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Stiefel–Whitney classes of representations of SL(2, 𝑞)

  • Neha Malik ORCID logo EMAIL logo and Steven Spallone
Published/Copyright: February 28, 2023

Abstract

We describe the Stiefel–Whitney classes (SWCs) of orthogonal representations 𝜋 of the finite special linear groups G = SL ( 2 , F q ) , in terms of character values of 𝜋. From this calculation, we can answer interesting questions about SWCs of 𝜋. For instance, we determine the subalgebra of H * ( G , Z / 2 Z ) generated by the SWCs of orthogonal 𝜋, and we also determine which 𝜋 have non-trivial mod 2 Euler class.

1 Introduction

The theory of Stiefel–Whitney classes (SWCs) of vector bundles is an old unifying concept in geometry. Real representations or, equivalently, orthogonal complex representations of a group 𝐺 give rise to flat vector bundles over the classifying space B G . Via this construction, one associates SWCs w i ( π ) H i ( G , Z / 2 Z ) to an orthogonal representation 𝜋 of 𝐺. Their sum w ( π ) , living in the group cohomology H * ( G , Z / 2 Z ) , is known as the total Stiefel–Whitney class of 𝜋.

There do not seem to be many explicit calculations of such SWCs, notably when 𝐺 is non-abelian. (However, see [14].) This paper contains formulas for SWCs in terms of character values for SL ( 2 , q ) , when 𝑞 is a prime power, achieved via detection results. Formulas for SWCs of cyclic groups are well known; we review this for the group of order 2 in Section 2.5. The second SWCs of representations of S n and related groups were found in [11].

The case of GL ( n , q ) with 𝑞 odd was completed recently by Ganguly–Joshi in [9, 10]. To explain how their work relates to ours, we need to introduce “detection”.

Let 𝐺 be a finite group, and write H * ( G , Z / 2 Z ) for the mod 2 group cohomology ring of 𝐺. Let H SW * ( G , Z / 2 Z ) be the subalgebra of H * ( G , Z / 2 Z ) generated by SWCs w i ( π ) of orthogonal representations 𝜋 of 𝐺. We say a subgroup 𝐾detects the mod 2 cohomology of 𝐺 when the restriction map

i * : H * ( G , Z / 2 Z ) H * ( K , Z / 2 Z )

is an injection, and we say 𝐾detects SWCs of 𝐺 when this map is injective on H SW * ( G , Z / 2 Z ) . Suppose one of these is true and that 𝜋 is an orthogonal representation of 𝐺. Then w ( π ) is specified by its image in H * ( K , Z / 2 Z ) , which is actually the SWC of the restriction of 𝜋 to 𝐾. When there is a detecting subgroup, one simply writes w ( π ) for this image.

An essential tool in Ganguly–Joshi’s papers is a theorem of Quillen [20], asserting that the diagonal subgroup of GL ( n , q ) detects its mod 2 cohomology. However, such a result is not available to us. Instead, most of this paper is devoted to establishing the following.

Theorem 1.1

Let G = SL ( 2 , q ) with 𝑞 odd. Then the center 𝑍 detects SWCs of 𝐺.

From this, we obtain the following theorem.

Theorem 1.2

Let G = SL ( 2 , q ) with 𝑞 odd. Let 𝜋 be an orthogonal representation of 𝐺. Then the total SWC of 𝜋 is

w ( π ) = ( 1 + e ) r π ,

where 𝔢 is the non-zero element in H 4 ( SL ( 2 , q ) , Z / 2 Z ) and

r π = 1 8 ( χ π ( 1 ) χ π ( 1 ) ) .

(Here 1 is the identity matrix.) If 𝜋 is also irreducible, then w ( π ) = 1 .

In future work, these two theorems will be applied to determine SWCs of other finite groups of Lie type.

The case of 𝑞 even is quite different. Here the upper unitriangular subgroup N F q detects the mod 2 cohomology of the special linear group, and we use this to prove the following.

Theorem 1.3

Let ( π , V ) be an orthogonal representation of G = SL ( 2 , q ) , with 𝑞 even. Then the total SWC of 𝜋 is

w ( π ) = ( 1 + D ) m π ,

where m π = dim C ( V / V G ) , where V G is the 𝐺-fixed vectors in 𝑉, and 𝒟 is the sum of the Dickson invariants of F q , viewed as a Z / 2 Z -vector space.

(Dickson invariants are reviewed in Section 5.)

There are several corollaries of Theorems 1.2 and 1.3. Let G = SL ( 2 , q ) . Firstly, we describe the subgroup of the complete cohomology ring H ( G , Z / 2 Z ) (see Section 2.6) generated by w ( π ) , as 𝜋 varies over orthogonal representations.

Corollary 1.4

This subgroup is equal to

  1. { ( 1 + e ) n : n Z } for 𝑞 odd,

  2. { ( 1 + D ) n : n Z } for 𝑞 even.

Secondly, we compute H SW * ( G , Z / 2 Z ) .

Corollary 1.5

The subalgebra H SW * ( G , Z / 2 Z ) is

  1. Z / 2 Z [ e ] for 𝑞 odd,

  2. generated by the Dickson invariants of F q for 𝑞 even.

Another characteristic class of importance is the Euler class e ( π ) H d ( G , Z ) , where d = deg π . We define w top ( π ) = w deg π ( π ) ; it is the “top” Stiefel–Whitney class of 𝜋. By [19, Property 9.5], we know that w top ( π ) is the reduction of e ( π ) mod 2.

Corollary 1.6

Let ( π , V ) be an orthogonal representation of 𝐺. Then we have w top ( π ) 0 precisely when

  1. π ( 1 ) = 1 , meaning π ( 1 ) acts on 𝑉 by the scalar −1, for 𝑞 odd,

  2. V N = { 0 } for 𝑞 even. (Equivalently, 𝜋 is cuspidal.)

Finally, we determine the obstruction degree of an orthogonal 𝜋, meaning the least k > 0 with w k ( π ) 0 . (If w ( π ) is trivial, then this degree is infinite.) Write ord 2 ( n ) for the highest power of 2 which divides an integer 𝑛.

Corollary 1.7

The obstruction degree of 𝜋 is

  1. 2 t + 2 , where t = ord 2 ( r π ) , for 𝑞 odd,

  2. 2 r + s 1 , where s = ord 2 ( m π ) and q = 2 r .

The layout of the paper is as follows. Section 2 recalls some fundamental notions used throughout the paper. Section 3 is dedicated to the generalized quaternions, particularly the quaternion group 𝑄 of order 8. These groups are featured in the detection of SL ( 2 , q ) when 𝑞 is odd. Here we also determine w 4 i ( π ) for orthogonal representations 𝜋 of 𝑄. In Section 4, we prove Theorems 1.1 and 1.2, the corollaries for 𝑞 odd, and finally compare our result to the GL ( 2 , q ) case. In Section 5, we prove Theorem 1.3 and the corollaries for 𝑞 even.

