text
stringlengths
16
3.88k
source
stringlengths
60
201
). We first describe the physical motivation and then state the mathematical problem. Imagine a material which occupies a certain region U in the physical space V = R3 (a space with a positive definite inner product). Suppose the material is deformed. This means, we have U �. The question in elasticity theory applie...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
part on the opposite side. It is easy to deduce from Newton’s laws that Fv is linear in v, so there exists a linear operator SP : V V such that Fv = SP v. It is called the stress tensor. ⊃ || || v An elasticity law is an equation SP = f (dP ), where f is a function. The simplest such law is a linear law (Hooke’s ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
and for x real numbers K, µ. � � In fact, it is clear from physics that K, µ are positive. Physically, the compression modulus K characterises resistance of the material to compression or dilation, while the shearing modulus µ characterizes its resistance to changing the shape of the object without changing its vol...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
cases, let B be the invariant bilinear form on V , and (, ) the invariant positive Hermitian form (they are defined up to a nonzero complex scalar and a V such that B(v, w) = (v, jw). positive real scalar, respectively), and define the operator j : V ij), and j 2 = ∂ Id, where ∂ is a real number, positive in Show t...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
, all five irreducible representations , C2 , C3 tions C+, C − 3 , C3 , C4 , C−5 are of real type. As for Q8, its one-dimensional representations are of of A5 – C, C+ real type, and the two-dimensional one is of quaternionic type. ⊃ − − − Definition 4.3. The Frobenius-Schur indicator F S(V ) of an irreducible represen...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
V ( − G | | g 2) = νS2V (P ) � G g � ν − 2V (P ) = dim(S2V )G − √ dim( √ 2V )G = Finally, the number of involutions in G equals 1, 1, 0, − if V is of real type if V is of quaternionic type if V is of complex type ⎞ ⎟ ⎠ 1 G | � V | dim V νV ( g 2) = dim V � G g � � real V dim V. − � quat V Corollary 4.5. Assu...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
by Frobenius, became the starting point for creation of representation theory (see [Cu]). Theorem 4.7. r det XG = Pj (x)deg Pj � j=1 for some pairwise non-proportional irreducible polynomials Pj (x), where r is the number of conju­ gacy classes of G. We will need the following simple lemma. Lemma 4.8. Let Y be a...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
ke’s theorem, we have r detV L(x) = (detVi L(x))dim Vi , � i=1 where Vi are the irreducible representations of G. We set Pi = detVi L(x). Let and Ei,jk End Vi be the matrix units in these bases. Then { is a basis of C[G] and eim} be bases of Vi Ei,jk} { � L(x) Vi = | � j,k yi,jkEi,jk, where yi,jk are new ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
coefficients). To show (4.9) (4.10), suppose z is a root of ≥ (4.9), notice that z is a root of the characteristic polynomial of the matrix ≥ p(x) = x n + a1x n − 1 + . . . + an 1x + an. − Then the characteristic polynomial of the following matrix (called the companion matrix) is p(x): 49 0 0 0 1 0 ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
� B The corresponding eigenvector is in both cases v w. This shows that both A and Q are rings. To show that the latter is a field, it suffices to note that if ϕ = 0 is a root of a polynomial p(x) of 1 is a root of x p(1/x). The last statement is easy, since a number ϕ is algebraic degree d, then ϕ− if and only if it...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
conjugates of ϕ; they are roots of any polynomial q with rational coefficients such that q(ϕ) = 0. 50 ⇒ ⇒ Note that any algebraic conjugate of an algebraic integer is obviously also an algebraic inte­ ger. Therefore, by the Vieta theorem, the minimal polynomial of an algebraic integer has integer coefficients. ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Hint. Consider the representations of G over the field Q of algebraic numbers. (b) Show that if V is an irreducible complex representation of a finite group G of dimension > 1 then there exists g G such that νV (g) = 0. � Hint: Assume the contrary. Use orthonormality of characters to show that the arithmetic mean 1...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
