα

= λ 1 1 e. = λ 1 =12. has the properties e 1. e 3,V(Y

= λ 1 1 e. = λ 1 =12. has the properties e 1. e 3,V(Y Stat 50 Homework Solutions Spring 005. (a λ λ λ 44 (b trace( λ + λ + λ 0 (c V (e x e e λ e e λ e (λ e by definition, the eigenvector e has the properties e λ e and e e. (d λ e e + λ e e + λ e e 8 6 4 4

Διαβάστε περισσότερα

Uniform Estimates for Distributions of the Sum of i.i.d. Random Variables with Fat Tail in the Threshold Case

Uniform Estimates for Distributions of the Sum of i.i.d. Random Variables with Fat Tail in the Threshold Case J. Math. Sci. Uiv. Tokyo 8 (2, 397 427. Uiform Estimates for Distributios of the Sum of i.i.d. om Variables with Fat Tail i the Threshold Case By Keji Nakahara Abstract. We show uiform estimates for distributios

Διαβάστε περισσότερα

Diane Hu LDA for Audio Music April 12, 2010

Diane Hu LDA for Audio Music April 12, 2010 Diae Hu LDA for Audio Music April, 00 Terms Model Terms (per sog: Variatioal Terms: p( α Γ( i α i i Γ(α i p( p(, β p(c, A j Σ i α i i i ( V / ep β (i j ij (3 q( γ Γ( i γ i i Γ(γ i q( φ q( ω { } (c A T

Διαβάστε περισσότερα

Adaptive Covariance Estimation with model selection

Adaptive Covariance Estimation with model selection Adaptive Covariace Estimatio with model selectio Rolado Biscay, Hélèe Lescorel ad Jea-Michel Loubes arxiv:03007v [mathst Mar 0 Abstract We provide i this paper a fully adaptive pealized procedure to select

Διαβάστε περισσότερα

On Inclusion Relation of Absolute Summability

On Inclusion Relation of Absolute Summability It. J. Cotemp. Math. Scieces, Vol. 5, 2010, o. 53, 2641-2646 O Iclusio Relatio of Absolute Summability Aradhaa Dutt Jauhari A/66 Suresh Sharma Nagar Bareilly UP) Idia-243006 aditya jauhari@rediffmail.com

Διαβάστε περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

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

Διαβάστε περισσότερα

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

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

Διαβάστε περισσότερα

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

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

Διαβάστε περισσότερα

MATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81

MATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 We know that KA = A If A is n th Order 3AB =3 3 A. B = 27 1 3 = 81 3 2. If A= 2 1 0 0 2 1 then

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

Degenerate Perturbation Theory

Degenerate Perturbation Theory R.G. Griffi BioNMR School page 1 Degeerate Perturbatio Theory 1.1 Geeral Whe cosiderig the CROSS EFFECT it is ecessary to deal with degeerate eergy levels ad therefore degeerate perturbatio theory. The

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

Supplement to A theoretical framework for Bayesian nonparametric regression: random series and rates of contraction

Supplement to A theoretical framework for Bayesian nonparametric regression: random series and rates of contraction Supplemet to A theoretical framework for Bayesia oparametric regressio: radom series ad rates of cotractio A Proof of Theorem 31 Proof of Theorem 31 First defie the followig quatity: ɛ = 3 t α, δ = α α

Διαβάστε περισσότερα

Μια εισαγωγή στα Μαθηματικά για Οικονομολόγους

Μια εισαγωγή στα Μαθηματικά για Οικονομολόγους Μια εισαγωγή στα Μαθηματικά για Οικονομολόγους Μαθηματικά Ικανές και αναγκαίες συνθήκες Έστω δυο προτάσεις Α και Β «Α είναι αναγκαία συνθήκη για την Β» «Α είναι ικανή συνθήκη για την Β» Α is ecessary for

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

p n r.01.05.10.15.20.25.30.35.40.45.50.55.60.65.70.75.80.85.90.95

p n r.01.05.10.15.20.25.30.35.40.45.50.55.60.65.70.75.80.85.90.95 r r Table 4 Biomial Probability Distributio C, r p q This table shows the probability of r successes i idepedet trials, each with probability of success p. p r.01.05.10.15.0.5.30.35.40.45.50.55.60.65.70.75.80.85.90.95

Διαβάστε περισσότερα

Reminders: linear functions

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

Διαβάστε περισσότερα

CRASH COURSE IN PRECALCULUS

CRASH COURSE IN PRECALCULUS CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter

Διαβάστε περισσότερα

= {{D α, D α }, D α }. = [D α, 4iσ µ α α D α µ ] = 4iσ µ α α [Dα, D α ] µ.

