Canonical systems of basic invariants for unitary reflection groups

Similar documents
Longest element of a finite Coxeter group

NOTES ON POINCARÉ SERIES OF FINITE AND AFFINE COXETER GROUPS

Generic section of a hyperplane arrangement and twisted Hurewicz maps

ALGEBRA QUALIFYING EXAM PROBLEMS LINEAR ALGEBRA

arxiv: v1 [math.rt] 11 Sep 2009

A PIERI RULE FOR HERMITIAN SYMMETRIC PAIRS. Thomas J. Enright, Markus Hunziker and Nolan R. Wallach

Background on Chevalley Groups Constructed from a Root System

A 2 G 2 A 1 A 1. (3) A double edge pointing from α i to α j if α i, α j are not perpendicular and α i 2 = 2 α j 2

MAT 445/ INTRODUCTION TO REPRESENTATION THEORY

arxiv: v1 [math.ac] 8 Jun 2010

A finite universal SAGBI basis for the kernel of a derivation. Osaka Journal of Mathematics. 41(4) P.759-P.792

FORMAL GROUPS OF CERTAIN Q-CURVES OVER QUADRATIC FIELDS

MATH Linear Algebra

Some notes on Coxeter groups

GEOMETRIC STRUCTURES OF SEMISIMPLE LIE ALGEBRAS

Linear Algebra 2 Spectral Notes

Math Linear Algebra

H A A}. ) < k, then there are constants c t such that c t α t = 0. j=1 H i j

Generalized Alexander duality and applications. Osaka Journal of Mathematics. 38(2) P.469-P.485

Representation Theory. Ricky Roy Math 434 University of Puget Sound

ne varieties (continued)

ON REGULARITY OF FINITE REFLECTION GROUPS. School of Mathematics and Statistics, University of Sydney, NSW 2006, Australia

LIMITING CASES OF BOARDMAN S FIVE HALVES THEOREM

Topics in linear algebra

Title. Author(s)Morita, Hideaki; Watanabe, Junzo. CitationHokkaido University Preprint Series in Mathematics, Issue Date DOI 10.

ON THE BETTI NUMBERS OF FILIFORM LIE ALGEBRAS OVER FIELDS OF CHARACTERISTIC TWO

THE STRONG TOPOLOGICAL MONODROMY CONJECTURE FOR COXETER HYPERPLANE ARRANGEMENTS

FORMALITY OF THE COMPLEMENTS OF SUBSPACE ARRANGEMENTS WITH GEOMETRIC LATTICES

Noetherian property of infinite EI categories

NOTES ON LINEAR ALGEBRA OVER INTEGRAL DOMAINS. Contents. 1. Introduction 1 2. Rank and basis 1 3. The set of linear maps 4. 1.

On Riesz-Fischer sequences and lower frame bounds

Reducibility of generic unipotent standard modules

Math 350 Fall 2011 Notes about inner product spaces. In this notes we state and prove some important properties of inner product spaces.

Title. Author(s)Morita, Hideaki; Wachi, Akihito; Watanabe, Junzo. CitationHokkaido University Preprint Series in Mathematics, Issue Date

Math 396. An application of Gram-Schmidt to prove connectedness

5 Quiver Representations

THE LIE ALGEBRA sl(2) AND ITS REPRESENTATIONS

INTRODUCTION TO LIE ALGEBRAS. LECTURE 10.

Math 121 Homework 4: Notes on Selected Problems

Group Gradings on Finite Dimensional Lie Algebras

Splitting criterion for reflexive sheaves

arxiv: v1 [math.rt] 14 Nov 2007

Honors Algebra 4, MATH 371 Winter 2010 Assignment 4 Due Wednesday, February 17 at 08:35

Math 396. Quotient spaces

Linear algebra 2. Yoav Zemel. March 1, 2012

Problems in Linear Algebra and Representation Theory

Projective Schemes with Degenerate General Hyperplane Section II

THE LARGEST INTERSECTION LATTICE OF A CHRISTOS A. ATHANASIADIS. Abstract. We prove a conjecture of Bayer and Brandt [J. Alg. Combin.

