Startseite Conjugacy classes of centralizers in unitary groups
Artikel Öffentlich zugänglich

Conjugacy classes of centralizers in unitary groups

  • Sushil Bhunia EMAIL logo und Anupam Singh
Veröffentlicht/Copyright: 11. Oktober 2018

Abstract

Let G be a group. Two elements x,yG are said to be in the same z-class if their centralizers in G are conjugate within G. Consider 𝔽 a perfect field of characteristic 2, which has a non-trivial Galois automorphism of order 2. Further, suppose that the fixed field 𝔽0 has the property that it has only finitely many field extensions of any finite degree. In this paper, we prove that the number of z-classes in the unitary group over such fields is finite. Further, we count the number of z-classes in the finite unitary group Un(q), and prove that this number is the same as that of GLn(q) when q>n.

1 Introduction

Let G be a group. Two elements x and yG are said to be z-equivalent, denoted as xzy, if their centralizers in G are conjugate, i.e., 𝒵G(y)=g𝒵G(x)g-1 for some gG, where 𝒵G(x) denotes the centralizer of x in G. Clearly, z is an equivalence relation on G. The equivalence classes with respect to this relation are called z-classes. It is easy to see that if two elements of a group G are conjugate, then their centralizers are conjugate thus they are also z-equivalent. However, in general, the converse is not true. We are interested in reductive linear algebraic groups, where a group may have infinitely many conjugacy classes but finitely many z-classes. In geometry, z-classes describe the behavior of dynamical types. That is, if a group G is acting on a manifold M, then understanding (dynamical types of) orbits is related to understanding (conjugacy classes of) centralizers. In this paper, we explore this topic for certain classical groups. Steinberg (see [25, Section 3.6, Corollary 1 to Theorem 2]) proved that for a reductive algebraic group G defined over an algebraically closed field, of good characteristic, the number of z-classes is finite (even though there could be infinitely many conjugacy classes). Thus, it is natural to ask how far “finiteness of z-classes” holds true for algebraic groups defined over a base field. This is certainly not true even for GL2 over the field (see Section 5). Thus we need to restrict to certain kind of fields.

Definition 1 (Property FE).

A perfect field 𝔽 of characteristic 2 has the property FE if 𝔽 has only finitely many field extensions of any finite degree.

Examples of such fields are: any algebraically closed field (for example, ), the field of real numbers , local fields (e.g., p-adics p) and finite fields 𝔽q. In [16] for GLn and in [11] for orthogonal groups O(V,B) and symplectic groups Sp(V,B), it is proved that over a field with the property FE these groups have only finitely many z-classes. In this paper, we extend this result to the unitary groups. We prove the following result:

Theorem 2.

Let 𝔽 be a field with a non-trivial Galois automorphism of order 2 and fixed field 𝔽0. Let V be a finite-dimensional vector space over 𝔽 with a non-degenerate hermitian form B. Suppose that the fixed field 𝔽0 has the property FE. Then the number of z-classes in the unitary group U(V,B) is finite.

This theorem is proved in Section 3.2.

If we look at the character table of SL2(q) (for example see [2] or [19]) we notice that the conjugacy classes and irreducible characters are grouped together. One observes a similar pattern in the work of Srinivasan [23] for Sp4(q). In [12], Green studied the complex representations of GLn(q), where he introduced the function t(n) for the “types of characters/classes” (towards the end of Section 1 on pages 407–408) which is the number of z-classes in GLn(q). He observed the following:

“The number t(n) appears as the number of rows or columns of a character table of GLn(q). This is because the irreducible characters, which by a well-known theorem of representation theory are the same in number as the conjugacy classes, themselves collect into types in a corresponding way, and the values of all the characters of a given type at all the classes of a given type can be included in a single functional expression.” [12, p. 408]

In Deligne–Lusztig theory, one studies the representation theory of finite groups of Lie type, and the z-classes of semisimple elements in the dual group play an important role. In [14, Section 8.11], Humphreys defined genus of an element in algebraic group G over 𝔽. Two elements have the same genus if they are z-equivalent in G(𝔽) and the genus number (respectively semisimple genus number) is the number of z-classes (respectively the number of z-classes of semisimple elements). Thus understanding z-classes for finite groups of Lie type, especially semisimple genus, and counting them, is of importance in representation theory (see [6, 7, 9, 10]). Bose, in [3], calculated the genus number for simply connected simple algebraic groups over an algebraically closed field and compact simple Lie groups. Classification of z-classes in U(n,1), the isometry group of the n-dimensional complex hyperbolic space is done in [5]. The second named author studied z-classes for the compact group of type G2 in [21]. In this paper, we count the z-classes in complex hyperbolic groups U(n,1) and in finite unitary groups. The main theorem is as follows (for proof see Section 4.4):

Theorem 3.

The number of z-classes in Un(q) is the same as the number of z-classes in GLn(q), when q>n. Thus, the number of z-classes for either group can be read off by looking at the coefficients of the function i=1z(xi), where z(x)=j=11(1-xj)p(j).

However, the above statement need not be true when qn. We mention this in Example 3.

2 Conjugacy classes and centralizers in unitary groups

In this section, we introduce the unitary groups. We begin with a more general definition of hermitian forms, following [20, Chapter 7], than what is available in [13] or in other textbooks on the subject of classical groups over a field. This is required for the description of conjugacy classes. Let R be a commutative ring with a non-trivial involution σ which, to simplify notation, we denote by a¯=σ(a). The subring of R fixed by σ is denoted by R0. Let V be a finitely generated projective module over R. A hermitian form on V is a sesquilinear map B:V×VR, satisfying

B(u,v)=B(v,u)¯

for all u,vV. The pair (V,B) is called a hermitian space. One can define when two hermitian spaces are equivalent (which is given in terms of an isometry defined in [20, Chapter 7, Definition 2.1 (iv)]). We list some results on the classification of hermitian forms which will be required later in this paper. The following result follows from the main theorem in [15].

