FORMULAS FOR MULTIPLICITIES OF sl(3) MODULES
|
|
- Ἀγαμέμνων Ρέντης
- 6 χρόνια πριν
- Προβολές:
Transcript
1 FORMULAS FOR MULTIPLICITIES OF sl() MODULES AMY BARKER AND LAUREN VOGELSTEIN Let g = sl(), = {α, α } and α = ε - ε, α = ε - ε, let λ be a dominant integral weight such that λ C +, let be the outer shell of WD(λ) and let µ WD(λ) C Figure. Weight diagram for λ = (6, ) Definitions Definition. If λ = (aω, bω ), then define λ θ as the line in C + such that λ θ = {λ qθ : 0 q min{a, b}}. Let C +I be the region in C + that contains all µ above λ θ and C +II is the region in C + that contains all µ below λ θ. Note: If µ C +I then there exist m, n Z + such that µ = λ mα nθ. If µ C +II then there exist l, k Z + such that µ = λ lα kθ. Definition. The distance between µ and λ is Date: June 8, 0. d(µ, λ) = min{t : µ = λ t α ij, α ij Φ + }. j=
2 AMY BARKER AND LAUREN VOGELSTEIN Figure. Weight diagram for λ = (6, ) with λ θ Definition. Let the distance between weight µ and outer shell be defined as follows: d(µ, ) = min{i : µ + iα / W D(λ), i Z +, α Φ + }. Barker Vogelstein Lemma Lemma. For all i in Z +, for all α Φ + either: d(µ + iα, λ) < d(µ, λ) or d(µ + iα, ) < d(µ, ) or both. Proof. Case A: Suppose µ C +I and µ + iα C +I for some i Z +. Then, by definition, d(µ, λ) = d(λ mα nθ, λ) = m + n. d(µ + iα, λ) = d(λ mα nθ + iα, λ) = d(λ (m i)α nθ, λ) = m i + n < m + n. Case B: Suppose µ C +I and µ + iα C +I where i Z +. Then, by definition, d(µ, δ) = d(λ mα nθ, δ) = n. Therefore, µ + iα = λ mα nθ + iα = λ mα nθ + i(θ α ) = λ (m + i)α (n ). d(µ + iα, δ) = d(λ (m + i)α (n )θ, δ) = n i < n.
3 FORMULAS FOR MULTIPLICITIES OF sl() MODULES Case C: Suppose µ C +I and µ + iθ C +I where i Z +. Then, by definition, d(µ, λ) = d(λ mα nθ, λ) = m + n. d(µ + iθ, λ) = d(λ mα (n i)θ, λ) = m + n i < m + n. Case A: Suppose µ C +II and µ + iα C +II where i Z +. Then, by definition, d(µ, δ) = d(λ lα kθ, δ) = k. Therefore, µ + iα = λ lα kθ + iα = λ lα kθ + i(θ α ) = λ (l + i)α (k i)θ. d(µ + iα, δ) = d(λ (l + i)α (k i)θ, δ) = k i < k. Case B: Suppose µ C +II then µ + iα C +II where i Z +. Then, by definition, d(µ, λ) = d(λ lα kθ, λ) = l + k. d(λ lα kθ + iα, λ) = d(λ (l i)α kθ, λ) = l + k i < l + k. Case C: Suppose µ C +II and µ + iθ C +II where i Z +. Case C is similar to Case C. Case A: Suppose µ λ θ and µ + iα λ θ where i Z +. Then, by definition, d(µ, δ) = d(λ qθ, δ) = q. Therefore, µ + iα = λ qθ + iα = λ qθ + i(θ α ) = λ iα (q i)θ. d(µ + iα ) = d(λ iα (q i)θ, δ) = q i < q. Case B: Suppose µ λ θ and µ + iα λ θ where i Z +. Then, by definition, d(µ, δ) = d(λ qθ, δ) = q. Therefore, µ + iα = λ qθ + iα = λ qθ + i(θ α ) = λ iα (q i)θ. d(µ + iα ) = d(λ iα (q i)θ, δ) = q i < q. Case C: Suppose µ λ θ andµ + iθ λ θ where i Z +. Case C is similar to Case C.