and derive a contradiction. g=1 | | � �⊃ 4.4 Frobenius divisibility Theorem 4.16. Let G be a finite group, and let V be an irreducible representation of G over C. Then Proof. Let C1, C2, . . . , Cn be the conjugacy classes of G. Set dim V divides G . | | ∂i = νV (gCi ) | Ci| dim V , where gCi is a representative o...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
gC| | i = e in G, the eigenvalues of δ(gCi ) are roots of unity), and (iii) A is a ring (Proposition 4.12). On the other hand, from the definition of ∂i, ∂iνV (gCi ) = � Ci � i Ci| | νV (gCi )νV (gCi ) . dim V Recalling that νV is a class function, this is equal to νV (g)νV (g) dim V � G g � = | G (νV , ν...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
mathematician William Burnside in the early 20-th century, using representation theory (see [Cu]). Here is this proof, presented in modern language. Before proving Burnside’s theorem we will prove several other results which are of independent interest. Theorem 4.21. Let V be an irreducible representation of a fini...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
of unity, so νV (g) is an algebraic integer. Since νV (g) is an algebraic integer. Also, by Proposition 4.17, n | gcd(n, C ) = 1, there exist integers a, b such that a C + bn = 1. This implies that C 1 | | | | | νV (g) n = (π1 + . . . + πn). 1 n is an algebraic integer. Thus, by Lemma 4.22, we get that either π1...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
N such that νV (g) = 0. � Proof. If V � D, the number 1 dim(V )νV (g) is an algebraic integer, so p a = 1 p � D V � dim(V )νV (g) is an algebraic integer. Now, by (4), we have 0 = νC(g) + dim V νV (g) + dim V νV (g) = 1 + pa + dim V νV (g). � V D � � V N � � N V � This means that the last summand is...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
qb, we see that there has to be more than one conjugacy class consisting just of one element. So G has a nontrivial center, which gives a contradiction. ⊂ a 4.6 Representations of products Theorem 4.25. Let G, H be finite groups, field k (of any characteristic), and irreducible representations of G Wj } H over k...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
, so ni = +1 and we are done. = 1, meaning that ni = 2 i . So 2 i ni i n ⎨ ⎨ ⎨ ± niVi. Then by 1 for exactly 4.8 Induced Representations Given a representation V of a group G and a subgroup H G, there is a natural way to construct H V is the representation given a representation of H. The restricted represent...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
�)(f )(x) for any g, g�, x G and h H. � � Remark 4.30. Notice that if we choose a representative xε from every right H-coset ε of G, then any f is uniquely determined by IndG . f (xε) H V � { } Because of this, dim(IndG H V ) = dim V . G | H | | | · Problem 4.31. Check that if K H is isomorphic to IndG →...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
� � G:xgx−1 x � Proof. For a right H-coset ε of G, let us define Vε = f { IndG H V | � f (g) = 0 g ⊕ ε . } ⇒� Then one has and so IndG = H V Vε, � ε ν(g) = νε(g), � ε 55 where νε(g) is the trace of the diagonal block of δ(g) corresponding to Vε. Since g(ε) = εg is a right H-coset...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
representation of G and W a representation of H. Then →G H W ) is naturally isomorphic to HomH (ResG H V, W ). Proof. Let E = HomG(V, IndG H W ) and E� E as follows: F (ϕ)v = (ϕv)(e) for any ϕ = HomH (ResG ⊃ E and (F �(α)v)(x) = α(xv) for any α H V, W ). Define F : E E and F � � E �. : E � ⊃ � � are well de...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
(g(F �(α)v))(x). (d) F ∞ F � = IdE⊗ . This holds since F (F �(α))v = (F �(α)v)(e) = α(v). (e) F � ∞ F = IdE , i.e., (F �(F (ϕ))v)(x) = (ϕv)(x). Indeed, (F �(F (ϕ))v)(x) = F (ϕxv) = (ϕxv)(e) = (xϕv)(e) = (ϕv)(x), and we are done. Exercise. The purpose of this exercise is to understand the notions of restricted and i...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Then, V is a left k [G]-module, thus a (k [G] , k)-bimodule. Thus, the tensor product k [G]1 �k[G] V is a (k [H] , k)-bimodule, i. e., a left k [H]-module. Prove that this tensor product is isomorphic to ResG ⊃ k [G]1 �k[G] V H V as a left k [H]-module. The isomorphism ResG �k[G] v for every v is given by v ResG...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Then, W is a left k [H]-module, thus a (k [H] , k)­ , W ), but also isomorphic to bimodule. Show that IndG k [G]2�k[H]W is given by f k [G]2�k[H]W . The isomorphism Homk[H] (k [G]1 , W ) f (g) for every f H-cosets in G. (This isomorphism is independent of the choice of representatives.) H W is not only isomorphi...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