2 Notation and preliminaries

2.1 Representations

Let 𝐺 be a finite group. All our representations will be finite-dimensional. Let 𝜋 be a representation of 𝐺 on a complex vector space 𝑉. Write χ π ( g ) for the character of 𝜋 at an element g G . If 𝐻 is a subgroup of 𝐺, write res H G π for the restriction of 𝜋 to 𝐻. Write reg ( G ) for the regular representation of 𝐺.

We say 𝜋 is orthogonal, provided there exists a non-degenerate 𝐺-invariant symmetric bilinear form B : V × V C . We say it is symplectic, provided there exists a non-degenerate 𝐺-invariant antisymmetric bilinear form B : V × V C .

When 𝜋 is self-dual and irreducible, it is either orthogonal or symplectic. In this case, the Frobenius–Schur indicator ε ( π ) is a sign defined as 1 when 𝜋 is orthogonal, and −1 when 𝜋 is symplectic.

2.2 Orthogonal representations

We are especially interested in orthogonal representations.

From [3, Chapter II, Section 6], we note the following result.

Proposition 2.1

If ( π , V ) is orthogonal, then there is a ( π 0 , V 0 ) , with V 0 a real vector space, so that π 0 R C π . Moreover, π 0 is unique up to isomorphism.

Given a representation ( π , V ) with dual ( π , V ) , we can symmetrize it to get an orthogonal representation of 𝐺 by defining S ( π ) := π π on the vector space V V . We give a symmetric 𝐺-invariant bilinear map 𝐵 on V V as

B ( ( v , α ) , ( w , β ) ) = α , w + β , v .

We call S ( π ) the symmetrization of 𝜋.

Every orthogonal complex representation Π of 𝐺 can be decomposed as

(2.1) Π i π i j S ( φ j )

such that each π i is irreducible orthogonal and φ j are irreducible non-orthogonal representations of 𝐺.

Definition 2.2

A complex representation 𝜋 of 𝐺 is said to be an orthogonally irreducible representation (OIR), provided 𝜋 is orthogonal, and cannot be decomposed into a direct sum of orthogonal representations.

An irreducible representation 𝜋 is orthogonally irreducible if and only if 𝜋 is orthogonal. Moreover, for 𝜑 irreducible and non-orthogonal, its symmetrization S ( φ ) is an OIR. In fact, the decomposition in (2.1) establishes that all the OIRs of 𝐺 are either irreducible orthogonal 𝜋, or of the form S ( φ ) with 𝜑 irreducible and non-orthogonal.

2.3 Stiefel–Whitney classes

In this section, we define Stiefel–Whitney classes for orthogonal complex representations of finite groups. This is equivalent to the definition in [2] or [15], given for real representations.

Recall from [19] that a (𝑑-dimensional real) vector bundle 𝒱 over a paracompact space 𝐵 is assigned a sequence w 1 ( V ) , , w d ( V ) of cohomology classes, with each w i ( V ) H * ( B , Z / 2 Z ) .

For every finite group 𝐺, there is a classifying space B G with a principal 𝐺-bundle E G , unique up to homotopy. From a real representation ( ρ , V ) , one can form the associated vector bundle E G [ V ] over B G . Then one puts

w i R ( ρ ) = w i ( E G [ V ] ) ;

see for instance [2, 15]. Moreover, the singular cohomology H * ( B G , Z / 2 Z ) is isomorphic to the group cohomology H * ( G , Z / 2 Z ) . At this point, we simply write H * ( G ) = H * ( G , Z / 2 Z ) .

Hence, to a real representation 𝜌, we can associate cohomology classes

w i R ( ρ ) H i ( G ) ,

called Stiefel–Whitney classes (SWCs). We prefer to work with an orthogonal complex representation 𝜋, which by Proposition 2.1 comes from a unique real representation π 0 . We thus define w i ( π ) := w i R ( π 0 ) for 0 i deg π .

A group homomorphism φ : G 1 G 2 induces a map φ * : H * ( G 2 ) H * ( G 1 ) . The SWCs are functorial in the following sense: if 𝜋 is an orthogonal representation of G 2 , then φ * ( w ( π ) ) = w ( π φ ) .

The SWCs are also multiplicative. This means if π 1 and π 2 are both orthogonal, then w ( π 1 π 2 ) = w ( π 1 ) w ( π 2 ) . The first few w i ( π ) have nice interpretations. Firstly, w 0 ( π ) = 1 H 0 ( G ) , and the first SWC, applied to linear characters G { ± 1 } Z / 2 Z , is the well-known isomorphism

w 1 : Hom ( G , ± 1 ) H 1 ( G ) .

More generally, if 𝜋 is an orthogonal representation, then w 1 ( π ) = w 1 ( det π ) , where det π is simply the composition of 𝜋 with the determinant map. When det π = 1 , then w 2 ( π ) vanishes if and only if 𝜋 lifts to the corresponding spin group. (See [11] for details.)

To complex representations 𝜋 of 𝐺 are associated cohomology classes

c i ( π ) H 2 i ( G , Z ) ,

called Chern classes. As with SWCs, c 0 ( π ) = 1 , and the first Chern class, applied to linear characters, gives the well-known isomorphism

c 1 : Hom ( G , S 1 ) H 2 ( G , Z ) .

More generally, c 1 ( π ) = c 1 ( det π ) for a complex representation 𝜋.

The SWC of a symmetrization S ( π ) can be obtained from the Chern class of 𝜋 via the formula w ( S ( π ) ) = κ ( c ( π ) ) . Here κ : H * ( G , Z ) H * ( G , Z / 2 Z ) is the coefficient homomorphism of cohomology. (See [9, Lemma 1], based on [19, Problem 14-B].)

From this, we make an observation for later use.

Lemma 2.3

If det π = 1 , then w i ( S ( π ) ) = 0 for i = 1 , 2 , 3 .

Proof

Since Chern classes live in even degrees, all the odd SWCs of S ( π ) vanish. Moreover, c 1 ( π ) = 0 by the determinant hypothesis. ∎

2.4 Steenrod squares

For n , i 0 , there are operations on cohomology, called Steenrod squares,

Sq i : H n ( G ) H n + i ( G ) .

These are additive homomorphisms and Sq 0 is the identity. Steenrod operations are functorial, meaning for a group homomorphism φ : G G , we have

φ * ( Sq i y ) = Sq i ( φ * ( y ) ) for all y H n ( G ) .

We now state the well-known Wu formula.

Proposition 2.4

Proposition 2.4 ([18, Chapter 23, Section 6])

Let 𝜋 be an orthogonal representation of 𝐺. Then the cohomology class Sq i ( w j ( π ) ) can be expressed as a polynomial in w 1 ( π ) , , w i + j ( π ) ,

Sq i ( w j ( π ) ) = t = 0 i ( j + t i 1 t ) w i t ( π ) w j + t ( π ) .

With i = 1 , j = 2 for instance, we can express w 3 ( π ) in terms of w 1 , w 2 as follows:

w 3 ( π ) = w 1 ( π ) w 2 ( π ) + Sq 1 ( w 2 ( π ) ) .

2.5 Elementary abelian 2-groups

Let C 2 = { ± 1 } , the cyclic group of order 2. Here we review explicit descriptions of group cohomology for elementary abelian 2-groups C 2 n and describe SWCs in terms of these descriptions.