Proposition 1.

Let 𝔽 be a field with a non-trivial Galois automorphism of order 2. Suppose 𝔽0 has the property FE and V is a finite-dimensional vector space over 𝔽. Then there are only finitely many non-equivalent hermitian forms on V.

Proof.

From Jacobson’s theorem (see [15, Theorem]), the classification of hermitian forms over 𝔽 is the same as the classification of symmetric bilinear forms over 𝔽0. Since symmetric bilinear forms can be diagonalised where the non-zero entries belong to 𝔽0×/𝔽0×2, which is known to be finite (as 𝔽0×/𝔽0×2 determines the distinct degree 2 field extensions of 𝔽0 which is finite as 𝔽0 has the property FE), this gives the required result. ∎

We need to understand Hermitian forms on a module V over ring A=𝔽×𝔽, where 𝔽 is a field. We consider A as an algebra over 𝔽 with diagonal embedding and the “switch” involution on A given by (a,b)(b,a). Then we have orthogonal idempotents e1=(1,0),e2=(0,1) in A satisfying e1+e2=1 and e1e2=0. We decompose V=V1V2, where V1=e1V and V2=e2V. Clearly, V1 and V2 are vector spaces over 𝔽, say, of dimension n and m respectively. Then:

Proposition 2.

With notation as above, any hermitian form on A-module V, up to equivalence, is determined by the Smith normal form (equivalently the rank) of an n×m matrix over 𝔽.

Proof.

For convenience, fix a basis of V1 and V2 as {ϵ1,,ϵn} and {δ1,,δm}, respectively, which together give a generating set for the A-module V. Let B be a sesquilinear form on V. Then, using orthogonality of idempotents we get, B(vi,vi)=0 for viVi. Thus, B is determined by the values B(ϵi,δj) and B(δj,ϵi) for all i and j. Further, if B is a hermitian form, then B is determined by the values B(ϵi,δj), an n×m matrix over A. That is, B is determined by its restriction on V1×V2, say by a matrix βMn×m(A). Hence, the matrix of B would look like

(0ββ¯t0).

We can also check that any isomorphism P of V will be given by (P100P2), where P1GL(V1) and P2GL(V2). To get the equivalence of forms we compute PtBP¯ and get P1tβP¯2. Thus, β is determined by its Smith-normal form. The converse can be easily checked by an explicit construction. ∎

Usually, to define the unitary group we begin with a field 𝔽 and a non-trivial Galois automorphism σ of order 2 on it. We consider only non-degenerate hermitian forms. An isometry of (V,B) is a linear map gGL(V) such that

B(u,v)=B(g(u),g(v))

for all u,vV. Such maps are called unitary transformations and the set of all such transformations is called the unitary groupU(V,B). There could be more than one hermitian form, up to equivalence, over a given field and similarly more than one non-isomorphic unitary group. For example, when 𝔽= with conjugation, then the hermitian forms are given by signature. However, over a finite field, there is a unique hermitian form (see [13, Corollary 10.4]). We discuss some of the cases in Section 4.

To study z-classes, it is important to understand the conjugacy classes first. This has been well understood for classical groups through the work of Asai, Ennola, Macdonald, Milnor, Springer-Steinberg, Wall, Williamson [1, 8, 17, 18, 22, 27, 28] and many others. Since the unitary group is a subgroup of GLn(𝔽), one hopes to exploit the theory of canonical forms to get the conjugacy classes in the unitary group. For our exposition, we follow Springer and Steinberg [22]. We begin by recalling notation involved in the description of conjugacy classes.

2.1 Self-U-reciprocal polynomials

Let f(x)=i=0daixi be a polynomial in 𝔽[x] of degree d. We extend the involution on 𝔽 to that of 𝔽[x] by

f¯(x):=i=0dai¯xi.

Let f(x) be a polynomial with f(0)0. The corresponding U-reciprocal polynomial of f(x) is a degree d polynomial defined by

f~(x):=f¯(0)-1xdf¯(x-1).

A monic polynomial f(x) with a non-zero constant term is said to be self-U-reciprocal if f(x)=f~(x). In terms of roots, it means that for a self-U-reciprocal polynomial, whenever λ is a root, λ¯-1 is also a root with the same multiplicity. Note that

f(x)=f~~(x),

and if f(x)=f1(x)f2(x), then f~(x)=f1~(x)f2~(x). Also, f(x) is irreducible if and only if f~(x) is irreducible. In the case of f(x)=(x-λ)n, the polynomial f(x) is self-U-reciprocal if and only if λλ¯=1. Over a finite field, we have the following result due to Ennola (see [8, Lemma 2]):

Proposition 3.

Let f(x) be a monic, irreducible, self-U-reciprocal polynomial over a finite field 𝔽q2. Then the degree of f(x) is odd.

Let TGL(V) and let f(x) be its minimal polynomial; then f~(x) is the minimal polynomial of T¯-1. If TU(V,B), then its minimal polynomial is monic with a non-zero constant term and is self-U-reciprocal. Let f(x) be a self-U-reciprocal polynomial. We can write it as follows:

(2.1)f(x)=i=1k1pi(x)mij=1k2(qj(x)qj~(x))nj,

where pi(x) is irreducible, self-U-reciprocal, and qj(x) is irreducible, not self-U-reciprocal for all i and j.

2.2 Space decomposition with respect to a unitary transformation

Let TU(V,B) and let f(x) be its minimal polynomial. Write f(x) as in equation (2.1). This gives a primary decomposition of V. Furthermore, we have the following:

Proposition 4.

The direct sum decomposition

V=iker(fi(T)si),

where either fi(x)=pi(x) and si=mi or fi(x)=qi(x)q~i(x) and si=ni, is a decomposition into non-degenerate mutually orthogonal T-invariant subspaces.