4 AMY BARKER AND LAUREN VOGELSTEIN Therefore, in C + either d(µ + iα, λ) < d(µ, λ) or d(µ + iα, δ) < d(µ, δ). This is true in all of WD(λ) by symmetry. Theorem (Freudenthal). [FH9,.] The multiplicity of µ W D(λ): Antoine-Speiser Formula (6) ((λ + ρ, λ + ρ) (µ + ρ, µ + ρ))m(µ) = α Φ + m(µ + iα)(µ + iα, α). Proposition 7 (Antoine-Speiser). Let g = sl(), then: () The multiplicity of any weight on the outer shell is. () The multiplicity increases by each time you move to any inner hexagonal shell. () Once the shells become triangular, the multiplicity remains constant. Proof. Let λ = (cω + dω ) = (c, d). First note that we can simplify the two sides of Freudenthal s Formula (6) as follows: On the left hand side: ((λ + ρ, λ + ρ) (µ + ρ, µ + ρ))m(µ) On the right hand side: = ((λ + θ, λ + θ) (µ + θ, µ + θ))m(µ) = ((λ, λ) + (λ, θ) (µ, µ) (µ, θ))m(µ). α Φ + m(µ + iα)(µ + iα, α) = [m(µ + iα )(µ + iα, α ) + m(µ + iα )(µ + iα, α ) +m(µ + iθ)(µ + iθ, θ)]. Our proof is a double induction. First we induct on distance to the outer shell and then we induct on distance to the vertex. We will do this first for the hexagonal shells and then for triangular shells. Base case for first induction on hexagonal shells: Suppose µ C + is on the outer shell, i.e. d(µ, ) =. We need to consider when µ is on the top edge of WD(λ) and when µ is on the right edge of WD(λ). Along the top edge: If µ is on the top edge, then µ = λ rα for some r Z 0.
5 FORMULAS FOR MULTIPLICITIES OF sl() MODULES The left hand side of Freudenthal s formula becomes ((λ, λ) + (λ, θ) (µ, µ) (µ, θ))m(µ) = ((λ, λ) + (λ, θ) (λ rα, λ rα ) (λ rα, θ))m(µ) = ((λ, λ) + (λ, θ) (λ, λ) + r(λ, α ) r (α, α ) (λ, θ) + r(α, θ))m(µ) = (r(cω + dω, ω ω ) r + r(ω ω, ω + ω ))m(µ) = (r(c(ω, ω ) c(ω, ω ) + d(ω, ω ) d(ω, ω )) r + r((ω, ω ) + (ω, ω ) (ω, ω ) (ω, ω ))m(µ) = (r(c c + d + d ) r + r( + ))m(µ) = (rc r + r)m(µ). The right hand side of Freudenthal s formula becomes α Φ + m(µ + iα)(µ + iα, α) = m(µ + iα )(µ + iα, α ) because µ + iα / WD(λ), µ + iθ / WD(λ). In order to simplify this further, we will now prove inductively that m(µ + iα ) =. Base Case: γ = λ kα, where k = 0 γ = λ therefore m(γ) = m(λ) =. Inductive Step: Assume m(γ) = for γ = λ kα such that k r. Then, because µ = λ rα m(µ + iα ) = m(λ rα + iα ) = m(λ (r i)α ) = m(λ kα ) =. Therefore m(µ + iα ) =. Returning to our simplification of the right hand side, we can now write: ()(µ + iα, α ) = r ((µ, α ) + i) = (µ, α ) r () + r i r(r + ) = r(µ, α ) + = r(λ rα, α ) + r(r + ) = r((λ, α ) r(α, α )) + r + r = r(λ, α ) r + r + r = r(cω + dω, ω ω ) r + r = r(c(ω, ω ) c(ω, ω ) + d(ω, ω ) d(ω, ω )) r + r = r(c c + d d ) r + r (8) = rc r + r.
6 6 AMY BARKER AND LAUREN VOGELSTEIN Combining the left and right hand sides (8), we have (rc r + r)m(µ) = rc r + r. Therefore, m(µ) =. Along the right edge: If µ is on the right edge, then µ = λ sα for some s Z 0. The left hand side of Freudenthal s formula becomes: ((λ, λ) + (λ, θ) (λ sα, λ sα ) (λ sα, θ))m(µ) = ((λ, λ) + (λ, θ) (λ, λ) + s(λ, α ) + s(λ, α ) s (α, α ) (λ, θ) + s(α, θ))m(µ) = (s(cω + dω, ω + ω ) s + s( ω + ω, ω + ω ))m(µ) = (s( c(ω, ω ) + c(ω, ω ) d(ω, ω ) + d(ω, ω )) s + s( (ω, ω ) (ω, ω ) + (ω, ω ) + (ω, ω )))m(µ) = (s( c + c d + d) s + s( + + )m(µ) = (sd s + s)m(µ). The right hand side of Freudenthal s formula becomes α Φ + m(µ + iα)(µ + iα, α) = m(µ + iα )(µ + iα, α ) because µ + iα / WD(λ), µ + iθ / WD(λ). Similarly, we can inductively prove that m(µ + iα ) =. Returning to our simplification of the right hand side, we can now write: (µ + iα, α ) = r [(µ, α ) + i] = (µ, α ) r () + r i s(s + ) = s(λ sα, α ) + = s(λ, α ) s (α, α ) + s(s + ) = s(cω + dω, ω + ω ) s + s + s = s( c(ω, ω ) + c(ω, ω ) d(ω, ω ) + d(ω, ω )) s + s = s( c + c d + d) s + s = sd s + s. Combining the left and right hand sides, we have Therefore, m(µ) =. (sd s + s)m(µ) = sd s + s.