We write “sgn” for the order 2 linear character of C 2 . It is known [16] that

(2.2) H * ( C 2 ) Z / 2 Z [ v ] ,

where v = w 1 ( sgn ) . Since this group is so simple, we can give our first example of expressing SWCs in terms of character values. (Note that every representation of C 2 is orthogonal.)

Lemma 2.5

Let 𝜋 be a representation of C 2 , and b π = 1 2 ( deg π χ π ( 1 ) ) . Then the total SWC of 𝜋 is w ( π ) = ( 1 + v ) b π .

Proof

We can write π = a  1 b ( sgn ) for non-negative integers a , b . From the multiplicativity of SWCs, we obtain w ( π ) = ( 1 + v ) b . To express 𝑏 in character values, consider the equations

χ π ( 1 ) = a + b , χ π ( 1 ) = a b

giving b = 1 2 ( χ π ( 1 ) χ π ( 1 ) ) = b π . ∎

Let C 2 n be the 𝑛-fold product of C 2 , with projection maps pr i : C 2 n C 2 for 1 i n . By Künneth, we have H * ( C 2 n ) = Z / 2 Z [ v 1 , , v n ] , where we put v i = w 1 ( sgn pr i ) .

2.6 SWCs for virtual representations

A virtual representation of 𝐺 can be thought as a difference π = π 1 π 2 for representations π 1 , π 2 . When the π i are orthogonal, one may define the SWC of 𝜋 as w ( π ) = w ( π 1 ) w ( π 2 ) 1 , but we must “complete” the cohomology ring so that the inversion makes sense.

More formally, let 𝐺 be a finite group, and let RO ( G ) be the free abelian group generated by the isomorphism classes of OIRs (following [3, Chapter II, Section 7]). Members of RO ( G ) are called virtual orthogonal representations of 𝐺.

Write

H ( G ) = i H i ( G )

for the complete mod 2 cohomology ring of 𝐺, consisting of all formal infinite series α 0 + α 1 + , with α i H i ( G ) . (Please see [22, page 44].) Each w ( π ) is invertible in this ring.

It is clear now that we may “extend” 𝑤 to a group homomorphism, taking values in the unit group of H ( G ) , i.e.

(2.3) w : RO ( G ) H ( G ) × .

Later in this paper, we shall determine the image of 𝑤 for G = SL ( 2 , q ) .

3 Quaternion groups

Our proof of Theorem 1.1 involves subgroups of SL ( 2 , q ) isomorphic to certain quaternion groups. In this section, we review the group cohomology of the quaternion group of order 8, and the so-called “generalized quaternions” Q 2 n . This will play a vital role in our detection theorem.

3.1 Orthogonal representations of 𝑄

Let 𝑄 be the quaternion group of order 8. If we write ℍ for the familiar real division algebra of quaternions, then 𝑄 can be quickly described as the subgroup of H × generated by 𝑖 and 𝑗.

There are 4 one-dimensional representations of 𝑄, which we denote by 1, χ 1 , χ 2 , χ 3 = χ 1 χ 2 . Each one is orthogonal. The group 𝑄 also possesses a unique 2-dimensional irreducible representation ρ : Q SL ( 2 , C ) defined by

ρ ( i ) = ( i 0 0 i ) , ρ ( j ) = ( 0 1 1 0 ) .

Of course, ℍ can be described as the algebra of complex matrices of the form

( s + t i u + v i u + v i s t i ) , where s , t , u , v R .

Since both ρ ( i ) , ρ ( j ) are of this form, 𝜌 is an injection of 𝑄 into H 1 , the subgroup of norm 1 quaternions. In particular, 𝜌 is symplectic. Thus, S ( ρ ) = ρ ρ is the only OIR of 𝑄, which is not irreducible.

3.2 The cohomology ring H * ( Q )

The SWCs of orthogonal representations of 𝑄 are certain elements in H * ( Q ) . Here we give a description of the cohomology ring H * ( Q ) with [1, Chapter IV] as our reference.

Recall that w 1 gives an isomorphism between Hom ( Q , ± 1 ) = { 1 , χ 1 , χ 2 , χ 3 } and H 1 ( Q ) . We define x := w 1 ( χ 1 ) and y := w 1 ( χ 2 ) .

The cohomology group H 4 ( Q ) is one-dimensional over Z / 2 Z , and we write “𝑒” for its non-zero element.

Proposition 3.1

Proposition 3.1 ([1, Section V.1])

The cohomology ring of 𝑄 is

H * ( Q ) Z / 2 Z [ x , y , e ] / ( x y + x 2 + y 2 , x 2 y + x y 2 ) .

The first few cohomology groups of 𝑄 are as follows:

H 0 ( Q ) = { 0 , 1 } , H 1 ( Q ) = { 0 , x , y , x + y } , H 2 ( Q ) = { 0 , x 2 , y 2 , x 2 + y 2 } , H 3 ( Q ) = { 0 , x 2 y } , H 4 ( Q ) = { 0 , e } .

Note that x 3 = y 3 = 0 . Moreover, one can obtain the higher cohomology groups via the cup product with 𝑒 due to Proposition 3.1. This means, for i 0 , the map

H i ( Q ) H i + 4 ( Q ) , z z e

is an isomorphism of groups.

3.3 SWCs of representations of 𝑄

We first compute the total SWCs of OIRs of 𝑄. For the linear orthogonal representations of 𝑄, it is clear that w ( 1 ) = 1 , w ( χ 1 ) = 1 + x , w ( χ 2 ) = 1 + y , and w ( χ 1 χ 2 ) = 1 + x + y with x , y H 1 ( Q ) from above.

Lemma 3.2

The total SWC of S ( ρ ) is w ( S ( ρ ) ) = 1 + e , where 𝑒 is the non-trivial element of H 4 ( Q ) .

Proof

From Lemma 2.3, we have

w i ( S ( ρ ) ) = 0 for i = 1 , 2 , 3 .

This gives w ( S ( ρ ) ) = 1 + w 4 ( S ( ρ ) ) . We now prove that w 4 ( S ( ρ ) ) = e H 4 ( Q ) .

Let 𝑍 be the center of 𝑄, which is { ± 1 } . Since

ρ ( 1 ) = ( 1 0 0 1 ) ,

we have the restriction res Z Q ρ = sgn sgn , where sgn : Z C × is the linear character of order 2.

From (2.2), we have H * ( Z ) Z / 2 Z [ v ] , where v = w 1 ( sgn ) . Then the multiplicativity of SWCs gives

w ( res Z Q S ( ρ ) ) = w ( sgn ) 4 = ( 1 + v ) 4 = 1 + v 4 ,

which implies w 4 ( S ( ρ ) ) 0 . Therefore, w 4 ( S ( ρ ) ) = e since this is the only nonzero element in H 4 ( Q ) . ∎

We also see from the above proof that 𝑒 maps to v 4 under the restriction

H 4 ( Q ) H 4 ( Z ) .