The proof of this is similar to the orthogonal case as in [11, Section 3] and hence we skip the details. This decomposition helps us reduce the questions about conjugacy classes and z-classes of a unitary transformation to those unitary transformations with minimal polynomial of one of the following two kinds:

  1. Type 1: p(x)m, where p(x) is monic, irreducible, self-U-reciprocal polynomial with a non-zero constant term,

  2. Type 2: (q(x)q~(x))m, where q(x) is monic, irreducible, not self-U-reciprocal polynomial with a non-zero constant term.

Proposition 4 above gives us a primary decomposition of V into T-invariant B non-degenerate subspaces

V=(i=1k1Vi)(j=1k2Vj),

where Vi corresponds to the polynomials of Type 1 and Vj=Vqj+Vqj~ corresponds to the polynomials of Type 2. Denote the restriction of T to each Vr by Tr. Then the minimal polynomial of Tr is one of the two types. It turns out that the centralizer of T in U(V,B) is

𝒵U(V,B)(T)=r𝒵U(Vr,Br)(Tr),

where Br is a hermitian form obtained by restricting B to Vr. The direct product here comes from the primary decomposition (see [22, Chapter IV, Section 2.8]). Thus the conjugacy class and the z-class of T is determined by the restriction of T to each of the primary subspaces. Hence it is enough to determine the conjugacy class and the z-class of TU(V,B), which has minimal polynomial of one of the types listed above.

2.3 Conjugacy classes and centralizers

Let us define

ET=𝔽[x]f(x),

an 𝔽 algebra. Then V is an ET-module, where x acts via T. To keep track of the action we denote this module by VT although it is simply V as an 𝔽-vector space. The ET-module structure on VT determines the GLn-conjugacy class of T. To determine the conjugacy class of T within U(V,B), Springer and Steinberg (see [22, Chapter IV, Section 2.6]) defined a non-degenerate hermitian form HT on VT induced from B and T. We briefly recall this here. As f(x) is a self-U-reciprocal polynomial, there exists a unique involution α on ET such that α(x)=x-1 and α is an extension of σ on scalars. Thus, (ET,α) is an algebra with involution. Further, there exists an 𝔽-linear function lT:ET𝔽 such that the symmetric bilinear form lT¯:ET×ET𝔽 given by lT¯(a,b)=lT(ab) is non-degenerate with lT(α(a))=lT(a) for all aET. The hermitian form HT on ET-module VT (with respect to α) satisfies B(eu,v)=lT(eHT(u,v)) for all eET and u,vVT and is non-degenerate. Then (see [22, Chapter IV, Sections 2.7–2.8]):

Proposition 5.

With notation as above, let S and TU(V,B). Then:

  1. the elements S and T are conjugate in U(V,B) if and only if

    1. there exists an algebra-isomorphism ψ:ESET induced by x going to x,

    2. an 𝔽-isomorphism ϕ:VSVT satisfying, for all aES, v,wVS,

      ϕ(av)=ψ(a)ϕ(v)andHT(ϕ(v),ϕ(w))=ψ(HS(v,w)).

  2. The centralizer 𝒵U(V,B)(T)=U(VT,HT).

We can decompose the algebra ET as a direct sum of subalgebras with respect to α as ET=E1E2Er, where each component Ei is α-indecomposable (see [22, Chapter IV, Section 2.2]). That is, Ei cannot be further written as a direct sum of α-stable subalgebras. Now denote the restriction of α to Ei by αi. The αi, thus obtained, is again an involution on Ei. Clearly, each Ei is of one of the following types (recall the decomposition of f(x) in equation (2.1), also see [1, Lemma 2.6]):

  1. 𝔽[x]p(x)d, where p(x) is a monic, irreducible, self-U-reciprocal polynomial.

  2. 𝔽[x]q(x)d𝔽[x]q~(x)d, where q(x) is a monic, irreducible but not self-U-reciprocal.

In the second case, the two components 𝔽[x]/q(x)d and 𝔽[x]/q~(x)d are isomorphic local rings (induced by the U-reciprocal polynomial structure) and the restriction of α is given by α(a,b)=(b,a) via the fixed isomorphism. Using Wall’s approximation theorem (see Corollary 7 in the next section) it is easy to see that all non-degenerate hermitian forms over such rings are equivalent. Thus to determine equivalence of HT we need to look at modules over rings of Type 1.

2.4 Wall’s approximation theorem

We have reduced the conjugacy problem to equivalence of hermitian forms over certain rings. However, it turns out (see the corollary below) that the second case is easy. Let R be a commutative ring, where 2 is invertible (so that it satisfies the trace condition), let J be its Jacobson radical, and let α be an involution on R. Let M be a finitely generated module over R and (M,B) a non-degenerate hermitian space. We define M¯:=MJM a module over R¯:=RJ. Now B induces a hermitian form B¯ on M¯ with respect to the involution α¯ of R¯ induced by α. Then it is easy to see that (M¯,B¯) is non-degenerate. The converse is a theorem of Wall (see [27, Theorem 2.2.1], and also [1, Proposition 2.5]) which would be useful for further analysis. For the general theory of hermitian forms over a ring (which need not be commutative) we refer the reader to [20, Chapter 7, Theorem 4.4].

Theorem 6 (Wall’s approximation theorem).

With notation as above:

  1. Any non-degenerate hermitian form over R¯ is induced by some non-degenerate hermitian form over R.

  2. Let (M1,B1) and (M2,B2) be non-degenerate hermitian spaces over R and correspondingly (M1¯,B1¯) and (M2¯,B2¯) non-degenerate hermitian spaces over R¯. Then (M1,B1) is equivalent to (M2,B2) if and only if (M1¯,B1¯) is equivalent to (M2¯,B2¯).

We need the following:

Corollary 7.

Let 𝔽 be a perfect field of characteristic 2. Let V be a finitely generated module over

A=𝔽[x]q(x)d𝔽[x]q~(x)d,

where q(x) is a monic, irreducible polynomial and let H1 and H2 be two non-degenerate hermitian forms on V with respect to the “switch” involution on A given by (b,a)¯=(a,b). Then H1 and H2 are equivalent.