� � ⎩ ⊃ k given by IndG ⊕ as representations of H (V ⊕) as Homk[H] (k [G]1 , V ⊕). Prove (f (Sx)) (v) is k [G] is the linear map defined by H V � ⎩ x f, �k[H] v ⎩ �⊃ �� ⎩ � 4.11 Examples Here are some examples of induced representations (we use the notation for representations from the character tables). ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
of Sn In this subsection we give a description of the representations of the symmetric group S n for any n. Definition 4.35. A partition ∂ of n is a representation of n in the form n = ∂1 + ∂2 + ... + ∂p, where ∂i are positive integers, and ∂i ∂i+1. ⊂ ∗ ∗ To such ∂ we will attach a Young diagram Y�, which is the ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Set c� = a�b�. Since P� � Q� g � b� := 1)gg, − ( where ( element is nonzero. − Q� = , this 1 } { ∈ The irreducible representations of Sn are described by the following theorem. Theorem 4.36. The subspace V� := C[Sn]c� of C[Sn] is an irreducible representation of Sn under left multiplication. Every irreducible re...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
representations of Sn are real, i.e., admit a nondegenerate invariant symmetric form. Then use the Frobenius-Schur theorem. 4.13 Proof of Theorem 4.36 Lemma 4.40. Let x � C[Sn]. Then a�xb� = σ�(x)c�, where σ� is a linear function. P�Q�, then g has a unique representation as pq, p 1)qc�. Proof. If g Thus, to p...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
ent columns of T �, so there exists q1� � have which moves all these elements to the first row. So there is p1 P� such that p1T and q1� T � the same first row. Now do the same procedure with the second row, finding elements p2, q2� such have the same first two rows. Continuing so, we will construct the desired that ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
��nd elements p1 same first row, and repeat the argument for the second row, and so on. Eventually, having done 1 such steps, we’ll have ∂i > µi, which means that some two elements of the i-th row of the first i − tableau are in the same column of the second tableau, completing the proof. 1 such that p1T and q1� T ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
to prove Theorem 4.36. Let ∂ µ. Then by Lemmas 4.42, 4.43 ⊂ HomSn (V�, Vµ) = HomSn (C[Sn]c�, C[Sn]cµ) = c�C[Sn]cµ. The latter space is zero for ∂ > µ by Lemma 4.41, and 1-dimensional if ∂ = µ by Lemmas 4.40 and 4.42. Therefore, V� are irreducible, and V� is not isomorphic to Vµ if ∂ = µ. Since the number of parti...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
the character of U�. Let Ci be the conjugacy class in Sn having il cycles 1 (here i is a shorthand notation for (i1, ..., il, ...)). Also let x1, ..., xN be of length l for all l variables, and let ⊂ be the power sum polynomials. Hm(x) = m xi � i Theorem 4.46. Let N �j in the polynomial of x� := xj ⊂ p (wh...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
= Zg| | � m m im im!, νU� (Ci) = m ⎛ mim im! j ∂j! | Ci . P�| ∈ m Sim ∼ (Z/mZ)im , so ⎛ Now, since P� = j S�j , we have ⎛ ⎛ Ci P�| ∈ | = r � � 1 j ∧ ∂j ! 1 mrjm rjm! , m ∧ ⎛ where r = (rjm) runs over all collections of nonnegative integers such that mrjm = ∂j , rjm = im. � m � j Indeed, an element ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
� p. Then νV� (Ci) is the coefficient of x�+χ := �j +N xj j − in the polyno­ �(x) Hm(x)im . � 1 m ∧ ⎛ Remark. Here is an equivalent formulation of Theorem 4.47: νV� (Ci) is the coefficient of x� in the (Laurent) polynomial 1 − �� i<j Hm(x)im . i � � 1 m x j x ∧ 61 Proof. Denote...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
µ > ∂ or µ = ∂, and the case µ = ∂ arises only if of the form ei − ε = 1, as desired. ε(δ) � ∂ + δ ε(χ) − − − − ◦ ◦ � � Therefore, to show that χ� = ν�, by Lemma 4.27, it suffices to show that (χ�, χ�) = 1. We have Using that (χ�, χ�) = 1 ! n � i χ�(Ci)2 . Ci | | = Ci | | n! , m mim im! we conclude that (χ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
xiyj) − yj ) . (zj zi)(yi − i,j(zi − yj) − yj ) = det( zi 1 − ). yj ⎛ (zi− Proof. Multiply both sides by yj). Then the right hand side must vanish on the hyperplanes zi = zj and yi = yj (i.e., be divisible by �(z)�(y)), and is a homogeneous polynomial of degree 1). This implies that the right hand s...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