7 FORMULAS FOR MULTIPLICITIES OF sl() MODULES 7 We have shown that for any µ on the top or right edge of the outer shell, m(µ) =. This is true on all of the outer shell by the symmetry of WD(λ). Inductive Assumption: We have proven that that the multiplicity of weights on the first shell is. Now we will assume that the multiplicity of the first k shells is m(µ S u ) = u, where S u is the u th shell and u {,,,..., k }. Base Case: vertex of the kth shell = µ = λ (k )θ = λ kθ + θ. The left hand side of Freudenthal s formula becomes: ((λ, λ) + (λ, θ) (λ kθ + θ, λ kθ + θ) (λ kθ + θ, θ))m(µ) = ((λ, λ) + (λ, θ) (λ, λ) + k(λ, θ) (λ, θ) + k(λ, θ) k (θ, θ) + k(θ, θ) (λ, θ) + k(θ, θ) (θ, θ) (λ, θ) + k(θ, θ) (θ, θ))m(µ) = ((k )(λ, θ) k + k + k + k )m(µ) = ((k )(λ, θ) k + 8k 6)m(µ). The right hand side of Freudenthal s formula is simplified by m(µ + iα) = k i for all α Φ + and becomes: α Φ + = m(µ + iα)(µ + iα, α) α Φ + = α Φ + = α Φ + = α Φ + (k i)(λ kθ + θ + iα, α) (k i)[(λ, α) k(θ, α) + (θ, α) + i] (λ, α)(k i) k(θ, α)(k i) + (θ, α)(k i) + i(k i) (λ, α)(k ) k term α Φ + (θ, α)(k i) + term α Φ + (θ, α)(k i) + term To simplify this further, we will break it down term by term. Term : (λ, α ) (k i) + (λ, α ) (k i) + (λ, θ) (k i) = ((λ, α ) + (λ, α ) + (λ, θ)) = (λ, θ)k(k ) = (k k)(λ, θ) k(k ) α Φ + i(k i). term
8 8 AMY BARKER AND LAUREN VOGELSTEIN Term : Term : Term : k(θ, α ) (k i) k(θ, α ) (k i) k(θ, θ) (k i) k(k ) k(k ) k(k ) = k k k = k (k ) k (k ) k (k ) = k (k ) (θ, α ) (k i) + (θ, α ) (k i) + (θ, θ) (k i) k(k ) = = k(k ) k(k ) + + (ki i ) = k i k(k ) k(k + ) k(k + )(k + ) = k 6 = 6k (k + ) k(k + )(k + ) i Term + Term + Term + Term Therefore, = (k k)(λ, θ) k (k ) + k(k ) + 6k (k + ) k(k + )(k + ) = (k k)(λ, θ) k + 8k 6k ((k )(λ, θ) k + 8k 6)m(µ) = (k k)(λ, θ) k + 8k 6k. Thus, m(µ) = k. This proves that the multiplicity of the vertex of the k th shell is k. Now, we will perform the second proof by induction. We will prove that the multiplicity of every weight on the k th shell is k by inducting on distance from the vertex. We will again do this along the top edge and the right edge of the k th hexagonal shell. Base for the Second Inductionon Hexagonal Shells: For µ on the k th shell, m(µ) = k. Second Inductive Assumption (Top Edge): Assume the multiplicity remains constant for (r ) steps away from the vertex of the k th shell in the α direction. Let µ be the weight r steps away from the k th vertex in the α direction such that µ = λ (k )θ + rα = λ kθ + θ + rα.
9 FORMULAS FOR MULTIPLICITIES OF sl() MODULES 9 The left hand side of Freudenthal s formula becomes ((λ, λ) (λ, θ) (λ kθ + θ + rα, λ kθ + θ + rα ) (λ kθ + θ + rα, θ))m(µ) = ((λ, λ) (λ, θ) (λ, λ) + k(λ, θ) (λ, θ) + r(λ, α ) + k(λ, θ) k (θ, θ) + k(θ, θ) kr(θ, α ) (λ, θ) + k(θ, θ) (θ, θ)r(θ, α ) rk(θ, α ) + r(θ, α ) r (α, α ) (λ, θ) + k(θ, θ) (θ, θ) + r(θ, α ))m(µ = ((k )(λ, θ) + r(λ, α ) k + k rk + k + r rk + r r + k + r)m(µ) = ((k )(λ, θ) + r(λ, α ) rk k + 8k + r 6 r )m(µ). The right hand side of Freudenthal s formula becomes m(µ + iα)(µ + iα, α) α Φ + = (λ kθ + θ rα + iα) = (λ, α) k(θ, α) + (θ, α) r(α, α) + i = m(µ + iα)[(λ, α) k(θ, α) + (θ, α) r(α, α) + i] α Φ + = α Φ + (λ, α)m(µ + iα) k }{{}}{{} r α Φ + term α Φ + (α, α)m(µ + iα) + term Term : α Φ + (λ, α)m(µ + iα) (θ, α)m(µ + iα) + term α Φ + r+k = (λ, α ) m(µ + iα ) +(λ, α ) (a) im(µ + iα). term α Φ + k m(µ + iα ) +(λ, θ) (b) (a): [ r+k r (λ, α ) m(µ + iα ) = (λ, α ) k + = (λ, α ) = (λ, α ) [ r+k k r+k i=r+ r+k i=r+ [ k(r + k) (k i + r) i + = (k k)(λ, α ) + rk(λ, α ) r=k i=r+ (θ, α)m(µ + iα) term k m(µ + iθ) (c) r ] ] (r + k)(r + k + ) r(r + ) ] + rk