Proof.

We use Wall’s approximation theorem. Here R=A and its Jacobson radical is

J=q(x)q(x)dq~(x)q~(x)d.

Then

R¯=A¯𝔽[x]q(x)𝔽[x]q~(x)KK

is a semisimple ring, where

K𝔽[x]q(x)𝔽[x]q~(x)

is a finite field extension of 𝔽 (thus separable). Now we have hermitian forms Hi¯:V¯×V¯A¯ defined by Hi¯(u+JV,v+JV)=Hi(u,v)J for all u,vV. Now, the result follows from Proposition 2 and noting that we have n=m and forms are non-degenerate. ∎

2.5 Unipotent elements

We look at Type 1 more closely, where the minimal polynomial is p(x)d with p(x) an irreducible, self-U-reciprocal polynomial. This includes unipotent elements. The theory of rational canonical forms, which determines conjugacy classes in the group GL(V), gives a decomposition of V=i=1kVdi with 1d1d2dk=d and each Vdi is a free module over the 𝔽-algebra 𝔽[x]/p(x)di (see [22, Chapter IV, Section 2.14]). Thus:

Proposition 8.

Let S and T be in U(V,B). Suppose the minimal polynomials of S and T are equal, and equal to p(x)d, where p(x) is an irreducible self-U-reciprocal polynomial. Then S and T are conjugate in U(V,B) if and only if

  1. the elementary divisors p(x)di, where 1d1d2dk=d, of S and T are the same, i.e., they are GL(V) conjugate, and

  2. the following sequences of non-degenerate hermitian spaces are equivalent:

    1. {(Vd1S,Hd1S),,(VdkS,HdkS)} corresponding to S,

    2. {(Vd1T,Hd1T),,(VdkT,HdkT)} corresponding to T.

    Note that HdiS and HdiT take values in the cyclic 𝔽-algebra 𝔽[x]/p(x)di.

Further, the centralizer of T, in this case, is the direct product

𝒵U(V,B)(T)=i=1kU(VdiT,HdiT).

This gives us the following:

Corollary 9.

Suppose 𝔽0 has the property FE. Then the number of conjugacy classes of unipotent elements in U(V,B) is finite. Hence, the number of z-classes of unipotent elements in U(V,B) is finite.

Proof.

We use the above Proposition 8. A unipotent element has minimal polynomial (x-1)d for some d, that is, we have p(x)=x-1. Then, the conjugacy classes of unipotents correspond to sequences 1d1d2dk=d, and non-degenerate hermitian spaces {(Vd1T,Hd1T),,(VdkT,HdkT)} up to equivalence. Now

E¯diT=𝔽[T]T-1𝔽.

Then, by Wall’s approximation theorem, the number of non-equivalent non-degenerate hermitian forms (V,B) is exactly equal to the number of non-equivalent hermitian forms (V¯,B¯). From Proposition 1, we know that there are only finitely many non-equivalent hermitian forms over 𝔽. Thus HdiT has only finitely many choices for each i. Hence the result. ∎

3 z-classes in unitary groups and fields with property FE

A unitary group is an algebraic group defined over 𝔽0. Since we are working with perfect fields, an element TU(V,B) has a Jordan decomposition

T=TsTu=TuTs,

where Ts is semisimple and Tu is unipotent. Further, one can use this to compute the centralizer 𝒵U(V,B)(T)=𝒵U(V,B)(Ts)𝒵U(V,B)(Tu). So, the Jordan decomposition helps us reduce the study of conjugacy and computation of the centralizer of an element to the study of that of its semisimple and unipotent parts. In this section, we analyze semisimple elements and then we prove our main theorem.

3.1 Semisimple z-classes

Let TU(V,B) be a semisimple element. First, we begin with a basic case.

Lemma 1.

Let TU(V,B) be a semisimple element such that the minimal polynomial is either p(x), which is irreducible, self-U-reciprocal or q(x)q~(x), where q(x) is irreducible but not self-U-reciprocal. Let E=𝔽[x]/p(x) in the first case and 𝔽[x]/q(x) in the second case. Then the z-class of T is determined by the following:

  1. the algebra E over 𝔽, and

  2. the equivalence class of E-valued hermitian form HT on VT.

Proof.

This is the case of a regular semisimple element (see [10, Section 3]). Suppose S,TU(V,B) are in the same z-class. Then 𝒵U(V,B)(S)=g𝒵U(V,B)(T)g-1 for some gU(V,B). We may replace T by its conjugate gTg-1, so we get 𝒵U(V,B)(S)=𝒵U(V,B)(T) which is a maximal torus. Since T is semisimple and regular (the condition on the minimal polynomial gives this), 𝒵End(V)(T)E in the first case and E×E in the second case, which consists of essentially polynomials in T. Thus, U(VT,HT)=𝒵End(V)(T)U(V,HT) and hence T uniquely determines E and HT. The converse follows from Proposition 5. ∎

Now for the general case, let TU(V,B) be a semisimple element with minimal polynomial written as in equation (2.1)

mT(x)=i=1k1pi(x)j=1k2(qj(x)q~j(x)),

where the pi(x) are irreducible, self-U-reciprocal polynomials of degree mi and the qj(x) are irreducible but not self-U-reciprocal of degree lj. Let the characteristic polynomial of T be

χT(x)=i=1k1pi(x)dij=1k2(qj(x)q~j(x))rj.

Let us write the primary decomposition of V with respect to mT into T-invariant subspaces as

V=i=1k1Vij=1k2(Wj+W~j).

Denote by Ei=𝔽[x]/pi(x) and Kj=𝔽[x]/qj(x) the field extensions of 𝔽 of degree mi and lj, respectively.

Theorem 2.