Topics in Representation Theory: Fourier Analysis and the Peter Weyl Theorem

L(C G (x) 0 ) c g (x). Proof. Recall C G (x) = {g G xgx 1 = g} and c g (x) = {X g Ad xx = X}. In general, it is obvious that

CHAPTER 6. Representations of compact groups

Bulletin of the Iranian Mathematical Society

REPRESENTATION THEORY NOTES FOR MATH 4108 SPRING 2012

Root systems. S. Viswanath

LECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI. 1. Maximal Tori

Euler characteristic of the truncated order complex of generalized noncrossing partitions

Non-separable AF-algebras

16.2. Definition. Let N be the set of all nilpotent elements in g. Define N

Lecture Notes Introduction to Cluster Algebra

REPRESENTATION THEORY OF S n

TITS SYSTEMS, PARABOLIC SUBGROUPS, PARABOLIC SUBALGEBRAS. Alfred G. Noël Department of Mathematics Northeastern University Boston, MA

The Waring rank of the Vandermonde determinant

On splitting of the normalizer of a maximal torus in groups of Lie type

Chapter 2 Linear Transformations

Representation Theory

MATH 223A NOTES 2011 LIE ALGEBRAS 35

On the singular elements of a semisimple Lie algebra and the generalized Amitsur-Levitski Theorem

A note on Samelson products in the exceptional Lie groups

LECTURE VI: SELF-ADJOINT AND UNITARY OPERATORS MAT FALL 2006 PRINCETON UNIVERSITY

A PRIMER ON SESQUILINEAR FORMS

Auerbach bases and minimal volume sufficient enlargements

Radon Transforms and the Finite General Linear Groups

ON PARABOLIC CLOSURES IN COXETER GROUPS

LECTURE NOTES AMRITANSHU PRASAD

Algebra II. Paulius Drungilas and Jonas Jankauskas

Linear Algebra. Min Yan

FINITE REGULARITY AND KOSZUL ALGEBRAS

Since G is a compact Lie group, we can apply Schur orthogonality to see that G χ π (g) 2 dg =

The Morozov-Jacobson Theorem on 3-dimensional Simple Lie Subalgebras

Real, Complex, and Quarternionic Representations

A Z N -graded generalization of the Witt algebra

SYMPLECTIC GEOMETRY: LECTURE 5

SELF-DUAL HOPF QUIVERS

How to sharpen a tridiagonal pair

On the Rothenberg Steenrod spectral sequence for the mod 3 cohomology of the classifying space of the exceptional Lie group E 8

MAT 5330 Algebraic Geometry: Quiver Varieties

Cartan s Criteria. Math 649, Dan Barbasch. February 26

arxiv:math/ v3 [math.qa] 16 Feb 2003

REPRESENTATIONS OF U(N) CLASSIFICATION BY HIGHEST WEIGHTS NOTES FOR MATH 261, FALL 2001

Contact trivialization of ordinary differential equations 1

DEFORMATIONS OF ALGEBRAS IN NONCOMMUTATIVE ALGEBRAIC GEOMETRY EXERCISE SHEET 1

On the Rothenberg Steenrod spectral sequence for the mod 3 cohomology of the classifying space of the exceptional Lie group E 8

THE THEOREM OF THE HIGHEST WEIGHT

algebras Sergey Yuzvinsky Department of Mathematics, University of Oregon, Eugene, OR USA August 13, 1996

Math 225B: Differential Geometry, Final

arxiv: v1 [math.gr] 8 Nov 2008

A method for construction of Lie group invariants

REMARKS ON REFLEXIVE MODULES, COVERS, AND ENVELOPES

arxiv:math/ v1 [math.ac] 24 Nov 2006

SELF-DUAL NORMAL BASES AND TRACE FORMS OF GALOIS ALGEBRAS E.