10 0 AMY BARKER AND LAUREN VOGELSTEIN (b): (c): (λ, α ) (λ, θ) k m(µ + iα ) = (λ, α ) k (k i) = (k k)(λ, α ) k m(µ + iθ) = (λ, θ) Combing parts (a), (b), and (c) we see that Term : k (k i) = (k k)(λ, θ) Term = (k k)(λ, α ) + rk(λ, α ) + (k k)(λ, α ) + (k k)(λ, θ) k α Φ + = (k k)(λ, α + α + θ) + rk(λ, α ) = (k k)(λ, θ) + rk(λ, α ) = (rk k)(λ, θ) + rk(λ, α ) (θ, α)m(µ + iα) [ r+k = k (θ, α ) m(µ + iα ) + (θ, α ) k m(µ + iα ) + (θ, θ) ] k m(µ + iθ) However, by (a) we know r+k m(µ + iα ) = (k k + kr). Similarly, by (b)(c) we know k m(µ + iα ) = k m(µ + iθ) = (k k). Using this to simplify, we have [ Term = k (k k + kr) + ] (k k) + (k k) = k + k k r Term : (Note that Term = Term.) k α Φ + (θ, α)m(µ + iα) [ r+k = k(/k) (θ, α ) m(µ + iα ) + (θ, α ) = k + k kr k m(µ + iα ) + (θ, θ) ] k m(µ + iθ)
11 Term : r α Φ + FORMULAS FOR MULTIPLICITIES OF sl() MODULES (α, α)m(µ + iα) r+k = r(α, α ) m(µ + iα ) r(α, α ) r+k = r m(µ + iα ) + r r+k = r m(µ + iα ) k (k ) r k m(µ + iα ) r(α, θ) k (k ) k m(µ + iθ) From (a) we know r+k m(µ + iα ) = (k k + kr). Using this to simplify, we have Term : r+k r m(µ + iα ) = r( (k k + rk)) r+k im(µ + iα ) + = = r(k k + rk). k im(µ + iα ) + r r+k ki + i(k i + r) + r+k = k i r+ r+k i=r+ i + r = r k + rk + k k r+k i=r+ k im(µ + iθ) k i(k i) + i + 8k k i 8 k k i(k i) i Term + Term + Term + Term + Term = (k k)(λ, θ) + rk(λ, α ) rk k + k + rk + k k r k rk + rk + r k + rk + k k = k((k )(λ, θ) + r(λ, α ) rk k + 8k + r 6 r ) Therefore, ((k )(λ, θ) + r(θ, α ) k + 8k rk r + r 6)m(µ) = k((k )(λ, θ) + r(λ, α ) rk k + 8k + r 6 r ) Thus, m(µ) = k. This proves that every µ on the top edge of the k th hexagonal shell has a multiplicity of k. We can prove the same for weights on the right edge of the k th hexagonal shell. Second Inductive Assumption (Right Edge):
12 AMY BARKER AND LAUREN VOGELSTEIN Assume the multiplicity remains constant for (s ) steps away from the vertex of the k th shell in the α direction. Let µ be the weight s steps away from the k th vertex in the α direction such that µ = λ (k )θ + sα = λ kθ + θ + sα. Similarly, the left hand side of Freudenthal s formula becomes ((k )(λ, θ) + s(λ, α ) k + 8k sk 6 + s s )m(µ) and the right hand side becomes k((k )(λ, θ) + s(λ, α ) k + 8k sk 6 + s s ). Therefore, m(µ) = k. This proves that the multiplicity of any weight on the k th hexagonal shell is k. Now we will go through a similar process for triangular shells. We will prove that once the shells become triangular, the multiplicity of the weights is constant. This is done by first inductively proving that the multiplicity of the weights on the vertex of each triangular shell are equal. Then, by a second inductive proof, we will show that the multiplicity of weights along the top and right edge of each triangular shell equal the multiplicity of the weight on the vertex. Base Case for the First Induction on Triangular Shells: The multiplicity of the outermost triangular shell of W D(λ), where λ = (aω, bω ) is min(a, b) +. Inductive Assumption: (to prove that every triangular shell will have weights of equal multiplicity): Assume the multiplicity of the weights for the first (t ) th triangular shells is min(a, b)+. Now, we will examine the t th triangular vertex for the case when (a > b). In this case, µ = λ bθ t(θ + α ) = λ (b + t)θ tα. The left hand side of Freudenthal s formula can be simplified as follows ((λ, λ) + (λ, θ) (λ bθ tθ tα, λ bθ tθ tα ) (λ bθ tθ tα, θ))m(µ) = ((b + t)(λ, θ) + t(λ, α ) b 6bt 6t + b + 6t)m(µ). Note: (λ, θ) = (aω + bω, ω + ω ) = a + b (λ, α ) = (aω + bω, ω ω ) = a. With this, we can further reduce the left hand side. = ((b + t)(a + b) + t(a) b 6bt 6t + b + 6t)m(µ) = (ab + at bt 6t + b + 6t)m(µ) The right hand side of Freudenthal s formula can be simplified as follows