This is a partial order, and µ � ⇔ − ∂ is a sum of ∂ implies ⇔ ∂. It follows from Theorem 4.47 and its proof that vectors of the form ei µ − ⊂ This implies that the Kostka numbers Kµ� vanish unless µ � ∂. ⇔ ν� = �µ ≥ �K µ�νUµ . 4.16 Problems In the following problems, we do not make a distinction between Young...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
1 and n 1. − − Hint. Represent E as Cn Cn − − 1, where Cn = C is the element from Problem 4.51. (b) Show that the element (12) + ... + (1n) acts on V� by a scalar if and only if ∂ is a rectangular Young diagram, and compute this scalar. 4.17 The hook length formula Let us use the Frobenius character formula t...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
) � 1 i<j N → → (5) ⇒ (where N p). ⊂ In this formula, there are many cancelations. After making some of these cancelations, we ∂ j), j. 1, i obtain the hook length formula. Namely, for a square (i, j) in a Young diagram ∂ (i, j ⊂ ∗ = i, j� = j or i� define the hook of (i, j) to be the set of a...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
, and B = EndA E. Then: (i) A = EndB E (i.e., the centralizer of the centralizer of A is A); (ii) B is semisimple; (iii) as a representation of A Wi, where Vi are all the B, E decomposes as E = irreducible representations of A, and Wi are all the irreducible representations of B. In particular, we have a natur...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
� 1 + 1 � b � ... � 1 + ... + 1 � 1 � ... � b, gl(V ). b � Proof. Clearly, the image of U(gl(V )) is contained in B, so we just need to show that any element of B is contained in the image of U(gl(V )). By definition, B = S n End V , so the result follows from part (ii) of the following lemma. 64 ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
which goes under the name “Schur-Weyl duality”. Theorem 4.57. (i) The image A of C[Sn] and the image B of U(gl(V )) in End(V � izers of each other. n) are central­ (ii) Both A and B are semisimple. In particular, V � n is a semisimple gl(V )-module. (iii) We have a decomposition of A L�, where the summation B-mo...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
ducible representations of GL(V ) or zero. GL(V ), V � n decomposes as ��V� L�, where � Example 4.60. If ∂ = (n) then L� = SnV , and if ∂ = (1n) (n copies of 1) then L� = shown in Problem 3.19 that these representations are indeed irreducible (except that if n > dim V ). √ √ nV . It was nV is zero 65 4....
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Proposition 4.62. Therefore, S�(1, z, z 2 , ..., z N 1) = − S�(1, ..., 1) = � 1 i<j N → → ∂i z�i i − i z− j z�j − j z− − − − ∂j + j i j i − − � 1 i<j N → → Proof. The first identity is obtained from the definition using the Vandermonde determinant. The second identity follows from the first one by set...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
of ∂. If N Therefore, the dimension of L� is given by the formula ⊂ dim L� = ∂i � 1 i<j N → → i − − ∂j + j i j − This shows that irreducible representations of GL(V ) which occur in V � by Young diagrams with any number of squares but at most N = dim V rows. n for some n are labeled Proposition 4.64. The ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
�1, ..., ∂N ) of integers (not necessarily positive) such that ∂1 ∂N . This sequence is called the highest weight of L�. r 1N := L� · N V ⊕)� ... � ⊂ ⊂ √ ( Theorem 4.66. (i) Every finite dimensional polynomial representation of GL(V ) is completely reducible, and decomposes into summands of the form L� (which ar...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
we may assume that Y is contained in a quotient of a (finite) form Sr(V ( √ N V ⊕, Y is contained in a direct sum of direct sum of such representations. As V ⊕ N V ⊕)� representations of the form V � s, and we are done. N V ⊕)� V ⊕) = � √ 1V Y ⊃ � → � � � √ ( n N − � √ (ii) Let Y be a polynomial representa...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
by scalars, the above results extend in a straightforward manner to representations of the Lie algebra sl(V ). Similarly, the results for GL(V ) extend to the case of the group SL(V ) of operators with determinant 1. The only difference is that in this case the representations L� and L�+1m are ∂N isomorphic, so th...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
�ecting the Young diagram of ∂. � � − 1)ss for any permutation s. . Show also that θ(C[Sn]a) = C[Sn]θ(a), is the conjugate partition to ∂, − � − = V�� , where ∂⊕ C Problem 4.69. Let Rk,N be the algebra of polynomials on the space of k-tuples of complex N by N matrices X1, ..., Xk, invariant under simultaneous c...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