From this, we deduce that the restriction maps in degrees divisible by 4,

(3.1) H 4 i ( Q ) H 4 i ( Z ) , e i v 4 i

are isomorphisms.

Let 𝜋 be an orthogonal representation of 𝑄. By (2.1), we can write

π m 0 1 m 1 χ 1 m 2 χ 2 m 2 χ 3 m 4 S ( ρ ) ,

where m i are non-negative integers.

Lemma 3.3

Let 𝜋 be as above. Then, for 0 4 i deg π , we have

w 4 i ( π ) = ( m 4 i ) e i ,

where m 4 = 1 8 ( χ π ( 1 ) χ π ( 1 ) ) .

Proof

Let us consider

S = Z / 2 Z [ x , y ] / ( x y + x 2 + y 2 , x 2 y + x y 2 ) ,

which is a 6-dimensional subalgebra of H * ( Q ) . By the multiplicativity of SWCs, we have

w ( π ) = w ( χ 1 ) m 1 w ( χ 2 ) m 2 w ( χ 3 ) m 3 w ( S ( ρ ) ) m 4 = ( 1 + x ) m 1 ( 1 + y ) m 2 ( 1 + x + y ) m 3 S ( 1 + e ) m 4 .

Therefore, we can write ( 1 + x ) m 1 ( 1 + y ) m 2 ( 1 + x + y ) m 3 as a polynomial of the form P ( x , y ) = 1 + A x + B y + C x 2 + D y 2 + E x y 2 with coefficients in Z / 2 Z , and

w ( π ) = P ( x , y ) ( 1 + e ) m 4 = P ( x , y ) i = 0 m 4 ( m 4 i ) e i ,

where e i H 4 i ( Q ) for each 𝑖. Comparing degrees gives

w 4 i ( π ) = ( m 4 i ) e i .

To express m 4 in terms of character values, we simply evaluate χ π at 1 and −1. Since 1 ker ( χ i ) for i = 1 , 2 , 3 and χ ρ ( 1 ) = 2 , χ ρ ( 1 ) = 2 , we have the equations

χ π ( 1 ) = m 0 + m 1 + m 2 + m 3 + 4 m 4 , χ π ( 1 ) = m 0 + m 1 + m 2 + m 3 4 m 4 ,

and so m 4 = 1 8 ( χ π ( 1 ) χ π ( 1 ) ) . ∎

3.4 Generalized quaternions

The construction of the quaternion group 𝑄 generalizes to give a family of non-abelian groups which have the presentation

Q 2 n := a , b a 2 n 2 = b 2 , b 4 = 1 , b a b 1 = a 1 , n 3 .

These groups are called generalized quaternion groups and have order 2 n . Again, there are 4 linear (orthogonal) representations of Q 2 n , say 1 , ψ 1 , ψ 2 , ψ 3 . These can be defined on the generators of Q 2 n as

ψ 1 ( a ) = 1 , ψ 2 ( a ) = 1 , ψ 3 ( a ) = 1 , ψ 1 ( b ) = 1 , ψ 2 ( b ) = 1 , ψ 3 ( b ) = 1 .

Let ζ = e 2 π i / 2 n 1 . There is an irreducible 2-dimensional representation 𝜚 of Q 2 n defined by

ϱ ( a ) = ( ζ 0 0 ζ ¯ ) , ϱ ( b ) = ( 0 1 1 0 ) .

As earlier, 𝜚 maps Q 2 n into H 1 , so it is symplectic.

Let n > 3 . We use the isomorphism

w 1 : Hom ( Q 2 n , ± 1 ) H 1 ( Q 2 n ) , { 1 , ψ 1 , ψ 2 , ψ 3 } { 0 , X , Y , X + Y }

to define X = w 1 ( ψ 1 ) and Y = w 1 ( ψ 2 ) .

A description of the mod 2 cohomology ring of generalized quaternions Q 2 n for n > 3 in [1, Chapter IV, Lemma 2.11] is as follows:

(3.2) H * ( Q 2 n ) Z / 2 Z [ X , Y , E ] / ( X Y , X 3 + Y 3 ) ,

where E H 4 ( Q 2 n ) .

Lemma 3.4

We have E = w 4 ( S ( ϱ ) ) in H * ( Q 2 n ) .

Proof

This can be proved precisely as in Lemma 3.2; again, w ( S ( ϱ ) ) = 1 + E . ∎

Remark 3.5

Let n > 3 . Let i : Q Q 2 n be any group homomorphism. Then

i * : H 3 ( Q 2 n ) H 3 ( Q )

is the zero map.

This can be seen as follows. From (3.2), we can deduce H 3 ( Q 2 n ) = { 0 , X 3 } , and since i * is a ring homomorphism, we have the image

i * ( X ) H 1 ( Q ) = { 0 , x , y , x + y } .

But x 3 = y 3 = ( x + y ) 3 = 0 in H * ( Q ) , which implies

i * ( X 3 ) = ( i * ( X ) ) 3 = 0 .

Consider the subgroup Q ( 1 ) = a 2 n 3 , b Q 2 n . This subgroup is isomorphic to 𝑄 by i a 2 n 3 and j b . With this identification, it is easy to see that

res Q Q 2 n ϱ = ρ .

Write ι Q for this inclusion of 𝑄 into Q 2 n . Now

ι Q * ( E ) = ι Q * ( w 4 ( ϱ ) ) = w 4 ( res Q Q 2 n ϱ ) = w 4 ( ρ ) = e .

This means the homomorphism ι Q * : H * ( Q 2 n ) H * ( Q ) is an isomorphism in degree 4. Therefore, we have the following.

Proposition 3.6

With notation as above, we have isomorphisms

(3.3) ι Q * : H 4 i ( Q 2 n ) H 4 i ( Q ) , E i e i

for all i 0 .

4 SL ( 2 , q ) with 𝑞 odd

Let G = SL ( 2 , q ) throughout this section, with 𝑞 odd. Write “ 1 ” for the identity matrix; then the center 𝑍 of 𝐺 is { ± 1 } . We begin with a description of the mod 2 cohomology of 𝐺.

Proposition 4.1

Proposition 4.1 ([6, Chapter VI, Section 5])

When 𝑞 is odd, the mod 2 cohomology ring of SL ( 2 , q ) is

H * ( SL ( 2 , q ) ) Z / 2 Z [ e ] Z / 2 Z [ b ] / b 2

with deg ( b ) = 3 , deg ( e ) = 4 .

4.1 Detection

The proof of Theorem 1.1 uses the following well-known detection.

Lemma 4.2

Lemma 4.2 ([1, Corollary 5.2, Chapter II])

Let 𝐻 be a finite group. A Sylow 2-subgroup of 𝐻 detects its mod 2 cohomology.

According to [12, Chapter 2, Theorem 8.3], a Sylow 2-subgroup of 𝐺 is generalized quaternion. We will therefore regard Q 2 n as a subgroup of 𝐺, where of course 𝑛 is the highest power of 2 dividing | G | . We now prove our main detection theorem.

Proof of Theorem 1.1

We deduce from Proposition 4.1 that

H n ( G ) { Z / 2 Z , n 0 , 3 ( mod 4 ) , 0 otherwise .