13 FORMULAS FOR MULTIPLICITIES OF sl() MODULES Note: m(µ + iα)(µ + iα, α) α Φ = (λ bθ tθ tα + iα, α) = (λ, α) b(θ, α) t(θ, α) t(α, α) + i = m(µ + iα)[(λ, α) (b + t)(θ, α) t(α, α) + i] α Φ = m(µ + iα)(λ, α) (b + t) m(µ + iα)(θ, α) α Φ α Φ }{{}}{{} term term t m(µ + iα)(α, α) + m(µ + iα)i. α Φ α Φ }{{}}{{} term term m(µ + iα ) = m(µ + iα ) = m(µ + iθ) = Therefore, m(µ + iα ) = m(µ + iα ) = m(µ + iθ) = { b + i t b + + t i t i b + t + t b+t+ (b + ) + (b + t + i) = b + bt + b + t. i=t+ We will use this to simplify Terms - below. Term : m(µ + iα)(λ, α) α Φ = (λ, α )(b + bt + b + t) + (λ, α )(b + bt + b + t) + (λ, θ)(b + bt + b + t) = [(λ, α ) + (λ, α ) + (λ, θ)](b + bt + b + t) = (λ, θ)(b + bt + b + t) = (λ, θ)(b + bt + b + t) = (a + b)(b + bt + b + t) = ab + abt + ab + at + b + b t + b + bt Term : (b + t) m(µ + iα)(θ, α) α Φ = [ (b + t)(θ, α ) (b + t)(θ, α ) (b + t)(θ, θ)](b + bt + b + t) = (b + t)( + + )(b + bt + b + t) = b b t b 8t bt 8bt
14 AMY BARKER AND LAUREN VOGELSTEIN Term : Term : m(µ + iα)i α Φ ( t = i(b + ) + = = ( ( (b + ) (b + ) t m(µ + iα)(α, α α Φ = [ t(α, α ) t(α, α ) t(α, θ)](b + bt + b + t) = [ t + t t](bt + t + b + b) = bt t b t bt t b+t+ b+t+ i=t+ i(b + + t i) ) b+t+ b+t+ i + (b + ) i + t i b+t+ i + t i=t+ i=t+ i b+t+ i=t+ i=t+ i ) ( ( ) (b + t + )(b + t + ) = (b + ) ( (b + t + )(b + t + )(b + t + ) 6 = 6bt + 6b t + bt + b + 6b + b + 6t + 6t b+t+ i=t+ i ) ( (b + t + )(b + t + ) + t )) t(t + )(t + ) 6 ) t(t + ) Term + Term + Term + Term = abt + ab + ab + at + b t + b + b + bt b t b bt 8bt 8t b t bt bt t + 6b t + b + 6b + bt + 6bt + 6t + b + 6t = (b + )(ab + at bt 6t + b + t). Now, setting the left hand side equal to the right hand side we have (ab + at bt 6t + b + 6t)m(µ) = (b + )(ab + at bt 6t + b + 6t). Thus, m(µ) = b +. Similarly, we can prove that m(µ) = a + for µ on the vertex of the t th triangular shell in the case where (a < b). Also, note that where (a = b) there will be no traingular shells. This proves that the weight on the vertex of every triangular shell will have the same multiplicity, namely min(a, b) +. Base Case for the Second Induction Step on Triangular Shells: For µ on the vertex of the t th triangular shell, m(µ) = min(a, b) + for any t. Inductive Assumption:
15 FORMULAS FOR MULTIPLICITIES OF sl() MODULES For a > b, assume that for the first (p-) steps from the t th triangular vertex in the α direction, these weights have a multiplicity of b + and µ = λ bθ tθ tα pα = λ (b + t)θ (p + t)α. The left hand side of Freudenthal s formula becomes ((λ, λ) + (λ, θ) (λ (b + t)θ (p + t)α, λ (b + t)θ (p + t)α ) (λ (b + t)θ (p + t)α, θ))m(µ) = (ab + at bt + ap 6t bp 6pt p + b + 6t + p)m(µ). The right hand side of Freudenthal s formula becomes m(µ + iα)(µ + iα, α) α Φ = (λ (b + t)θ (p + t)α + iα, α) = (λ, α) (b + t)(θ, α) (p + t)(α, α) + i = m(µ + iα)[(λ, α) (b + t)(θ, α) (p + t)(α, α) + i] α Φ = m(µ + iα)(λ, α) (b + t) m(µ + iα)(θ, α) (p + t) m(µ + iα)(α, α) α Φ α Φ α Φ }{{}}{{}}{{} term term term + m(µ + iα)i. α Φ }{{} term Note: { b + i t + p m(µ + iα ) = b + + p + t i p + t i b + p + t + { b + i t m(µ + iα ) = m(µ + iθ) = b + + t i t i b + t + Therefore, and α Φ α Φ b+p+t+ b+t+ m(µ + iα ) = α Φ b+t+ t+p m(µ + iα ) = (b + ) + m(µ + iθ) = b + bt + b + t b+p+t+ i=p+t+ b+p+t+ = (b + ) () + (p + t) = b + bp + bt + b + p + t. We will use this to simplify Terms - below. (b + + t + p i) b+p+t+ i=p+t+ () b+p+t+ i=p+t+ i
16 6 AMY BARKER AND LAUREN VOGELSTEIN Term : α Φ m(µ + iα)(λ, α) b+p+t+ = (λ, α ) b+t+ m(µ + iα ) + (λ, α ) b+t+ m(µ + iα ) + (λ, θ) m(µ + iθ = (λ, α )(b + bp + bt + b + p + t) + (λ, α )(b + bt + b + t) + (λ, θ)(b + bt + b + t) Term : (b + t) α Φ m(µ + iα)(θ, α) b+p+t+ = (b + t)(θ, α ) b+t+ m(µ + iα ) (b + t)(θ, α ) = (b + t)(b + bp + bt + b + p + t) (b + t)(b + bt + b + t) b+t+ m(µ + iα ) (b + t)(θ, θ) m(µ + iθ) Term : (p + t) α Φ m(µ + iα)(α, α) b+p+t+ b+t+ = (p + t)(α, α ) m(µ + iα ) (p + t)(α, α ) m(µ + iα ) b+t+ (p + t)(α, θ) m(µ + iθ) = (p + t)(b + bp + bt + b + p + t) Term : α Φ b+p+t+ m(µ + iα)i = m(µ + iα )i (a) b+t+ + b+t+ m(µ + iα )i + m(µ + iθ)i (b)