Transcription:

Canonical systems of basic invariants for unitary reflection groups Norihiro Nakashima, Hiroaki Terao and Shuhei Tsujie Abstract It has been known that there exists a canonical system for every finite real reflection group. The first and the third authors obtained an explicit formula for a canonical system in the previous paper. In this article, we first define canonical systems for the finite unitary reflection groups, and then prove their existence. Our proof does not depend on the classification of unitary reflection groups. Furthermore, we give an explicit formula for a canonical system for every unitary reflection group. Key Words: groups. basic invariants; invariant theory; finite unitary reflection 2010 Mathematics Subject Classification: Primary 13A50; Secondary 20F55. 1 Introduction Let V be an n-dimensional unitary space, and W U(V ) a finite unitary reflection group. Each reflection fixes a hyperplane in V pointwise. Let S denote the symmetric algebra S(V ) of the dual space V, and S k the vector space consisting of homogeneous polynomials of degree k together with the zero polynomial. Then W acts contravariantly on S by (w f)(v) = f(w 1 v) for v V, w W and f S. The action of W on S preserves the degree of homogeneous polynomials, and W acts also on S k. The subalgebra R = S W of W -invariant polynomials of S email: nakashima@toyota-ti.ac.jp email: hterao00@za3.so-net.ne.jp email: tsujie@math.sci.hokudai.ac.jp 1

is generated by n algebraically independent homogeneous polynomials by Chevalley [2]. A system of such generators is called a system of basic invariants of R. Let x 1,..., x n be an orthonormal basis for V, and 1,..., n the basis for V dual to x 1,..., x n. The symmetric algebra of V acts naturally on S as differential operators (e.g., Kane [8, 25-2]). Let c denote the complex conjugate of c C. For f = a c ax a S, a differential operator f is defined by f := f( ) := a c a a, (1.1) where a = (a 1,..., a n ) Z n 0, c a C, x a = x a 1 1 x an n, and a = a 1 1 an n. Note that (cf) = cf, w (f ) = (w f) and w (f g) = (w f) (w g) for c C, w W, f, g S. Flatto and Wiener introduced canonical systems to solve a mean value problem related to vertices for polytopes in [3, 4, 5]. They proved that there exists a canonical system for every finite real reflection group. Later in [7], Iwasaki gave a new definition of the canonical systems as well as explicit formulas for canonical systems for some types of reflection groups. The first and the third authors, in their previous work [9], obtained an explicit formula for a canonical system for every reflection group. In this article, we extend the definition of canonical systems to the finite unitary reflection groups as follows. Definition 1.1. A system {f 1,..., f n } of basic invariants is said to be canonical if it satisfies the following system of partial differential equations: for i, j = 1,..., n, where δ ij is the Kronecker delta. Our main result is the following existence theorem. f i f j = δ ij (1.2) Theorem 1.2. There exists a canonical system for every finite unitary reflection group. Our proof of Theorem 1.2 is classification free. Furthermore, we give an explicit formula (Theorem 4.3) for a canonical system. The organization of this article is as follows. In Section 2, we introduce Lemma 2.2 which will play an important role in Section 3 when we prove the existence theorem 1.2. In Section 4, we give an explicit formula for a canonical system. 2