Let 𝜋 be an orthogonal representation of 𝐺. Let n = 4 k + 3 for some 𝑘. With i = 1 , j = n 1 such that i + j = n , we now apply the Wu formula from Proposition 2.4,

Sq 1 ( w n 1 ( π ) ) = w 1 ( π ) w n 1 ( π ) + ( n 2 1 ) w 0 ( π ) w n ( π ) .

Here, Sq 1 ( w n 1 ( π ) ) = 0 because w n 1 ( π ) H 4 k + 2 ( G ) is zero and Sq 1 is a homomorphism. Also, w 1 ( π ) = 0 and ( n 2 ) is odd, which implies w n ( π ) = 0 when n 3 ( mod 4 ) . Therefore, the non-zero SWCs of representations of 𝐺 only occur in degrees divisible by 4, which means H SW * ( G ) Z / 2 Z [ e ] . Since Q 2 n is a 2-Sylow subgroup of 𝐺, it detects the mod 2 cohomology of 𝐺 by Lemma 4.2. Consider the Quaternion subgroup Q Q ( 1 ) Q 2 n . Note that the center of 𝑄 is 𝑍. By the isomorphisms (3.1) and (3.3), we obtain the following sequence of inclusions for each i 0 :

H 4 i ( G ) H 4 i ( Q 2 n ) H 4 i ( Q ) H 4 i ( Z ) , e i E i e i v 4 i .

Therefore, the subalgebra Z / 2 Z [ e ] , which contains the SWCs of 𝐺, injects into H * ( Z ) , completing the proof. ∎

4.2 Formulas for SWCs

We now prove Theorem 1.2 which gives an explicit formula for the total SWCs of orthogonal representations of 𝐺 in terms of character values.

Proof of Theorem 1.2

To find w ( π ) , it is enough to work with res Z G π due to the detection theorem, Theorem 1.1. This restriction has been done in two steps. We first restrict 𝜋 to the quaternion group Q G , and then further from 𝑄 to 𝑍.

With the notation from Section 3, it looks like

res Q G π m 0 1 m 1 χ 1 m 2 χ 2 m 3 χ 3 m 4 ( S ( ρ ) ) ,

where m i are non-negative integers. It is easy to see that

res Z Q χ i 1 for i = 1 , 2 , 3 , and res Z Q ρ sgn sgn .

Therefore, the further restriction of res Q G π to the center 𝑍 will be

res Z G π = res Z Q res Q G π ( m 0 + m 1 + m 2 + m 3 ) 1 4 m 4 ( sgn ) .

From Lemma 2.5, we then obtain

w ( res Z G π ) = ( 1 + v ) 4 m 4 = ( 1 + v 4 ) m 4 ,

with 4 m 4 = 1 2 ( χ π ( 1 ) χ π ( 1 ) ) . From the proof of Theorem 1.1, we have

i Z * ( e ) = v 4 ,

where i Z : Z G is the inclusion. Therefore, w ( π ) = ( 1 + e ) r π , where r π = m 4 is the multiplicity of S ( ρ ) in res Q G π . ∎

Example 4.3

We have w ( reg ( G ) ) = ( 1 + e ) 1 8 | G | .

4.3 Corollaries

We can go deeper by applying the following result due to R. Gow.

Theorem 4.4

Theorem 4.4 ([13, Theorem 1])

Let 𝜋 be an irreducible self-dual representation of 𝐺 with central character ω π . Then the Frobenius–Schur indicator ε ( π ) is equal to ω π ( 1 ) .

We simply call this equality Gow’s formula; it leads to the following corollary.

Corollary 4.5

Let 𝜋 be an irreducible orthogonal representation of 𝐺. Then its total SWC is w ( π ) = 1 .

Proof

For 𝜋 irreducible orthogonal, the sign is ε ( π ) = 1 by definition. Therefore,

r π = 1 8 ( χ π ( 1 ) χ π ( 1 ) ) = χ π ( 1 ) 8 ( 1 ω π ( 1 ) ) = 0 .

Let 𝜋 be an irreducible, non-orthogonal representation of 𝐺. Then, for the representation S ( π ) = π π , we have

r S ( π ) = 1 8 ( χ S ( π ) ( 1 ) χ S ( π ) ( 1 ) ) = 1 4 ( χ π ( 1 ) χ π ( 1 ) ) = χ π ( 1 ) 4 ( 1 ω π ( 1 ) ) .

Furthermore, for symplectic 𝜋, it turns out to be

(4.1) r S ( π ) = χ π ( 1 ) 2 = deg ( π ) 2

due to Gow’s formula.

Corollary 4.6

Let G = SL ( 2 , q ) with 𝑞 odd. Then the image of 𝑤 in (2.3) is

{ ( 1 + e ) n n Z } .

Proof

For q = 3 , there exists a unique irreducible symplectic representation π 0 of 𝐺 with degree 2. From (4.1), we obtain r S ( π 0 ) = 1 , and so w ( S ( π 0 ) ) = 1 + e .

For q > 3 , there exist irreducible symplectic representations π 1 and π 2 of 𝐺 of degrees q + 1 and q 1 respectively. (See Remark 4.7 for details.) From equation (4.1), we have

r S ( π 1 ) = q + 1 2 , r S ( π 2 ) = q 1 2

which are co-prime. So by Bézout’s identity, there exist integers a , b such that a ( q + 1 2 ) + b ( q 1 2 ) = 1 .

Therefore, there is a virtual representation π RO ( G ) with r π = 1 such that w ( π ) = 1 + e . Hence, the result follows from the multiplicativity of SWCs. ∎

Remark 4.7

For completeness, we give explicit descriptions of π 1 and π 2 . This entails recalling the construction of the principal series and irreducible cuspidal representations of 𝐺. The reader is referred to [8, 5] for more details.

Let T ~ be the diagonal subgroup, isomorphic to F q × × F q × , contained in the standard Borel subgroup B ~ of upper-triangular matrices of G ~ = GL ( 2 , q ) . When α , β are linear characters of F q × , we will write α β for the corresponding linear character of T ~ . Choose α : F q × C × satisfying

α ( 1 ) = 1 , α 2 1 .

One can inflate α 1 from T ~ to B ~ and then consider the usual complex parabolic induction π α := Ind B ~ G ~ ( α 1 ) . This is an irreducible principal series representation of G ~ of degree q + 1 .

We take π 1 = res G G ~ π α . This restriction is self-dual and irreducible. By Gow’s formula, π 1 is symplectic.

Let T ~ e be an elliptic torus of G ~ , thus isomorphic to F q 2 × . Let Z ~ be the center and 𝑁 the upper unitriangular subgroup of G ~ . Choose a linear character 𝜒 of T ~ e such that

χ q χ , χ 2 1 , χ ( 1 ) = 1 .

We fix a non-trivial character 𝜑 of 𝑁 and define a linear character of Z ~ N as χ φ ( z n ) = χ ( z ) φ ( n ) . Set

π χ = Ind Z ~ N G ~ χ φ Ind T ~ e G ~ χ .

This is an irreducible, cuspidal representation of G ~ of dimension q 1 .