17 FORMULAS FOR MULTIPLICITIES OF sl() MODULES 7 (a): b+p+t+ m(µ + iα )i p+t b+p+t+ = i(b + ) + i(b + p + t + i) b+p+t+ = (b + ) i=p+t+ b+p+t+ i + (p + t) i=p+t+ b+p+t+ i i=p+t+ = b + b p + b t + b + bp + bpt + bp + bt + bt + b + p + pt + t + t + p i (b): b+t+ b+t+ m(µ + iα )i + b+t+ = 8 m(µ + iα )i m(µ + iθ)i = (6bt + 6b t + bt + b + 6b + b + 6t + 6t) Now, we have Term = (a) + (b) = b + b p + 6b t + 6b + bp + bpt + bp + 6bt + bt + b + p + pt + 6t + 6t + p. Combining Terms - will give us the complete and simplified right hand side of Freudenthal s formula. Term + Term + Term + Term = ((λ, α )(b + bp + bt + b + p + t) + (λ, α )(b + bt + b + t) + (λ, θ)(b + bt + b + t)) + ( (b + t)(b + bp + bt + b + p + t) (b + t)(b + bt + b + t)) + ( (p + t)(b + bp + bt + b + p + t)) + (b + b p + 6b t + 6b + bp + bpt + bp + 6bt + bt + b + p + pt + 6t + 6t + p) = (b + )(ab + at bt + ap 6t bp 6pt p + b + 6t + p) Setting the left hand side equal to the right hand side gives us: (ab + at bt + ap 6t bp 6pt p + b + 6t + p)m(µ) = (b + )(ab + at bt + ap 6t bp 6pt p + b + 6t + p) Thus, m(µ) = b +
18 8 AMY BARKER AND LAUREN VOGELSTEIN This proves that for a > b the multiplicity of any µ W D(λ) on a triangular shell when λ = (aω, bω ) is b +. Similarly, it can be proved that for b > a the multiplicity of any µ W D(λ) on a triangular shell when λ = (aω, bω ) is a +. Combining these conclusions, we see that the multiplicity of any µ on a triangular shell in W D(λ) for λ = (aω, bω )i is min(a, b) +. References [FH9] William Fulton and Joe Harris, Representation theory, Graduate Texts in Mathematics, vol. 9, Springer-Verlag, New York, 99. A first course; Readings in Mathematics. MR9 (9a:0069)
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 περισσότερα3.4 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 περισσότεραFractional 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 περισσότεραEvery 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 περισσότεραLecture 2. Soundness and completeness of propositional logic
Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness
Διαβάστε περισσότεραSrednicki 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 περισσότεραC.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 περισσότεραOrdinal 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 περισσότεραHomework 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 περισσότεραCRASH 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 περισσότεραMatrices 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 περισσότερα4.6 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 περισσότεραderivation 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 περισσότεραSolutions 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 περισσότεραEE512: 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 περισσότεραApproximation 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 περισσότεραHomework 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 περισσότεραORDINAL 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 περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραST5224: 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 περισσότεραNowhere-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 περισσότεραExample 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 περισσότεραA 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 περισσότεραCHAPTER 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 περισσότεραMath 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.
Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:
Διαβάστε περισσότεραFinite 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 περισσότεραSection 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 περισσότεραHOMEWORK 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 περισσότεραSCHOOL 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 περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραPhys460.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 περισσότεραMath221: 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 περισσότεραLecture 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 περισσότεραFourier 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 περισσότερα9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr
9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότεραTridiagonal 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 περισσότεραb. 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 περισσότεραSCITECH 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 περισσότεραLecture 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 περισσότεραUniform 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 περισσότεραΚΥΠΡΙΑΚΗ 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 περισσότεραConcrete 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 περισσότερα2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)
Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok
Διαβάστε περισσότεραSecond 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 περισσότερα12. Radon-Nikodym Theorem
Tutorial 12: Radon-Nikodym Theorem 1 12. Radon-Nikodym Theorem In the following, (Ω, F) is an arbitrary measurable space. Definition 96 Let μ and ν be two (possibly complex) measures on (Ω, F). We say
Διαβάστε περισσότεραLecture 10 - Representation Theory III: Theory of Weights
Lecture 10 - Representation Theory III: Theory of Weights February 18, 2012 1 Terminology One assumes a base = {α i } i has been chosen. Then a weight Λ with non-negative integral Dynkin coefficients Λ
Διαβάστε περισσότεραThe 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 περισσότεραDistances in Sierpiński Triangle Graphs
Distances in Sierpiński Triangle Graphs Sara Sabrina Zemljič joint work with Andreas M. Hinz June 18th 2015 Motivation Sierpiński triangle introduced by Wac law Sierpiński in 1915. S. S. Zemljič 1 Motivation
Διαβάστε περισσότεραSOLVING CUBICS AND QUARTICS BY RADICALS
SOLVING CUBICS AND QUARTICS BY RADICALS The purpose of this handout is to record the classical formulas expressing the roots of degree three and degree four polynomials in terms of radicals. We begin with
Διαβάστε περισσότεραProblem 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 περισσότεραTrigonometric Formula Sheet
Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ
Διαβάστε περισσότεραOn a four-dimensional hyperbolic manifold with finite volume
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In
Διαβάστε περισσότεραw 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( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Διαβάστε περισσότεραEcon 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 περισσότεραDifferential forms and the de Rham cohomology - Part I
Differential forms and the de Rham cohomology - Part I Paul Harrison University of Toronto October 30, 2009 I. Review Triangulation of Manifolds M = smooth, compact, oriented n-manifold. Can triangulate
Διαβάστε περισσότεραde Rham Theorem May 10, 2016
de Rham Theorem May 10, 2016 Stokes formula and the integration morphism: Let M = σ Σ σ be a smooth triangulated manifold. Fact: Stokes formula σ ω = σ dω holds, e.g. for simplices. It can be used to define
Διαβάστε περισσότεραLecture 15 - Root System Axiomatics
Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the
Διαβάστε περισσότεραOther 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 περισσότερα1 String with massive end-points
1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε
Διαβάστε περισσότεραGenerating Set of the Complete Semigroups of Binary Relations
Applied Mathematics 06 7 98-07 Published Online January 06 in SciRes http://wwwscirporg/journal/am http://dxdoiorg/036/am067009 Generating Set of the Complete Semigroups of Binary Relations Yasha iasamidze
Διαβάστε περισσότεραLecture 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 περισσότεραChapter 3: Ordinal Numbers
Chapter 3: Ordinal Numbers There are two kinds of number.. Ordinal numbers (0th), st, 2nd, 3rd, 4th, 5th,..., ω, ω +,... ω2, ω2+,... ω 2... answers to the question What position is... in a sequence? What
Διαβάστε περισσότεραΑπόκριση 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 περισσότεραMINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS
MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS FUMIE NAKAOKA AND NOBUYUKI ODA Received 20 December 2005; Revised 28 May 2006; Accepted 6 August 2006 Some properties of minimal closed sets and maximal closed
Διαβάστε περισσότεραSection 9.2 Polar Equations and Graphs
180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify
Διαβάστε περισσότεραPg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is
Pg. 9. The perimeter is P = The area of a triangle is A = bh where b is the base, h is the height 0 h= btan 60 = b = b In our case b =, then the area is A = = 0. By Pythagorean theorem a + a = d a a =