G | GL2(Fq) | | = q(q + 1)(q 1)2 . − 68 The goal of this section is to describe the irreducible representations of G. To begin, let us find the conjugacy classes in GL2(Fq). Representatives Scalar 0 x 0 x � ⎩ Parabolic 1 x 0 x � ⎩ Hyperbolic 0 x 0 y , y = x � ⎩ x ζy y x Elliptic Fq, , x � F...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Let A be such a matrix, and consider a quadratic extension of Fq, Over this field, A will have eigenvalues and with corresponding eigenvectors Fq(∀π), π Fq � F2 .q \ ϕ = ϕ1 + ∀πϕ2 ϕ = ϕ1 − ∀πϕ2, v, v (Av = ϕv, Av = ϕv). Choose a basis In this basis, the matrix A will have the form e1 = v + v, e2 = ∀π(v ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
only the first two matrices are commutators. But it is easy to see that the matrix is the commutator of the matrices 1 1 0 1 � � while the matrix A = 1 1/2 1 0 � � , B = 1 0 � 0 1 � − , a 0 1 0 a− � � is the commutator of the matrices A = a 0 0 1 � � , B = 0 1 1 0 � , � This completes the proof. There...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
where C� is the 1-dimensional representation of B in which B acts by ∂. We have Wµ, where Wµ is a q-dimensional irreducible representation of if and only if ∂1, ∂2} { = ⊗ ∂ ⊗ 1, ∂ 2} { (in the ∂(aga− 1). dim(V�1,�2 ) = | | G B | | = q + 1. V�1,�2 is irreducible. Theorem 4.71. 2. ∂1 = ∂2 = µ G. ≥ 1. ∂1 =...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
∂(g) 1, · 1 aga− B a � ≥ � B. g = x 0 0 y � � , ∂1(x)∂2(y) + ∂1(y)∂2(x) 1, · � ⎩ B or a is an element of B multiplied by the transposition matrix. g = x πy x y � � , x = y the expression on the right evaluates to 0 because matrices of this type don’t have eigenvalues over Fq (and thus cannot be conjugate...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Clearly, since νV�1,�2 , νV�1,�2 � ◦ = 2. IndG B Cµ,µ, Cµ ∧ HomG(Cµ, IndG BCµ,µ) = HomB(Cµ, Cµ) = C (Theorem 4.33). Therefore, IndG BCµ,µ = Cµ values of µ, proving that Wµ are distinct. Wµ; Wµ � is irreducible; and the character of Wµ is different for distinct 72 ⇒ ∞ If ∂1 = ∂2, let z = xy...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
bolic elements and note that the function ∂1(x)∂2(y) + ∂1(y)∂2(x) determines ∂1, ∂2 up to permutation. 4.24.4 Complementary series representations ∩ Fq be a quadratic extension Fq(∀π), π Let Fq2 q. We regard this as a 2-dimensional vector � space over Fq; then G is the group of linear transformations of Fq2 ov...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Therefore, for λ q = K Cξq ∪ IndG = IndG λ we get 2 1 q(q 1) representations. − Next, we look at the following tensor product: � where 1 is the trivial character and W1 is defined as in the previous section. The character of this representation is W1 V�,1, x 0 0 x � ν � = q(q + 1)ϕ(x); ν(A) = 0 for A para...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Proof. ν, ν � ◦ = 1 ν(1) > 0. We now compute the inner product ν, ν � ◦ ν(1) = q(q + 1) (q + 1) q(q 1) = q 1 > 0. − − . Since ϕ is a root of unity, this will be equal to − − 1 (q 1)2q(q + 1) � (q − 1) (q · − − 1)2 1+(q · 2 1) 1 (q · · − − q(q 1)+ − 2 1) · (λ(ψ)+λq(ψ))(λ(ψ) + λ q(ψ)) � λ elliptic...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
(q q(q + 1) ⎩ 1) (q · − 1)2 1+(q · − 2 1) 1 (q · · − − 1)+ q(q − 2 1) · 2 (2(q q) − − 2(q − 1)) = 1. � We have now shown that for any λ with λ q = λ the representation Yξ with the same character as W1 � V�,1 − V�,1 − IndG K Cξ ⊃ We have thus found q λq), so there are q(q − 2 exists and is irred...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
of characters of induced representations IndG H V , where H X and V is an irreducible representation of H. � Remark. Statement (ii) of Theorem 4.73 is equivalent to the same statement with Q-span replaced by C-span. Indeed, consider the matrix whose columns consist of the coefficients of the decomposition of IndG ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
νU vanishes on H for any H X. Hence by (i), νU is identically zero. This implies (ii) (because of the above remark). H | � Corollary 4.74. Any irreducible character of a finite group is a rational linear combination of induced characters from its cyclic subgroups. 4.26 Representations of semidirect products Let ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