With notation as above, let TU(V,B) be a semisimple element. Then the z-class of T is determined by the following:

  1. A finite sequence of integers (m1,,mk1;l1,,lk2) each 1 such that

    n=i=1k1dimi+2j=1k2rjlj.
  2. Finite field extensions Ei of 𝔽 of degree mi for 1ik1, and Kj of 𝔽 of degree lj, for 1jk2.

  3. Equivalence classes of Ei-valued hermitian forms Hi of rank di and Kj×Kj-valued hermitian forms Hj (which is unique up to equivalence) of rank rj.

Further, with this notation, 𝒵U(V,B)(T)i=1k1Udi(Hi)×j=1k2GLrj(Kj).

Proof.

The proof of this follows from Proposition 5 and Lemma 1. ∎

Corollary 3.

Let 𝔽0 have property FE. Then the number of semisimple z-classes in U(V,B) is finite.

Proof.

This follows if we can show that there are only finitely many hermitian forms over 𝔽, up to equivalence, of any degree n. But this is the content of Proposition 1. ∎

3.2 Proof of Theorem 2

It is already known that the number of z-classes in GLn(𝔽) is finite when 𝔽 has the property FE (see [16, p. 323, (iv)]). The number of conjugacy classes of centralizers of semisimple elements is finite; this follows from Corollary 3. Hence, up to conjugacy, there are finitely many possibilities for 𝒵U(V,B)(s) for s semisimple in U(V,B). Let TU(V,B); then it has a Jordan decomposition

T=TsTu=TuTs.

Recall that 𝒵U(V,B)(T)=𝒵U(V,B)(Ts)𝒵U(V,B)(Tu) and TuZU(V,B)(Ts) (see [22, Chapter V, Section 3.16]). Now, 𝒵U(V,B)(Ts) is a product of certain unitary groups and general linear groups possibly over a finite extension of 𝔽 (e.g. Ei and Kj in Theorem 2). Since 𝔽0 has the property FE, any finite extension of it has this property. Thus we can apply Corollary 9 to the group 𝒵U(V,B)(Ts) and get that, up to conjugacy, Tu has finitely many possibilities in 𝒵U(V,B)(Ts). Hence, up to conjugacy, 𝒵U(V,B)(T) has finitely many possibilities in U(V,B). Therefore the number of z-classes in U(V,B) is finite.

4 Counting z-classes in unitary group

We recall that there could be more than one non-equivalent non-degenerate hermitian form over a given field 𝔽 and hence more than one non-isomorphic unitary group. In this section, we want to count the number of z-classes and write its generating function. Special focus is on the unitary group over a finite field 𝔽=𝔽q2 of characteristic 2 with σ given by x¯=xq and 𝔽0=𝔽q. It is well known that over a finite field there is a unique non-degenerate hermitian form, up to equivalence, thus a unique unitary group up to conjugation. We denote the unitary group by Un(q)={gGLn(q2):gtJg¯=J}, where J is an invertible hermitian matrix (for example, the identity matrix). The groups GLn(q) and Un(q) are both subgroups of GLn(q2). It is interesting to note that the sizes of these groups as a function of q can be obtained from one another by q-q. Ennola noted that this idea goes forward to the sizes of conjugacy classes and representations of small rank unitary groups. This came to be known as Ennola duality and later it was proved that indeed the Green polynomial for unitary groups could be obtained this way from that of GLn(q). Thus, the representation theory of both these groups is closely related (for example see [24, 26]). For applications in the subject of derangements see Burness and Giudici [4]. Thus it is always useful to compare any computation for Un(q) with that of GLn(q). We begin by recording some well-known results about GLn.

4.1 z-classes in general linear group

Let p(n) denote the number of partitions of n with generating function

p(x):=n=0p(n)xn=i=111-xi.

Let z𝔽(n) denote the number of z-classes in GLn(𝔽) and let the generating function be

z𝔽(x):=n=0z𝔽(n)xn.

Let us denote a partition of n by (1k12k2nkn) with n=iiki. For convenience, we denote this by n(1k12k2nkn). The following result is a consequence of the theory of Jordan canonical forms and the formula is given in [16, Section 10, The absolute case]. However, the formula there has a printing error.

Proposition 1.

Let K be an algebraically closed field. Then:

  1. The number of z-classes of semisimple elements in GLn(K) is p(n), and is equal to the number of z-classes of unipotent elements.

  2. The number of z-classes in GLn(K) is

    zK(n)=n(1k12k2nkn)i=1n(p(i)+ki-1ki),

    and the generating function is

    z(x):=zK(x)=i=11(1-xi)p(i).

Green computed the number of z-classes in GLn(q) (see [12, Section 1]), which is the function t(n) there. We list them here in our notation (see [16, Section 10, General case]).

Proposition 2.

Let z(x)=i=11(1-xi)p(i). Then:

  1. z(x)=z(x).

  2. z(x)=z(x)z(x2).

  3. When q>n, the function i=1z(xi) computes z𝔽q(n).

Thus if we treat z𝔽q(x)=i=1z(xi), this proposition beautifully reflects the arithmetic nature of the field. To compare these numbers we make a table for small rank. The last row of this table is there in the work of Green.

zk(n)z(1)z(2)z(3)z(4)z(5)z(6)z(7)z(8)z(9)z(10)
136142758111223424817
1472036871623556661367
𝔽q,q>n14822421031994418591784

4.2 z-classes in hyperbolic unitary group

In geometry the unitary groups used are over . Let V be a vector space over of dimension n+1. Hermitian forms are classified by signature (as in the case of quadratic forms over ) and the corresponding groups are denoted as U(r,s), where r+s=n+1. The group given by the identity matrix is the compact unitary group denoted as Un+1(In+1)=U(n+1,0). The genus number (which is the number of z-classes) of the compact special unitary group has been computed in [3, Theorem 3.1]. We record the result here as follows:

Proposition 3.

The number of z-classes in Un+1(In+1) is p(n+1).