When restricted to 𝐺, π χ remains irreducible and is called an irreducible cuspidal representation of 𝐺. (A representation of 𝐺 is called cuspidal, provided each of its irreducible constituents is irreducible cuspidal.)

Define π 2 = res G G ~ π χ . Again, one sees that π 2 is symplectic by Gow’s formula.

It is already known from Theorem 1.1 that H SW * ( G ) Z / 2 Z [ e ] . Here we make a stronger statement.

Corollary 4.8

Let G = SL ( 2 , q ) with 𝑞 odd. Then H SW * ( G ) = Z / 2 Z [ e ] .

Proof

For equality, we construct an orthogonal representation 𝜂 of 𝐺 such that w 4 ( η ) = e as follows. For q > 3 , consider the irreducible symplectic representations π 1 , π 2 of 𝐺 from Corollary 4.6. Let η = S ( π 1 ) S ( π 2 ) . It can easily be seen that r π π = r π + r π for any orthogonal π , π . Therefore, we have

r η = r S ( π 1 ) S ( π 2 ) = r S ( π 1 ) + r S ( π 2 ) = q + 1 2 + q 1 2 = q .

Since 𝑞 is odd, we have w ( η ) = ( 1 + e ) q = 1 + e + . Therefore, w 4 ( η ) = e .

Moreover, we already have w 4 ( S ( π 0 ) ) = e for q = 3 , which completes the proof. ∎

Next, we give a nonvanishing condition for the top SWC.

Corollary 4.9

Let G = SL ( 2 , q ) with 𝑞 odd. Let 𝜋 be an orthogonal representation of 𝐺. Then the following are equivalent.

  1. w top ( π ) 0 .

  2. π = S ( φ ) , where every irreducible constituent φ i of 𝜑 has central character satisfying ω φ i ( 1 ) = 1 .

  3. π ( 1 ) = 1 , meaning π ( 1 ) acts by the scalar −1.

Proof

We first prove (i) and (ii) are equivalent. Assume π = S ( φ ) = i = 1 r S ( φ i ) such that ω φ i ( 1 ) = 1 for all 1 i r .

Clearly, χ π ( 1 ) = 2 χ φ ( 1 ) , and since χ φ i ( 1 ) = ω φ i ( 1 ) χ φ i ( 1 ) = χ φ i ( 1 ) , we have

χ π ( 1 ) = 2 i = 1 r χ φ i ( 1 ) = 2 χ φ ( 1 ) .

This gives

r π = 1 2 χ φ ( 1 ) = 1 4 χ π ( 1 ) .

Therefore, we have w ( π ) = ( 1 + e ) 1 4 deg π , implying w top ( π ) = e 1 4 deg π 0 . For the converse, suppose w top ( π ) 0 . Since 𝜋 is orthogonal, we can write it as

π = i ρ i j S ( ϕ j ) k S ( φ k )

such that each ρ i is irreducible orthogonal, whereas ϕ j , φ k are irreducible non-orthogonal with ω ϕ j ( 1 ) = 1 for each 𝑗, and ω φ k ( 1 ) = 1 for each 𝑘.

From Theorem 1.2 and Corollary 4.5, we obtain

w ( π ) = k ( 1 + e ) deg φ k 2 = ( 1 + e ) deg φ 2 , where φ = k φ k .

Now the condition w top ( π ) 0 implies deg π = 4 deg φ 2 . Therefore,

i deg ρ i + 2 j deg ϕ j + 2 k deg φ k = 2 deg φ , i deg ρ i + 2 j deg ϕ j = 0 ,

which means ρ i and S ( ϕ j ) do not appear in 𝜋. Hence π = i S ( φ i ) , with each φ i irreducible and ω φ i ( 1 ) = 1 .

Next, suppose that π 1 , , π r are representations of 𝐺, and 𝜋 is their direct sum. Then 𝜋 satisfies condition (iii) if and only if each π i satisfies condition (iii). (Because a block matrix is equal to the negative of the identity matrix if and only if each block is the negative of the identity matrix.) In particular, this shows that (ii) implies (iii). By Gow’s formula, no irreducible orthogonal representation satisfies condition (iii), and so, by decomposing 𝜋, we see that (iii) implies (ii). ∎

For 𝜋 orthogonal, let k 0 be the least k > 0 such that w k ( π ) 0 . Then w k 0 ( π ) is known as the obstruction class of 𝜋, following [9].

Corollary 4.10

Let 𝜋 be an orthogonal representation of 𝐺. Put t = ord 2 ( r π ) . Then the obstruction class of 𝜋 is w 2 t + 2 ( π ) = e 2 t .

Proof

By Theorem 1.2,

w k ( π ) = { ( r π i ) e i , 0 k = 4 i deg π , 0 otherwise .

Therefore, the problem amounts to finding the smallest positive k = 4 i so that the binomial coefficient ( r π i ) is odd. This is an elementary application of Lucas’s Theorem [7]; proceeding as in [9, Proposition 3], we find that the smallest such 𝑘 is k = 2 t + 2 , giving the corollary. ∎

4.4 Relation with GL ( 2 , q )

Ganguly and Joshi compute in [9] SWCs for orthogonal representations 𝜋 of G ~ = GL ( 2 , q ) , with 𝑞 odd. Let us review their result here and see that it is harmonious with ours.

Their SWCs are identified with members of H * ( T ~ ) for the bicyclic group T ~ , isomorphic to C q 1 × C q 1 . When q 3 ( mod 4 ) , the cohomology is generated by elements v 1 , v 2 of degree 1, by Künneth. When q 1 ( mod 4 ) , it is generated by elements s 1 , s 2 , t 1 , t 2 , where deg s i = 1 and deg t i = 2 . Put δ = 0 if det π = 1 and δ = 1 otherwise.

In these terms, the total SWC of 𝜋 is

(4.2) w ( π ) = { ( 1 + δ ( s 1 + s 2 ) ) ( 1 + t 1 + t 2 + t 1 t 2 ) r π ( 1 + t 1 + t 2 ) s π / 2 , q 1 ( mod 4 ) , ( 1 + v 1 2 + v 2 2 + v 1 2 v 2 2 ) r π ( 1 + v 1 + v 2 ) s π , q 3 ( mod 4 ) ,

for a certain integer s π , and r π = 1 8 ( χ π ( 1 ) χ π ( 1 ) ) as above.

Our two papers are compatible via the following diagram, formed from the restriction maps on cohomology:

The right-hand side of (4.2) lies in H * ( T ~ ) . The left map is injective by Quillen’s work, and the right map is injective on SWCs by Theorem 1.1. The lower map H * ( T ~ ) H * ( Z ) maps v i to 𝑣 for q 3 ( mod 4 ) , and when q 1 ( mod 4 ) , it maps s i to 0 and t i to v 2 . This gives w ( π | Z ) = ( 1 + v 4 ) r π in all cases. Thus, for orthogonal representations of 𝐺 which extend to orthogonal representations of G ~ , Theorem 1.2 agrees with the main result of [9].