= {{D α, D α }, D α }. = [D α, 4iσ µ α α D α µ ] = 4iσ µ α α [Dα, D α ] µ. PHY 396 T: SUSY Solutions for problem set #1. Problem 2(a): First of all, [D α, D 2 D α D α ] = {D α, D α }D α D α {D α, D α } = {D α, D α }D α + D α {D α, D α } (S.1) = {{D α, D α }, D α }. Second, {D

Διαβάστε περισσότερα

Outline. Detection Theory. Background. Background (Cont.)

Outline. Detection Theory. Background. Background (Cont.) Outlie etectio heory Chapter7. etermiistic Sigals with Ukow Parameters afiseh S. Mazloum ov. 3th Backgroud Importace of sigal iformatio Ukow amplitude Ukow arrival time Siusoidal detectio Classical liear

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

Space-Time Symmetries

Space-Time Symmetries Chapter Space-Time Symmetries In classical fiel theory any continuous symmetry of the action generates a conserve current by Noether's proceure. If the Lagrangian is not invariant but only shifts by a

Διαβάστε περισσότερα

ORDINAL ARITHMETIC JULIAN J. SCHLÖDER

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

Διαβάστε περισσότερα

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

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

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

Διαβάστε περισσότερα

Appendix S1 1. ( z) α βc. dβ β δ β

Appendix S1 1. ( z) α βc. dβ β δ β Appendix S1 1 Proof of Lemma 1. Taking first and second partial derivatives of the expected profit function, as expressed in Eq. (7), with respect to l: Π Π ( z, λ, l) l θ + s ( s + h ) g ( t) dt λ Ω(

Διαβάστε περισσότερα

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

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

Διαβάστε περισσότερα

Γιάννης Σαριδάκης Σχολή Μ.Π.Δ., Πολυτεχνείο Κρήτης

Γιάννης Σαριδάκης Σχολή Μ.Π.Δ., Πολυτεχνείο Κρήτης 2 η Διάλεξη Ακολουθίες 29 Νοεµβρίου 206 Γιάννης Σαριδάκης Σχολή Μ.Π.Δ., Πολυτεχνείο Κρήτης ΑΠΕΙΡΟΣΤΙΚΟΣ ΛΟΓΙΣΜΟΣ, ΤΟΜΟΣ Ι - Fiey R.L. / Weir M.D. / Giordao F.R. Πανεπιστημιακές Εκδόσεις Κρήτης 2 Όρια Ακολουθιών

Διαβάστε περισσότερα

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits. EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.

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

Optimal Parameter in Hermitian and Skew-Hermitian Splitting Method for Certain Two-by-Two Block Matrices

Optimal Parameter in Hermitian and Skew-Hermitian Splitting Method for Certain Two-by-Two Block Matrices Optimal Parameter in Hermitian and Skew-Hermitian Splitting Method for Certain Two-by-Two Block Matrices Chi-Kwong Li Department of Mathematics The College of William and Mary Williamsburg, Virginia 23187-8795

Διαβάστε περισσότερα

MATH 38061/MATH48061/MATH68061: MULTIVARIATE STATISTICS Solutions to Problems on Matrix Algebra

MATH 38061/MATH48061/MATH68061: MULTIVARIATE STATISTICS Solutions to Problems on Matrix Algebra MATH 38061/MATH48061/MATH68061: MULTIVARIATE STATISTICS Solutios to Poblems o Matix Algeba 1 Let A be a squae diagoal matix takig the fom a 11 0 0 0 a 22 0 A 0 0 a pp The ad So, log det A t log A t log

Διαβάστε περισσότερα

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

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

Διαβάστε περισσότερα

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

TMA4115 Matematikk 3

TMA4115 Matematikk 3 TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet

Διαβάστε περισσότερα

Lecture 13 - Root Space Decomposition II

Lecture 13 - Root Space Decomposition II Lecture 13 - Root Space Decomposition II October 18, 2012 1 Review First let us recall the situation. Let g be a simple algebra, with maximal toral subalgebra h (which we are calling a CSA, or Cartan Subalgebra).

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

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds! MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.

Διαβάστε περισσότερα

5. Choice under Uncertainty

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

Διαβάστε περισσότερα

Lecture 34 Bootstrap confidence intervals

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

Διαβάστε περισσότερα

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

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

Διαβάστε περισσότερα

Supplemental Material to Comparison of inferential methods in partially identified models in terms of error in coverage probability

Supplemental Material to Comparison of inferential methods in partially identified models in terms of error in coverage probability Supplemetal Material to Compariso of iferetial methods i partially idetified models i terms of error i coverage probability Federico A. Bugi Departmet of Ecoomics Duke Uiversity federico.bugi@duke.edu.

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

INTEGRATION OF THE NORMAL DISTRIBUTION CURVE

INTEGRATION OF THE NORMAL DISTRIBUTION CURVE INTEGRATION OF THE NORMAL DISTRIBUTION CURVE By Tom Irvie Email: tomirvie@aol.com March 3, 999 Itroductio May processes have a ormal probability distributio. Broadbad radom vibratio is a example. The purpose

Διαβάστε περισσότερα