{ ⊃ Next, we introduce an additional action of A on this space by (af )(g) = x(g(a))f (g). Then it’s easy to check that these two actions combine into an action of G ∼ A. Also, it is clear that this O, representation does not really depend on the choice of x, in the following sense. Let x, y G be such that gx = y...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
W V(O,U )| � V is a subrepresentation, then W = → v(g) = 0 unless gy = where Vy = Vy. Now, Vy is a x representation of Gy, which goes to U under any isomorphism Gy G mapping x to y. Hence, Vy is irreducible over Gy, so Wy = 0 or Wy = Vy for each y. Also, if hy = z then hWy = Wz, so either Wy = 0 for all y o...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
. Field embeddings. Recall that k(y1, ..., ym) denotes the field of rational functions of y1, ..., ym over a field k. Let f : k[x1, ..., xn] k(y1, ..., ym) be an injective k-algebra homomor­ n. (Look at the growth of dimensions of the spaces WN of polynomials of phism. Show that m ⊂ degree N in xi and their images ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
5.1. ⊃ (c) generalize the result of this problem to the case when G = GLn1 (k) × ... × GLnm (k). Problem 5.3. Dynkin diagrams. Let � be a graph, i.e., a finite set of points (vertices) connected with a certain number of edges (we allow multiple edges). We assume that � is connected (any vertex can be connected t...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
diagram if and only if it is one on the following graphs: An : • Dn: • E6 : • �−−� · · · �−−� �−−� · · · �−−� | � �−−�−−�−−�−−� | � 78 E7 : E8 : • • �−−�−−�−−�−−�−−� | � �−−�−−�−−�−−�−−�−−� | � (a) Compute the determinant of A� where � = AN , DN . (Use the row decomposition rule, and write dow...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
�) = 0 for all graphs � below: 1 2 1 2 3 2 1 2 1 2 3 4 3 2 1 7Recall the Sylvester criterion: a symmetric real matrix is positive definite if and only if all its upper left corner principal minors are positive. 8The Sylvester criterion says that a symmetric bilinear form (, ) on RN is positive definite if and o...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
iver Q is of finite type if and only if the corresponding unoriented graph (i.e., with directions of arrows forgotten) is a Dynkin diagram. In this problem you will prove the “only if” direction of this theorem (i.e., why other quivers are NOT of finite type). (a) Show that if Q is of finite type then for any rational...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
��nite subgroup of SU (2), and V be the 2-dimensional representation of G coming from its embedding into SU (2). Let Vi, i I, be all the irreducible representations of G. Let rij be the multiplicity of Vi in V Vj. � � (a) Show that rij = rji. (b) The McKay graph of G, M (G), is the graph whose vertices are labe...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
numbers labeling the vertices of the affine Dynkin diagrams on our pictures). Compare with the results on subgroups of SO(3) we obtained in Problem 3.24. → 5.2 Indecomposable representations of the quivers A1, A2, A3 We have seen that a central question about representations of quivers is whether a certain connected ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
W . ⊃ • � � • A � � W• V• be a complement to the kernel of A in V and be a complement to the image of A in W . Then we can decompose the representation as To decompose this representation, we first let V � let W � follows A V• W• = 0 ker• A •0 � V•� A � � Im•A � •0 0 W• � The first summand is a multiple of t...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
split away �0 �0 . Next, let Y � be a complement of ImB in Y . 0 � � 0 • 0 � � • Y � • 0 which is a multiple of the object 0 A is injective and the map B is surjective (we rename the spaces to simplify notation): �1 . This results in a situation where the map �0 Next, let X = ker(B of A(X) in W such that A(X...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
• W � = • Y • V A � B � � • X � • 0 A(•V ) � � • W � B � � � � • X � Here, the first summand is a multiple of 1 � � �1 � � the second summand can be decomposed into multiples of 0 So, on the whole, this quiver has six indecomposable representations: �1 � � �1 . By splitting away the kernel of B, �1 and 0 �1 �0...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
��rst choose a complement W � Y . Then we can decompose the representation as follows: Y in W , and set V � = W � = W � V , Y � of V ∈ ∈ ∈ � • V � � � � • W � • Y = • V � � � • W � � � • Y The second summand is a multiple of the object 1 � � first summand. Again, to simplify notation, we let �1 � � � � Y ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