The centralizers and z-classes in the group U(n,1) have been described by Cao and Gongopadhyay in [5, Section 4]. However, they have not done explicit counting. Keeping in mind the spirit of this section, we enumerate the number of z-classes in this group as well. We briefly recall the notation here and urge the interested reader to see the source and references therein for details. Let V be an (n+1)-dimensional vector space over with the hermitian form given by

β=(-100In)

which is of signature (n,1). The unitary group is

U(n,1)={gGL(n+1,):g¯tβg=β}.

Let V- be the vectors of negative length in V. The image of V- in the projective space (V) is denoted as n which is a complex hyperbolic space. An element of the group is called elliptic if it has a fixed point on n and is said to be parabolic, respectively, hyperbolic, if it has exactly one, respectively, two fixed points on the boundary of n. Every element falls in one of these three classes. Using the conjugation classification, we know that if an element gU(n,1) is elliptic or hyperbolic, then it is semisimple. But a parabolic element need not be semisimple. However, it has a Jordan decomposition g=gsgu, where gs is elliptic, hence semisimple, and gu is unipotent. In particular, if a parabolic isometry is unipotent, then it has minimal polynomial (x-1)2 or (x-1)3 and is called a vertical translation or non-vertical translation respectively. The centralizers of these elements are described in [5, Corollary 1.2] and we present the counting for z-classes here.

Proposition 4.

In the group U(n,1), the following statements hold:

  1. The number of z-classes of elliptic elements is m=1n+1p(n+1-m).

  2. The number of z-classes of hyperbolic elements is p(n-1).

  3. The number of z-classes of parabolic elements is 2+p(n-1)+p(n-2), in this case n2.

Proof.

Let TU(n,1) be an elliptic element (see [5, Section 4.1 (1)]). Then T has a negative class of eigenvalue say [λ]. Let m=dim(Vλ) which is 1. It follows from the conjugacy classification that all the eigenvalues have norm 1, and there is a negative eigenvalue. All other eigenvalues are of positive type. Then V=VλVλ=Vλ(i=1sVλi). Suppose dim(Vλi)=ri; then

𝒵U(n,1)(T)=𝒵U(Vλ)(T|Vλ)×i=1sU(ri).

Now since T|Vλ is of negative type, so

𝒵(T|Vλ)=U(m-1,1).

Here n+1=m+i=1sri, therefore

i=1sri=n+1-m.

This gives that the number of z-classes of elliptic elements is m=1n+1p(n+1-m).

Now, suppose TU(n,1) is hyperbolic (see [5, Section 4.1 (2)]). Then V has an orthogonal decomposition V=Vr(i=1kVi), where dim(Vi)=ri and Vi is the eigenspace of T corresponding to the similarity class of positive eigenvalue [λi] with |λi|=1. The subspace Vr is the two-dimensional T-invariant subspace spanned by the corresponding similarity class of null-eigenvalues [reiθ],[r-1eiθ] for r>1, respectively. Then

𝒵U(n,1)(T)=𝒵(T|Vr)×j=1kU(rj)=S1××j=1kU(rj).

Here n+1=2+j=1krj, i.e.,

j=1krj=n-1.

Thus, the number of z-classes of hyperbolic elements is p(n-1).

Let TU(n,1) be parabolic (see [5, Section 4.2]). First, let T be unipotent. If the minimal polynomial of T is (x-1)2 (i.e., T is a vertical translation), then

𝒵U(n,1)(T)=U(n-1)(n-1×).

If the minimal polynomial of T is (x-1)3 (i.e., T is a non-vertical translation), then

𝒵U(n,1)(T)=(S1×U(n-2))((×n-2)).

Hence there are exactly two z-classes of unipotents, one corresponds to the vertical translations and the other to the non-vertical translations. Now assume that T is not unipotent. Suppose that the similarity class of the null-eigenvalue is [λ]. Then V has a T-invariant orthogonal decomposition V=VλVλ, where Vλ is a T-indecomposable subspace of dim(Vλ)=m, which is either 2 or 3. Then 𝒵U(n,1)(T)=𝒵(T|Vλ)×𝒵(T|Vλ). For each choice of λ, there is exactly one choice for the z-classes of T|Vλ in U(m-1,1), i.e., U(1,1) or U(2,1). Note that T|Vλ can be embedded into U(n+1-m). Hence it suffices to find out the number of z-classes of T|Vλ in U(m-1,1). Hence the total number of z-classes of non-unipotent parabolic is p(n-1)+p(n-2). Therefore the total number of z-classes of parabolic transformations is 2+p(n-1)+p(n-2) (n2). ∎

4.3 z-classes in finite unitary group

Now let us look at the finite unitary group in characteristic 2.

Proposition 5.

The following statements hold:

  1. The number of z-classes of unipotent elements in Un(q) is p(n), which is equal to the number of z-classes of unipotent elements in GLn(q).

  2. The number of z-classes of semisimple elements in Un(q) is equal to the number of z-classes of semisimple elements in GLn(q) if q>n.

Proof.

Let u=[J1a1J2a2Jnan] be a unipotent element in GLn(q2) written in Jordan block form. Wall proved the following membership test (see [27, Case(A) on p. 34]). Let AGLn(q2); then A is conjugate to A¯-1t in GLn(q2) if and only if A is conjugate to an element of Un(q). Since unipotents are conjugate to their own inverse in GLn(q2), this implies u is conjugate to u¯-1t in GLn(q2). Hence u is conjugate to an element of Un(q). Wall also proved that two elements of Un(q) are conjugate in Un(q) if and only if they are conjugate in GLn(q2) (see also [17, Section 6.1]). Thus, up to conjugacy, there is a one-one correspondence of unipotent elements between GLn(q2) and Un(q). This shows that the number of unipotent conjugacy classes in Un(q) is p(n), and it is the same as that of GLn(q). Now, we note that

𝒵Un(q)(u)=Qi=1nUai(q),

where

|Q|=qi=2n(i-1)ai2+2i<jiaiaj

(see [4, Lemma 3.3.8]). Clearly, the centralizers are distinct and hence cannot be conjugate. Thus the number of unipotent z-classes in Un(q) is p(n).