Remark 4.11

Not every orthogonal representation of 𝐺 extends to G ~ . For instance, when q 1 ( mod 4 ) , the representation π = Ind B ~ G ~ ( sgn 1 ) (with B ~ the upper triangular subgroup of G ~ ), when restricted to 𝐺, is the sum of two irreducible orthogonal representations, neither of which extend to G ~ .

5 SL ( 2 , q ) with 𝑞 even

Let G = SL ( 2 , q ) with q = 2 r throughout this section. Recall that we write 𝑁 for the subgroup of upper unitriangular matrices. It is well known that this is a Sylow 2-subgroup of 𝐺, and therefore 𝑁 detects the mod 2 cohomology of 𝐺 by Lemma 4.2. All representations of 𝐺 are orthogonal by the main result in [21].

5.1 Formulas for SWCs

The subgroup 𝑁 is an elementary abelian 2-group of rank 𝑟, so as in Section 2.5, the mod 2 cohomology ring of N C 2 r may be written as

H * ( N ) H * ( C 2 r ) Z / 2 Z [ v 1 , v 2 , , v r ] .

Let 𝑇 be the subgroup of diagonal matrices in 𝐺. That is

T = { ( a 0 0 a 1 ) : a F q × } .

The conjugation action of 𝑇 on 𝑁 is equivalent to the action of F q × on F q through multiplication by squares. Since F q × has odd order, this action is transitive on F q { 0 } . Therefore, we have the following.

Lemma 5.1

𝑇 acts transitively on the non-trivial linear characters of 𝑁.

Let N ^ = Hom ( N , C × ) , the character group of 𝑁. From the above lemma, the 𝑇-orbits of N ^ are { 1 } , { χ : χ 1 } . Let us define

reg ( N ) = reg ( N ) 1 = χ 1 χ .

Let 𝜋 be a representation of 𝐺. Since res N G π is 𝑇-invariant, it is of the form

(5.1) res N G π π 1 m π reg ( N ) ,

where π , m π are non-negative integers.

Lemma 5.2

Let 𝜋 be a non-trivial irreducible representation of 𝐺. Then m π = 1 .

Proof

For r 2 , it is known that 𝐺 has no non-trivial normal subgroups. For non-trivial 𝜋, we must have m π 1 because ker ( π ) = 1 and N ker ( π ) . Now, from (5.1), we have

deg π = π + m π ( q 1 ) .

If m π > 1 , then the sum π + m π ( q 1 ) would be greater than the highest possible degree for an irreducible representation of 𝐺, which is ( q + 1 ) . So actually m π = 1 .

For r = 1 , we have SL ( 2 , 2 ) S 3 with only two non-trivial irreducible representations. That is 𝜋 is either the “sgn” representation or the 2-dimensional standard representation of S 3 . Here we can see from direct calculations that m π = 1 . ∎

It follows that m π = dim C ( V / V G ) , where 𝑉 denotes the representation space of 𝜋. It is also the number of non-trivial irreducible constituents of 𝜋. We can get a character formula for m π by taking character values at n 0 = ( 1 1 0 1 ) N . In fact,

χ π ( 1 ) = π + ( q 1 ) m π and χ π ( n 0 ) = π m π

so that m π = 1 q ( χ π ( 1 ) χ π ( n 0 ) ) .

We are now ready to describe the SWCs of representations of 𝐺. Since 𝑁 is a detecting subgroup, we may and will identify w ( π ) with its image in H * ( N ) .

Theorem 5.3

Let q = 2 r . Let 𝜋 be a representation of SL ( 2 , q ) . Then the total SWC of 𝜋 is

w ( π ) = ( v H 1 ( N ) ( 1 + v ) ) m π .

Proof

The restriction res N G π , from (5.1), is of the form

res N G π ( π m π ) 1 m π reg ( N ) .

Since reg ( N ) = χ N ^ χ , we use the isomorphism between N ^ and H 1 ( N ) and the multiplicativity of SWCs to obtain

w ( res N G π ) = w ( reg ( N ) ) m π = ( v H 1 ( N ) ( 1 + v ) ) m π .

Remark 5.4

The formula in Theorem 5.3 above is also valid for G ~ = GL ( 2 , q ) with 𝑞 even since 𝑁 is also a Sylow 2-subgroup of G ~ . Thus, this result in some sense completes [9].

5.2 Dickson invariants

The expansion of the product above is well known. We have

v H 1 ( N ) ( 1 + v ) = 1 + i = 1 r d i H * ( N ) ,

where d i are Dickson invariants in the algebra H * ( N ) .

We digress for a moment to recount the theory of Dickson invariants for mod 2 spaces. Let 𝐸 be an F 2 -vector space. The ring of polynomials from 𝐸 to F 2 can be identified with the symmetric algebra S [ E ] on the dual space E . The linear group GL ( E ) acts on S [ E ] via the contragradient map. It is natural to look for the invariants under this action.

Theorem 5.5

Theorem 5.5 ([23])

Let dim ( E ) = r . Then the ring of invariants S [ E ] GL ( E ) is a polynomial algebra generated by elements d i called Dickson invariants, for 1 i r . The polynomial d i has degree 2 r 2 r i . Moreover,

v E ( 1 + v ) = 1 + i = 1 r d i S [ E ] .

These invariants are described explicitly in terms of certain determinants. (See [23] or [1, Chapter III] for instance.)

Let us illustrate with some examples. If E = F 2 , then S [ E ] is a polynomial algebra with only one generator 𝑣, that is S [ E ] Z / 2 Z [ v ] . Here d 1 = v giving the ring of invariants

S [ E ] GL ( V ) Z / 2 Z [ v ] GL ( 1 , 2 ) = Z / 2 Z [ v ] .

Also, Theorem 5.3 for G = SL ( 2 , 2 ) and π 1 irreducible says that

w ( π ) = 1 + v = 1 + d 1 .

Next, suppose dim E = 2 . Then S [ E ] is a polynomial algebra with two generators, say v 1 , v 2 such that S [ E ] Z / 2 Z [ v 1 , v 2 ] . Here the ring of invariants S [ E ] GL ( E ) Z / 2 Z [ v 1 , v 2 ] GL ( 2 , 2 ) is generated by

d 1 = v 1 2 + v 2 2 + v 1 v 2 , d 2 = v 1 v 2 ( v 1 + v 2 ) .

Theorem 5.3 gives the following: for G = SL ( 2 , 4 ) , the total SWC of a non-trivial irreducible representation 𝜋 of 𝐺 is w ( π ) = 1 + d 1 + d 2 .

Now let D = i = 1 r d i be the sum of the Dickson invariants so that we can succinctly write w ( π ) = ( 1 + D ) m π , which is Theorem 1.3 from the introduction.

Example 5.6

We have w ( reg ( G ) ) = ( 1 + D ) q 2 1 .

5.3 Corollaries

Now we prove the corollaries mentioned in the introduction.

Corollary 5.7

Let G = SL ( 2 , q ) with even 𝑞. Then the image of 𝑤 in (2.3) is

{ ( 1 + D ) n n Z } .