other orientation - we get 6 indecomposable representations of A3: 1 0 �0 � �1� 0 , 0 0 , 1 �0 � �1 � 1 , 1 � �1 � � 1 , 0 , 0 �1 � 1 5.3 Indecomposable representations of the quiver D4 As a last - slightly more complicated - example we consider the quiver D4. Example 5.10 (D4). We restrict ourselves ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
a situation where all of the maps A1, A2, A3 are injective. � A1 V A3 � � � �• � � � • V1 � • V3 • 0 0 � � • • 0 0 • 1 A2 • V2 As in 2, we can then identify the spaces V1, V2, V3 with subspaces of V . So we get to the triple of subspaces problem of classifying a triple of subspaces of a given space V . The ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
to simplify notation - we are in a situation where As a next step, we let Y = V1 and set V = V � 1� = V � � • V1 ∈ V1, V2� V � � • ∈ ∈ V1 V2 V = V1 + V2 + V3, V3 = 0. V2 and we choose a complement V � ∈ V2. This yields the decomposition ∈ � • V3 � • V3 V �� � � • • Y • 1�V � = � • 2�V of Y in V su...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
2 = V1 V3 = V2 V3 = 0. ∈ ∈ ∈ (V2 � • Y • 0 � � • V3 V �� � � • • V2 � • V1 V � �• � V3 • � V 1� � � • • V 1� = � • V2 The first of these summands is a multiple of � • 1 • 0 1 � �• • 0 • 0 ∧ By splitting these away we get to a situation where V1 objects of the type V2 V3. Similarly, we can spl...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
implies that V3 = 0. ∈ V3 V1 ∧ � V2. So we get and V1 � V2 = V1 � V3 = V2 � V3 = V. dim V1 = dim V2 = dim V3 = n dim V = 2n. Since V3 V1 ∧ � V2 we can write every element of V3 in the form V3, x � x = (x1, x2), x1 V1, x2 V2. � � We then can define the projections B1 : V3 ⊃ V1, (x1, x2)...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
: V1 decomposition � � V• 1 V •� � V• 2 � � C(1•, 0) � � V• 3 = n � j=1 These correspond to the indecomposable object • 1 � � 2 � � • • 1 • 1 � C(0• , 1) Thus the quiver D4 with the selected orientation has 12 indecomposable objects. If one were to explicitly decompose representations for the oth...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
2. By the definition of the Cartan matrix we get B(x, x) = x T A�x = xi aij xj = 2 � i,j � i 2 xi + � i,j, i=j xi aij xj = 2 � i 2 xi + 2 · � i<j aij xixj which is even. Definition 5.13. A root with respect to a certain positive inner product is a shortest (with respect to this inner product), nonzero vector i...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
Next, let φ be the edge connecting i with the next vertex towards j and i� end of φ. We then let �1, �2 be the graphs obtained from � by removing φ. Since � is supposed to be a Dynkin diagram - and therefore has no cycles or loops - both �1 and �2 will be connected graphs, which are not connected to each other. • • ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
⎨ kiϕi a positive root if all ki 0. A root for which ki 0 ∗ ⊂ Remark 5.18. Lemma 5.16 states that every root is either positive or negative. Example 5.19. 1 can be realized as 1. Then the lattice L = ZN 1. Let � be of the type AN − a subgroup of the lattice ZN by letting L ZN be the subgroup of all vectors (x1...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
0, . . . , 0) = − (ϕi + ϕi+1 + + ϕj 1) − · · · − are the roots of L. Therefore the number of positive roots in L equals N (N 2 − 1) . 2. As a fact we also state the number of positive roots in the other Dynkin diagrams: DN E6 E7 E8 1) − N (N 36 roots 63 roots 120 roots Definition 5.20. Let ϕ � Zn be ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
We are now able to formulate Gabriel’s theorem using roots. Theorem 5.23 (Gabriel’s theorem). Let Q be a quiver of type An, Dn, E6, E7, E8. Then Q has finitely many indecomposable representations. Namely, the dimension vector of any indecomposable representation is a positive root (with respect to B�) and for any pos...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
k = i +F i (V )i = ker ⎧ � : Vi � . Vj ⊃ ⎝ � i j ⊥ � Also, all maps stay the same but those now pointing out of i; these are replaced by compositions of the inclusion of ker � into Vj with the projections Vk. Vj � � ⊃ Definition 5.27. Let Q be a quiver, i the canonical map � Q be a source. Let V be a repr...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
be a source. Then either dim Vi = 1, dim Vj = 0 for j = i or ξ : Vi Vj ⊃ � j i ⊥ is injective. Proof. 1. Choose a complement W of Im�. Then we get • V = 0 W � � � � � � • • 0 • 0 V � � Since V is indecomposable, one of these summands has to be zero. If the first summand is zero, then � has to be surjective. I...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