2 Basic invariants Let R + be the ideal of R generated by homogeneous elements of positive degrees, and I = SR + the ideal of S generated by R +. We define a unitary inner product, : S S C by f, g = f g x=0 = f( )g x=0 (f, g S), (2.1) where x = (x 1,..., x n ) and = ( 1,..., n ). Let e H be the order of the cyclic group generated by the reflection s H W corresponding to a reflecting hyperplane H. Fix L H V satisfying ker L H = H. Let denote the product of L e H 1 H as H runs over the set of all reflecting hyperplanes. Then is skew-invariant, i.e., w = (det w) for any w W. Set The following lemma is obtained by Steinberg [12]. H := {f f S}. (2.2) Lemma 2.1. Let f S be a homogeneous polynomial. Then we have the following: (1) f I if and only if f = 0, (2) g f = 0 for any g I if and only if f H. It follows from Lemma 2.1 (2) that I is the orthogonal complement of H with respect to the inner product (2.1) degreewise. In the rest of this paper, we assume that W acts on V irreducibly. We fix a W -stable graded subspace U of S such that S = I U. It has been known that the U is isomorphic to the regular representation of W (see Bourbaki [1, Chap. 5 5 Theorem 2].) Hence the multiplicity of V in U is equal to dim C V = n. Let π : S U be the second projection with respect to the decomposition S = I U. Then π is a W -homomorphism. Let {h 1,..., h n } be a system of basic invariants with deg h 1 deg h n. The multiset of degrees m i := deg h i (i = 1,..., n) does not depend on a choice of basic invariants. There exists a unique linear map d : S S C V satisfying d(fg) = fd(g) + gd(f) for f, g S and dl := 1 L C C V for L V. The map d is called the differential map. The differential 1-form dh is expressed as dh = j h x j = 3 ( j h)dx j

for h S. Note that dh is invariant if h is invariant. Define a W -homomorphism by ε : (S C V ) W R + ( ) ε h j dx j = x j h j. Then ε d(h) = (deg h)h for any homogeneous polynomial h. The projection π : S U is extended to a W -homomorphism π : (S V ) W (U V ) W defined by π( n g j x j ) := n π(g j) x j. Lemma 2.2. Let {h 1,..., h n } be a system of basic invariants. Put f i := (ε π)(dh i ), and {f 1,..., f n } is a system of basic invariants. Proof. Since h 1,..., h n are invariants, so are the 1-forms dh 1,..., dh n. Thus each f i is invariant because both ε and π are W -homomorphisms. Next we prove that {f 1,..., f n } is a system of basic invariants. Define f ij := π( j f i ). Then f i = n x jf ij. For j = 1,..., n, we express j h i = f ij + r ij for some r ij I. Then r ij = l k=1 h kg ijk for some g ijk S. Put r i := n x jr ij for i = 1,..., n. Then we have m i h i = x j j h i = f i + r i. Since f i is invariant, the polynomial r i = m i h i f i is also invariant. This implies ( l ) r i = r i = x j g i,j,k h k I 2 R, k=1 where denotes the averaging operator, i.e., f = 1 W w f for f S. Thus we have j r i I for i, j {1,..., n}. Let J(g 1,..., g n ) denote the Jacobian for g 1,..., g n S. Then w W J(m 1 h 1,..., m n h n ) = det[ j h i ] i,j = det[ j f i + j r i ] i,j det[ j f i ] i,j = J(f 1,..., f n ) (mod I). 4

It immediately follows that / I by Lemma 2.1 (1). Since J(h 1,..., h n ) is a nonzero constant multiple of, we obtain J(f 1,..., f n ) / I, and thus J(f 1,..., f n ) 0. By the Jacobian criterion (e.g., [6, Proposition 3.10]), {f 1,..., f n } is algebraically independent. Therefore {f 1,..., f n } is a system of basic invariants because deg f i = deg h i for i = 1,..., n. Remark. There exists a W -stable subspace U of S such that S = I U and df 1,..., df n (U C V ) W. However, we do not know whether U coincides with U or not. In section 3, we see that U and U coincide when U = H. 3 Existence of a canonical system In this section, we prove Theorem 1.2 which is the existence theorem of a canonical system. The following lemma is widely known. Lemma 3.1. Let g S be a homogeneous polynomial, and put g j := j g for j = 1,..., n. Then, for any h S, we have g (x j h) = x j g h + g j h. (3.1) Proof. We only need to verify the assertion when g is a monomial. We verify it by induction on deg g. Let a = (a 1,..., a n ) be a multi-index with a = deg g. Then a (x j h) = a e j j (x j h) = a e j h + a e j (x j j h) = a e j h + ( x j a e j j h + (a j 1) a 2e j j h ) = x j a h + a j a e j h. By Lemma 2.1, I is the orthogonal complement of H with respect to the inner product (2.1), and the W -stable graded space S is decomposed into the direct sum of the W -stable graded subspaces I and H, i.e., S = I H. Let π : S H be the second projection with respect to the decomposition S = I H. Let h 1,..., h n be an arbitrary system of basic invariants. Put f ij := π( j h i ) for i, j = 1,..., n, and f i := (ε π)(dh i ) = n x jf ij for i = 1,..., n. Then {f 1,..., f n } is a system of basic invariants by Lemma 2.2. We are now ready to give a proof of Theorem 1.2. 5