Proof

Let 𝜋 be a non-trivial irreducible representation of 𝐺. Then its total SWC is w ( π ) = 1 + D since m π = 1 by Lemma 5.2. With the virtual representation n π , we obtain ( 1 + D ) n in the image of 𝑤 for each n Z . ∎

The above proof also gives the following corollary.

Corollary 5.8

Let G = SL ( 2 , q ) with q = 2 r . Then

H SW * ( G ) = Z / 2 Z [ d 1 , , d r ] .

Corollary 5.9

Let G = SL ( 2 , q ) with 𝑞 even. Let ( π , V ) be a representation of 𝐺. Then w top ( π ) 0 if and only if V N = { 0 } .

Proof

From the preceding, we have w top ( reg ( N ) ) = d r since this invariant has degree q 1 . The highest degree term of w ( π ) is therefore d r m π , which has degree m π ( q 1 ) ; this is the degree of 𝜋 if and only if π = 0 if and only if V N = { 0 } . ∎

Remark 5.10

A representation 𝜋 of SL ( 2 , q ) is cuspidal if and only if V N = { 0 } . (See [4, page 410].)

Corollary 5.11

Let G = SL ( 2 , q ) with q = 2 r . Let 𝜋 be a representation of 𝐺. Put s = ord 2 ( m π ) . Then the obstruction class of 𝜋 is equal to w 2 r + s 1 ( π ) = d 1 2 s .

Proof

From Theorem 1.3, we have

w ( π ) = i = 0 m π ( m π i ) D i .

As in Corollary 4.10, we can say that ( m π 2 s ) is the first odd binomial coefficient appearing in the above sum. By expanding the term

( m π 2 s ) D 2 s = ( m π 2 s ) ( d 1 2 s + + d r 1 2 s + d r 2 s ) ,

we can deduce that ( m π 2 s ) d 1 2 s has the least degree, which is ( 2 r 1 2 s ) . Therefore, the least k > 0 such that w k ( π ) 0 is 2 r + s 1 , as claimed. ∎

Funding statement: The first author gratefully acknowledges the Ph.D. fellowship provided by the Council of Scientific and Industrial Research, India, during this work.

Acknowledgements

This paper comes out of the first author’s Ph.D. thesis [17] at IISER Pune. The authors would like to thank Ryan Vinroot, Dipendra Prasad, and Rohit Joshi for helpful discussions.

  1. Communicated by: Olivier Dudas

References

[1] A. Adem and R. J. Milgram, Cohomology of Finite Groups, Grundlehren Math. Wiss. 309, Springer, Berlin, 2004. 10.1007/978-3-662-06280-7Search in Google Scholar

[2] D. J. Benson, Representations and Cohomology. II: Cohomology of Groups and Modules, Cambridge Stud. Adv. Math. 31, Cambridge University, Cambridge, 1998. Search in Google Scholar

[3] T. Bröcker and T. tom Dieck, Representations of Compact Lie Groups, Grad. Texts in Math. 98, Springer, New York, 1995. Search in Google Scholar

[4] D. Bump, Automorphic Forms and Representations, Cambridge Stud. Adv. Math. 55, Cambridge University, Cambridge, 1998. 10.1017/CBO9780511609572Search in Google Scholar

[5] C. J. Bushnell and G. Henniart, The Local Langlands Conjecture for GL ( 2 ) , Grundlehren Math. Wiss. 335, Springer, Berlin, 2006. 10.1007/3-540-31511-XSearch in Google Scholar

[6] Z. Fiedorowicz and S. Priddy, Homology of Classical Groups Over Finite Fields and Their Associated Infinite Loop Spaces, Lecture Notes in Math. 674, Springer, Berlin, 2006. Search in Google Scholar

[7] N. J. Fine, Binomial coefficients modulo a prime, Amer. Math. Monthly 54 (1947), 589–592. 10.2307/2304500Search in Google Scholar

[8] W. Fulton and J. Harris, Representation Theory. A First Course, Grad. Texts in Math. 129, Springer, New York, 1991. Search in Google Scholar

[9] J. Ganguly and R. Joshi, Stiefel Whitney classes for real representations of GL 2 ( F q ) , Internat. J. Math. 33 (2022), no. 1, Paper No. 2250010. 10.1142/S0129167X22500100Search in Google Scholar

[10] J. Ganguly and R. Joshi, Total Stiefel–Whitney classes for real representations of GL n over F q , R and ℂ, Res. Math. Sci., to appear. Search in Google Scholar

[11] J. Ganguly and S. Spallone, Spinorial representations of symmetric groups, J. Algebra 544 (2020), 29–46. 10.1016/j.jalgebra.2019.09.025Search in Google Scholar

[12] D. Gorenstein, Finite Groups, 2nd ed., Chelsea, New York, 1980. Search in Google Scholar

[13] R. Gow, Real representations of the finite orthogonal and symplectic groups of odd characteristic, J. Algebra 96 (1985), no. 1, 249–274. 10.1016/0021-8693(85)90049-3Search in Google Scholar

[14] P. Guillot, The computation of Stiefel–Whitney classes, Ann. Inst. Fourier (Grenoble) 60 (2010), no. 2, 565–606. 10.5802/aif.2533Search in Google Scholar

[15] J. Gunarwardena, B. Kahn and C. Thomas, Stiefel–Whitney classes of real representations of finite groups, J. Algebra 126 (1989), no. 2, 327–347. 10.1016/0021-8693(89)90309-8Search in Google Scholar

[16] F. Kamber and P. Tondeur, Flat bundles and characteristic classes of group-representations, Amer. J. Math. 89 (1967), 857–886. 10.2307/2373408Search in Google Scholar

[17] N. Malik, Stiefel–Whitney classes of representations of some finite groups of Lie type, Ph.D. thesis, Indian Institute of Science Education and Research Pune, 2022. Search in Google Scholar

[18] J. P. May, A Concise Course in Algebraic Topology, Chic. Lectures in Math., University of Chicago, Chicago, 1999. Search in Google Scholar

[19] J. W. Milnor and J. D. Stasheff, Characteristic Classes, Ann. of Math. Stud. 76, Princeton University, Princeton, 2016. Search in Google Scholar

[20] D. Quillen, On the cohomology and 𝐾-theory of the general linear groups over a finite field, Ann. of Math. (2) 96 (1972), 552–586. 10.2307/1970825Search in Google Scholar

[21] C. R. Vinroot, Real representations of finite symplectic groups over fields of characteristic two, Int. Math. Res. Not. IMRN 2020 (2020), no. 5, 1281–1299. 10.1093/imrn/rny047Search in Google Scholar

[22] C. A. Weibel, The 𝐾-Book: An Introduction to Algebraic 𝐾-theory, Grad. Stud. Math. 145, American Mathematical Society, Providence, 2013. Search in Google Scholar

[23] C. Wilkerson, A primer on the Dickson invariants, Proceedings of the Northwestern Homotopy Theory Conference, Contemp. Math. 19, American Mathematical Society, Providence (1983), 421–434. 10.1090/conm/019/711066Search in Google Scholar

Received: 2022-09-15
Revised: 2023-01-10
Published Online: 2023-02-28
Published in Print: 2023-09-01

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