ourselves to showing that the spaces of V and Fi−F +V are the same. It is enough to do so for the i-th space. Let ⊃ i � : � i j ⊥ Vj Vi ⊃ 91 ⇒ ⇒ be surjective and let K = ker �. When applying F + i , the space Vi gets replaced by K. Furthermore, let After applying Fi−, ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
0. i � : � i j ⊥ Vj Vi ⊃ So we can assume that � is surjective. In this case, assume that F V is decomposable as + i with X, Y = 0. But F V is injective at i, since the maps are canonical projections, whose direct sum is the tautological embedding. Therefore X and Y also have to be injective at i and hence (by ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
dim K = dim Vj � i j ⊥ dim Vi. − d(F +V ) i − d(V ) i � ⎩ = dim Vj � i j ⊥ 2 dim Vi = − − B (d(V ), ϕi) and This implies ⎩ d(Fi +V ) − j = 0, j = i. d(V ) � +V ) d(Fi d(F +V ) = d(V ) − i − ⊆ d(V ) = B (d(V ), ϕi) ϕi − B (d(V ), ϕi) ϕi = si (d(V )) . 5.7 Coxeter elements Definition 5.32. Let Q ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
one of the elements must have at least one strictly negative one. Furthermore, it is enough to show that 1 is not an eigenvalue for c, since cα, c2α, . . . , cM 1α − ≥ cw = c ⎩ 1 + c + c + � (1 + c + c 2 + 2 + c M · · · 1 − · · · + c M 1)v = w = 0 − 2 v = (c + c + c + 3 · · · + c M 1 + 1)v = w. − Assume th...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
a sink of the remaining quiver and so on. This way we create a labeling of the desired kind. We now consider the sequence V (0) = V, V (1) = F + n V, V (2) = F + F + n − 1 n V, . . . This sequence is well defined because of the selected labeling: n has to be a sink of Q, n 1 has to be a sink of Qn (where Qn ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
indefinitely - since d may not have any negative entries. Let i be smallest number such that V (i) is not surjective at the appropriate vertex. By Proposition ⎩ 5.30 it is indecomposable. So, by Proposition 5.28, we get � V (i) for some p. d(V (i)) = ϕp We are now able to prove Gabriel’s theorem. Namely, we get th...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
V � (0). F −F − . . . F −V i = n 1 n k − Fn−F − . . . F −F + . . . F + Fn + 1 n n 1 k k − − + + . . . F n +V � 1 . . . F k−Fk Fn−F n− 1Fn − − V (0) = V (0) (0) = V � = V (0) = V � � 95 These two corollaries show that there are only finitely many indecomposable representations (since there a...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
functors work. Consider the quiver D4 with the orientation of all arrows towards the node (which is labeled by 4). Start with the 1-dimensional representation V�4 sitting at the 4-th vertex. Apply to V�4 the functor F3−F2−F1−. This yields F1−F2−F3−V�4 = V�1+�2+�3+�4 . Now applying F4− we get F4−F1−F2−F3−V�4 = V�1...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
by exchanging V with W and A with B. 96 3) Hn: V = Cn with basis vi, W = Cn 1 with basis wi, Avi = wi, Bwi = vi+1 for i < n, and − Avn = 0. 4) Kn is obtained from Hn by exchanging V with W and A with B. Show that these are indecomposable and pairwise nonisomorphic. (b) Show that if E is a representation of Q2 su...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
classification to Qn, n > 2, with any orientation? Problem 5.40. Let L or all half-integers (but not integers), and the sum of all coordinates is an even integer. 1 Z8 be the lattice of vectors where the coordinates are either all integers 2 → (a) Let ϕi = ei of L (over Z). − ei+1, i = 1, ..., 6, ϕ7 = e6 + e7, ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
else. (a) Show that if i is a source then Ext1(V, V�i ) = 0 for any representation V of Q, and if i is a sink, then Ext1(V�i , V ) = 0. (b) Given an orientation of the quiver, find a Jordan-H¨older series of V� for that orientation. 97 ⇒ 6 Introduction to categories 6.1 The definition of a category We have now ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf
write f : X C Y ); ⊃ (iii) For any objects X, Y, Z (f, g) f ∞ �⊃ g, Ob( C � ), a composition map Hom(Y, Z) × Hom(X, Y ) ⊃ Hom(X, Z), which satisfy the following axioms: 1. The composition is associative, i.e., (f g) ∞ ), there is a morphism 1X ∞ h = f (g ∞ ∞ h); 2. For each X Ob( f = f and g ...
https://ocw.mit.edu/courses/18-712-introduction-to-representation-theory-fall-2010/24d8b3fa2ce48e48ee6c2d8d5e3562f6_MIT18_712F10_replect.pdf