Διαβάστε περισσότεραChapter 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 περισσότερα6.1. 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 περισσότεραA 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 περισσότεραDESIGN 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 περισσότεραCommutative Monoids in Intuitionistic Fuzzy Sets
Commutative Monoids in Intuitionistic Fuzzy Sets S K Mala #1, Dr. MM Shanmugapriya *2 1 PhD Scholar in Mathematics, Karpagam University, Coimbatore, Tamilnadu- 641021 Assistant Professor of Mathematics,
Διαβάστε περισσότεραECE Spring Prof. David R. Jackson ECE Dept. Notes 2
ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =
Διαβάστε περισσότεραProblem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
Διαβάστε περισσότεραPractice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
Διαβάστε περισσότεραCyclic or elementary abelian Covers of K 4
Cyclic or elementary abelian Covers of K 4 Yan-Quan Feng Mathematics, Beijing Jiaotong University Beijing 100044, P.R. China Summer School, Rogla, Slovenian 2011-06 Outline 1 Question 2 Main results 3
Διαβάστε περισσότεραAffine Weyl Groups. Gabriele Nebe. Summerschool GRK 1632, September Lehrstuhl D für Mathematik
Affine Weyl Groups Gabriele Nebe Lehrstuhl D für Mathematik Summerschool GRK 1632, September 2015 Crystallographic root systems. Definition A crystallographic root system Φ is a finite set of non zero
Διαβάστε περισσότεραThe Pohozaev identity for the fractional Laplacian
The Pohozaev identity for the fractional Laplacian Xavier Ros-Oton Departament Matemàtica Aplicada I, Universitat Politècnica de Catalunya (joint work with Joaquim Serra) Xavier Ros-Oton (UPC) The Pohozaev
Διαβάστε περισσότεραExercises 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 περισσότεραEE101: Resonance in RLC circuits
EE11: Resonance in RLC circuits M. B. Patil mbatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Deartment of Electrical Engineering Indian Institute of Technology Bombay I V R V L V C I = I m = R + jωl + 1/jωC
Διαβάστε περισσότεραPartial 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 περισσότεραReminders: 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 περισσότεραω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
Διαβάστε περισσότεραSome new generalized topologies via hereditary classes. Key Words:hereditary generalized topological space, A κ(h,µ)-sets, κµ -topology.
Bol. Soc. Paran. Mat. (3s.) v. 30 2 (2012): 71 77. c SPM ISSN-2175-1188 on line ISSN-00378712 in press SPM: www.spm.uem.br/bspm doi:10.5269/bspm.v30i2.13793 Some new generalized topologies via hereditary
Διαβάστε περισσότεραPotential Dividers. 46 minutes. 46 marks. Page 1 of 11
Potential Dividers 46 minutes 46 marks Page 1 of 11 Q1. In the circuit shown in the figure below, the battery, of negligible internal resistance, has an emf of 30 V. The pd across the lamp is 6.0 V and
Διαβάστε περισσότεραCoefficient Inequalities for a New Subclass of K-uniformly Convex Functions
International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for
Διαβάστε περισσότεραSOME PROPERTIES OF FUZZY REAL NUMBERS
Sahand Communications in Mathematical Analysis (SCMA) Vol. 3 No. 1 (2016), 21-27 http://scma.maragheh.ac.ir SOME PROPERTIES OF FUZZY REAL NUMBERS BAYAZ DARABY 1 AND JAVAD JAFARI 2 Abstract. In the mathematical
Διαβάστε περισσότεραHigher Derivative Gravity Theories
Higher Derivative Gravity Theories Black Holes in AdS space-times James Mashiyane Supervisor: Prof Kevin Goldstein University of the Witwatersrand Second Mandelstam, 20 January 2018 James Mashiyane WITS)
Διαβάστε περισσότερα= {{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 περισσότεραNotes 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 περισσότεραStatistical 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 περισσότεραOscillatory integrals
Oscilltory integrls Jordn Bell jordn.bell@gmil.com Deprtment of Mthemtics, University of Toronto August, 0 Oscilltory integrls Suppose tht Φ C R d ), ψ DR d ), nd tht Φ is rel-vlued. I : 0, ) C by Iλ)
Διαβάστε περισσότερα( ) 2 and compare to M.
Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8
Διαβάστε περισσότεραMath 6 SL Probability Distributions Practice Test Mark Scheme
Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry
Διαβάστε περισσότεραk 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 περισσότεραDERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C
DERIVATION OF MILES EQUATION FOR AN APPLIED FORCE Revision C By Tom Irvine Email: tomirvine@aol.com August 6, 8 Introduction The obective is to derive a Miles equation which gives the overall response
Διαβάστε περισσότεραPhysics 523, Quantum Field Theory II Homework 9 Due Wednesday, 17 th March 2004
Physics 5 Quantum Field Theory II Homework 9 Due Wednesday 7 th March 004 Jacob Lewis Bourjaily β-functions in Pseudo-Scalar Yukawa Theory Let us consider the massless pseudo-scalar Yukawa theory governed
Διαβάστε περισσότεραΚΥΠΡΙΑΚΟΣ ΣΥΝΔΕΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY 21 ος ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ Δεύτερος Γύρος - 30 Μαρτίου 2011
Διάρκεια Διαγωνισμού: 3 ώρες Απαντήστε όλες τις ερωτήσεις Μέγιστο Βάρος (20 Μονάδες) Δίνεται ένα σύνολο από N σφαιρίδια τα οποία δεν έχουν όλα το ίδιο βάρος μεταξύ τους και ένα κουτί που αντέχει μέχρι
Διαβάστε περισσότερα= 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