For semisimple elements we use Theorem 2. Since over a finite field, there is a unique hermitian form (see [13, Corollary 10.4]) the third condition is irrelevant in counting. Over a finite field for q>n, we get that semisimple z-classes are characterized by simply

n=i=1k1dimi+j=1k2ejlj,

where di is odd (being the degree of a monic, irreducible, self-U-reciprocal polynomial, see Proposition 3) and ej=2rj is even. This corresponds to the number of ways n can be written as

n=iaibi

when q>n which is the same as the number of semisimple z-classes in GLn(q) (see [16, Theorem 7.2]). Notice that in the case qn we do not get enough field extensions to meet the requirement in the second condition of the Theorem 2 and hence we may not get all partitions of n. ∎

4.4 Proof of the Theorem 3

We begin by recalling the parametrization of z-classes in GLn(q) described by Green in [12, last paragraph and equation (1) on p. 407]. It is given by zq(n)=t(n) which is the number of functions ρ(ν) satisfying ν|ρ(ν)||ν|=n and ρ(ν) is the partition-valued function on the non-zero partitions ν (here ρ(ν) is allowed to take value 0). Following the proof there we note that zq(n) is the number of z-classes in GLn(q) which is equal to

[s]znumber of unipotent z-classes in 𝒵GLn(q)(s),

and 𝒵GLn(q)(s) is a product of GLm(q), where mn and 𝔽q is a field extension of 𝔽q of degree n. Green also clarifies that this formula works for “sufficiently large q”. We use the same strategy and show that the z-classes in Un(q) are parameterized by the same function for q>n. Recall that if g=gsgu is a Jordan decomposition of g, then

𝒵Un(q)(g)=𝒵Un(q)(gs)𝒵Un(q)(gu)=𝒵𝒵Un(q)(gs)(gu),

and the structure of the centralizer 𝒵Un(q)(gs) in Theorem 2 implies that the number of z-classes in Un(q) is equal to

[s]z number of unipotent z-classes in 𝒵Un(q)(s),

where the sum runs over semisimple z-classes and is same as for GLn(q). Now, we know that the number of unipotent z classes in Um(q) and GLm(q) is the same and thus unitary groups appearing in the centralizer of a semisimple element have the same effect in counting as for the general linear group. Hence the number of z-classes in Un(q) is the same as the number of z-classes in GLn(q).

5 Examples

We give some examples which highlight the need of the property FE on the field.

Example 1.

Over the field , there are infinitely many non-conjugate maximal tori in GLn. Since a maximal torus is the centralizer of a regular semisimple element in it, we get an example of infinitely many z-classes. For the sake of clarity let us write down this concretely when n=2.

The group GL2() has infinitely many semisimple z-classes. For this, we take f(x)[x] a degree 2 irreducible polynomial, then the centralizer of the companion matrix CfGL2() is isomorphic to f*, where f=[x]/f(x), a degree 2 field extension of . For example, if we take f(x)=x2-p, where p is a prime, we get infinitely many non-isomorphic degree 2 field extensions of . Since these are not isomorphic, the corresponding centralizers f* cannot be conjugate. This way we get infinitely many z-classes of semisimple elements, in fact, this gives infinitely many non-conjugate maximal tori in GL2().

Consider 𝔽=[d], a quadratic extension. We embed GL2() in U4 with respect to the hermitian form (I2I2) given by

A(AA¯-1t).

This embedding describes maximal tori in U4 starting from that of GL2. Yet again, non-isomorphic degree 2 field extensions would give rise to distinct z-classes. In turn, this gives infinitely many z-classes (of semisimple elements) in U4.

Example 2.

For a𝔽*, consider a unipotent element ua=(1a1) in SL2(𝔽). We have 𝒵SL2(𝔽)(ua)={(xyx):x2=1,y𝔽}. Then ua is conjugate to ub in SL2(𝔽) if and only if ab(mod(𝔽*)2). Let 𝔽 be a (perfect or non-perfect) field with 𝔽*/(𝔽*)2 infinite. Then this would give an example, where we have infinitely many conjugacy classes of unipotents but still, they are in a single z-class.

Example 3.

Over a finite field 𝔽q, if q is not large enough, we may not have as many finite extensions available as required in part (2) of Theorem 2. Thus we expect a smaller number of z-classes. We use GAP [29] to calculate the number of z-classes for small order and present our findings below.

z𝔽q(2)q=2q=3q=4q=5q=7q=9
GL2(q)344444
U2(q)344444
z𝔽q(3)q=2q=3q=4q=5q=7q=9
GL3(q)578888
U3(q)788888
z𝔽q(4)q=2q=3q=4q=5q=7
GL4(q)1119212222
U4(q)1522222222

Thus we demonstrate the following:

  1. When qn, the number of z-classes in GLn(q) and Un(q) are not given by the formula in Theorem 3.

  2. When qn, the number of z-classes in GLn(q) and Un(q) need not be equal.


Communicated by Radha Kessar


Funding statement: The first named author gratefully acknowledges the PhD fellowship provided by CSIR during this work. The second named author acknowledges the support of NBHM grant during this work.

Acknowledgements

The authors would like to thank Ben Martin, University of Aberdeen for his comments on the paper. The authors thank the referees for the wonderful comments which improved the readability of this paper.