Let g R + be a homogeneous invariant polynomial with deg g < m i. By using Lemma 2.1 and Lemma 3.1 we obtain ( ) g f i = g (x j f ij ) = xj g f ij + gj f ij = gj f ij H. Meanwhile, g f i is an invariant polynomial of positive degree since g and f i are invariant and deg g < m i. Therefore we have g f i H I = {0}. In particular, when g = f j with deg f j < m i, we have fj f i = 0. It immediately follows that fj f i = 0 if deg f j > deg f i. Applying the Gram-Schmidt orthogonalization with respect to the inner product (2.1), we obtain a canonical system of basic invariants. This completes our proof of Theorem 1.2. The subspace spanned by a canonical system can be characterized as follows: Proposition 3.2. Let {f 1,..., f n } be a canonical system and F := f 1,..., f n C. Then (1) F = k=1 {f R k g f = 0 for g R l with 0 < l < k}, where R k := R S k, (2) df 1,..., df n C = (H C V ) W, (3) F = ε((h C V ) W ). Proof. Define G := {f R k g f = 0 for g R l with 0 < l < k}. k=1 Let f G be a homogeneous polynomial. For any g I, it is not hard to see that g ( j f) = j (g f) = 0. Thus we have j f H for j = 1,..., n by Lemma 2.1. This implies d(g) (H C V ) W. The inclusion F G follows immediately because {f 1,..., f n } is a canonical system. Hence we have the following commutative diagram: G d (H C V ) W F d df 1,..., df n C. (3.2) 6

Since ker(d) = C and G does not contain any nonzero constant, the horizontal maps d are both injective. Recall that V is an irreducible representation and that H affords the regular representation of W. Hence we have dim(h C V ) W = dim V = n because (H C V ) W Hom W (V, H) (e.g., [10] or [11, Lemma 6.45]). By comparing the dimensions, we have F = G, which is (1). Sending both sides of this equality by d, we obtain df 1,..., df n C = d(f) = d(g) = (H C V ) W. (3.3) So the equality (2) is proved. Moreover, we have by applying ε to (3.3). This verifies (3). f 1,..., f n C = F = G = ε((h C V ) W ) (3.4) 4 An explicit construction of a canonical system The following is a key to our explicit formula for a canonical system. Definition 4.1 (c.f. [9]). Define a linear map ϕ : S H by ϕ(f) := (f ) for f S. The map ϕ induces a W -homomorphism defined by ϕ( f x) := ϕ(f) x. One has ϕ : (S V ) W (H V ) W w ϕ(f) = ((w f) (w )) (w ) = ((w f) (det(w) )) (det(w) ) =det(w) det(w)((w f) ) ( ) = ϕ(w f) for w W and f S. Therefore ϕ is a W -homomorphism, and so is ϕ. Let {h 1,..., h n } be an arbitrary system of basic invariants, and assume deg h i = m i for i = 1,..., n. Let {f 1,..., f n } be a canonical system with deg f i = m i. We have already shown in Proposition 3.2 (1) that (H V ) W = df 1,..., df n C. 7