References

[1] T. Asai, The conjugacy classes in the unitary, symplectic and orthogonal groups over an algebraic number field, J. Math. Kyoto Univ. 16 (1976), no. 2, 325–350. 10.1215/kjm/1250522918Suche in Google Scholar

[2] C. Bonnafé, Representations of SL2(𝔽q), Algebra Appl. 13, Springer, London, 2011. Suche in Google Scholar

[3] A. Bose, On the genus number of algebraic groups, J. Ramanujan Math. Soc. 28 (2013), no. 4, 443–482. Suche in Google Scholar

[4] T. C. Burness and M. Giudici, Classical Groups, Derangements and Primes, Austral. Math. Soc. Lect. Ser. 25, Cambridge University Press, Cambridge, 2016. 10.1017/CBO9781139059060Suche in Google Scholar

[5] W. Cao and K. Gongopadhyay, Commuting isometries of the complex hyperbolic space, Proc. Amer. Math. Soc. 139 (2011), no. 9, 3317–3326. 10.1090/S0002-9939-2011-10796-2Suche in Google Scholar

[6] R. W. Carter, Finite Groups of Lie Type, Wiley Class. Libr., John Wiley & Sons, Chichester, 1993. Suche in Google Scholar

[7] F. Digne and M. J. François, Representations of Finite Groups of Lie Type, London Math. Soc. Stud. Texts 21, Cambridge University Press, Cambridge, 1991. 10.1017/CBO9781139172417Suche in Google Scholar

[8] V. Ennola, On the conjugacy classes of the finite unitary groups, Ann. Acad. Sci. Fenn. Ser. A I 313 (1962), 1–13. 10.5186/aasfm.1962.313Suche in Google Scholar

[9] P. Fleischmann, Finite fields, root systems, and orbit numbers of Chevalley groups, Finite Fields Appl. 3 (1997), no. 1, 33–47. 10.1006/ffta.1996.0171Suche in Google Scholar

[10] J. Fulman and R. Guralnick, The number of regular semisimple conjugacy classes in the finite classical groups, Linear Algebra Appl. 439 (2013), no. 2, 488–503. 10.1016/j.laa.2013.03.031Suche in Google Scholar

[11] K. Gongopadhyay and R. S. Kulkarni, The Z-classes of isometries, J. Indian Math. Soc. (N.S.) 81 (2014), no. 3–4, 245–258. Suche in Google Scholar

[12] J. A. Green, The characters of the finite general linear groups, Trans. Amer. Math. Soc. 80 (1955), 402–447. 10.1090/S0002-9947-1955-0072878-2Suche in Google Scholar

[13] L. C. Grove, Classical Groups and Geometric Algebra, Grad. Stud. Math. 39, American Mathematical Society, Providence, 2002. 10.1090/gsm/039/06Suche in Google Scholar

[14] J. E. Humphreys, Conjugacy Classes in Semisimple Algebraic Groups, Math. Surveys Monogr. 43, American Mathematical Society, Providence, 1995. Suche in Google Scholar

[15] N. Jacobson, A note on Hermitian forms, Bull. Amer. Math. Soc. 46 (1940), 264–268. 10.1007/978-1-4612-3692-4_21Suche in Google Scholar

[16] R. S. Kulkarni, Dynamics of linear and affine maps, Asian J. Math. 12 (2008), no. 3, 321–343. 10.4310/AJM.2008.v12.n3.a4Suche in Google Scholar

[17] I. G. Macdonald, Numbers of conjugacy classes in some finite classical groups, Bull. Aust. Math. Soc. 23 (1981), no. 1, 23–48. 10.1017/S0004972700006882Suche in Google Scholar

[18] J. Milnor, On isometries of inner product spaces, Invent. Math. 8 (1969), 83–97. 10.1007/BF01404612Suche in Google Scholar

[19] A. Prasad, Representations of GL2(𝔽q) and SL2(𝔽q), and some remarks about GLn(𝔽q)”, preprint (2007), https://arxiv.org/abs/0712.4051. Suche in Google Scholar

[20] W. Scharlau, Quadratic and Hermitian Forms, Grundlehren Math. Wiss. 270, Springer, Berlin, 1985. 10.1007/978-3-642-69971-9Suche in Google Scholar

[21] A. Singh, Conjugacy classes of centralizers in G2, J. Ramanujan Math. Soc. 23 (2008), no. 4, 327–336. Suche in Google Scholar

[22] T. A. Springer and R. Steinberg, Conjugacy classes, Seminar on Algebraic Groups and Related Finite Groups (Princeton 1968/69), Lecture Notes in Math. 131, Springer, Berlin (1970), 167–266. 10.1007/BFb0081546Suche in Google Scholar

[23] B. Srinivasan, The characters of the finite symplectic group Sp(4,q), Trans. Amer. Math. Soc. 131 (1968), 488–525. 10.1090/S0002-9947-1968-0220845-7Suche in Google Scholar

[24] B. Srinivasan and C. R. Vinroot, Semisimple symplectic characters of finite unitary groups, J. Algebra 351 (2012), 459–466. 10.1016/j.jalgebra.2011.08.012Suche in Google Scholar

[25] R. Steinberg, Conjugacy Classes in Algebraic Groups. Notes by Vinay V. Deodhar, Lecture Notes in Math. 366, Springer, Berlin, 1974. 10.1007/BFb0067854Suche in Google Scholar

[26] N. Thiem and C. R. Vinroot, On the characteristic map of finite unitary groups, Adv. Math. 210 (2007), no. 2, 707–732. 10.1016/j.aim.2006.07.018Suche in Google Scholar

[27] G. E. Wall, On the conjugacy classes in the unitary, symplectic and orthogonal groups, J. Aust. Math. Soc. 3 (1963), 1–62. 10.1017/S1446788700027622Suche in Google Scholar

[28] J. Williamson, Normal matrices over an arbitrary field of characteristic zero, Amer. J. Math. 61 (1939), no. 2, 335–356. 10.2307/2371503Suche in Google Scholar

[29] The GAP Group, GAP – Groups, Algorithms, and Programming, Version 4.8.7, 2017, http://www.gap-system.org. Suche in Google Scholar

Received: 2017-04-19
Revised: 2018-09-15
Published Online: 2018-10-11
Published in Print: 2019-03-01

© 2020 Walter de Gruyter GmbH, Berlin/Boston

Heruntergeladen am 23.9.2025 von https://www.degruyterbrill.com/document/doi/10.1515/jgth-2018-0036/html
Button zum nach oben scrollen