Lemma 4.2.. The restriction is isomorphic. ϕ dh1,...,dh n C : dh 1,..., dh n C (H V ) W = df 1,..., df n C Proof. It is enough to prove the injectivity. Fix h h 1,..., h n C with ϕ(dh) = 0. It follows from Lemma 2.1 that ker ϕ = (I C V ) W. Then we have dh (I C V ) W. At the same time, since {f 1,..., f n } is a system of basic invariants, we may write h = λ k f k + P, k=1 where λ k C and P I 2 R. Then the 1-form dp lies in (I C V ) W, and df k (H C V ) W for k = 1,..., n by Proposition 3.2. Hence we have λ k df k = dh dp (H C V ) W (I C V ) W = {0}. k=1 This implies λ k = 0 for all k = 1,..., n since {df 1,..., df n } is linearly independent over C. Thus we have h = P I 2 R. The algebraic independence of h 1,..., h n implies h 1,..., h n I 2 = {0}. Therefore h = 0. The image of ϕ dh1,...,dh n C coincides with df 1,..., df n C by Lemma 4.2. Therefore we have a chain of the linear maps: h 1,..., h n C d dh 1,..., dh n C ϕ df1,..., df n C ε f 1,..., f n C. (4.1) The image of {h 1,..., h n } by the composition of all the maps in (4.1) forms a basis for f 1,..., f n C. Thus we have the following explicit formula for a canonical system of basic invariants. Theorem 4.3 (c.f. [9]). Let h 1,..., h n be an arbitrary system of basic invariants. Applying the Gram-Schmidt orthogonalization to { } ε ϕ(dh i ) = x j ϕ( j h i ) i = 1,..., n with respect to the inner product (2.1), we obtain a canonical system of basic invariants. 8

References [1] N. Bourbaki, Groupes et Algèbres de Lie, Chapitres 4, 5 et 6, Hermann, Paris, (1968). [2] C. Chevalley, Invariants of finite groups generated by reflections, Amer. J. Math, 77, 778-782, (1955). [3] L. Flatto, Basic sets of invariants for finite reflection groups, Bull. Amer. Math. Soc. 74, 730-734, (1968). [4] L. Flatto, Invariants of finite reflection groups and mean value problems. II, Amer. J. Math. 92, 552-561, (1970). [5] L. Flatto and M. M. Wiener, Invariants of finite reflection groups and mean value problems, Amer. J. Math. 91, 591-598, (1969). [6] J. E. Humphreys, Reflection Groups and Coxeter Groups, Cambridge Univ. Press, Cambridge, New York (1990). [7] K. Iwasaki, Basic invariants of finite reflection groups. J. Algebra. 195, 538-547, (1997). [8] R. Kane, Reflection groups and invariant theory, CMS Books in Mathematics/Ouvrages de Mathématiques de la SMC, 5, Springer-Verlag, New York, (1997). [9] N. Nakashima and S. Tsujie, A canonical system of basic invariants of a finite reflection group, J. Algebra, 406 (2014), 143-153. [10] P. Orlik and L. Solomon, Unitary reflection groups and cohomology, Invent. Math. 59, 77-94, (1980). [11] P. Orlik and H. Terao, Arrangements of Hyperplanes. Grundlehren dermatematischen Wissenschaften 300, Springer-Verlag, 1992. [12] R. Steinberg, Differential equations invariant under finite reflection groups, Trans. Amer. Math. Soc. 112, 392-400, (1964). Norihiro Nakashima Department of Electronics and Information Science, Toyota Technological Institute, Nagoya, 468-8511, Japan 9

Hiroaki Terao Department of Mathematics, Hokkaido University, Sapporo, 060-0810, Japan Shuhei Tsujie Department of Mathematics, Hokkaido University, Sapporo, 060-0810, Japan 10