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Maximal antipodal sets of G 2 and G 2 /SO (4) and related geometry

Makiko Sumi Tanaka ∗ , Hiroyuki Tasaki and Osami Yasukura

The 22nd International Workshop on Differential Geometry of Submanifolds in Symmetric Spaces 

July 31–August 5, 2019

Kyungpook National University, Korea

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Contents

1. Introduction 2. Polars

3. Maximal antipodal sets of G 2 and G 2 /SO (4) 4. Explicit descriptions of maximal antipo-

dal sets

5. G 2 /SO (4) as an oriented real Grassmann

manifold

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1. Introduction

M : a compact Riemannian symmetric space s x : the geodesic symmetry at x ∈ M

S ⊂ M : a subset

S : an antipodal set ⇐⇒ ∀ def x, y ∈ S, s x ( y ) = y the 2-number of M

# 2 M := max {| S | | S ⊂ M : an antipodal set } S : a great antipodal set ⇐⇒ | def S | = # 2 M

(Chen-Nagano)

Theorem A (Takeuchi 1989)

If M is a symmetric R -space, # 2 M coincides

with the sum of the Z 2 -Betti numbers of M .

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Theorem B (Tanaka-Tasaki 2013) M : a symmetric R -space

(1) Any antipodal set of M is included in a great antipodal set.

(2) Any two great antipodal sets are con- gruent, that is, if A, A ′ are great antipodal sets, there is g ∈ I 0 ( M ), the identity compo- nent of the group of isometries of M , such that A ′ = gA .

G 2 , G 2 /SO (4) are not symmetric R -spaces.

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2. Polars

M : a compact connected Riemnnian sym- metric space, o ∈ M

A connected component of

F ( s o , M ) := { p ∈ M | s o ( p ) = p } is called a polar of M w.r.t. o .

F ( s o , M ) =

∪

k

i =0

M i + , M i + : a polar, M 0 + = { o } dim M i + > 0 ⇒ a totally geodesic submanifold A : an antipodal set of M

o ∈ A ⇒ A ⊂ F ( s o , M )

A ∩ M i + ̸ = ∅ ⇒ an antipodal set of M i +

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G := I 0 ( M )

K := { g ∈ G | go = o } , M = ∼ G/K K 0 : the identity component of K M i + = K 0 x i ( x i ∈ M i + )

I 0 ( M i + ) = { k | M

+

i

| k ∈ K 0 }

Proposition 1 When F ( s o , M ) = { o } ∪ M 1 + ,

the assignment A 7→ { o } ∪ A from the set

of maximal antipodal sets in M 1 + to that

of in M induces a bijection between their

congruence classes.

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S i m : m -dim sphere with radius r i ( i = 1 , 2) S 1 m × S 2 m : a Riemannian symmetric space s ( x

1

,x

2

) ( y 1 , y 2 ) = ( s x

1

( y 1 ) , s x

2

( y 2 )) ( x i , y i ∈ S i m ) Z 2 = { 1 , − 1 } ↷ S 1 m × S 2 m

− 1 acts as ( x 1 , x 2 ) 7→ ( − x 1 , − x 2 )

S 1 m × S 2 m ∈ ( x 1 , x 2 ) 7→ [ x 1 , x 2 ] ∈ ( S 1 m × S 2 m ) / Z 2 : the natural projection

( S 1 m × S 2 m ) / Z 2 : a Riem. symmetric space s [ x

1

,x

2

] [ y 1 , y 2 ] = [ s x

1

( y 1 ) , s x

2

( y 2 )] ( x i , y i ∈ S i m )

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By Proposition 1 we obtain :

Lemma 2 Let { e 1 . . . . , e m +1 } ⊂ S 1 m and { f 1 , . . . , f m +1 } ⊂ S 2 m be orthogonal frames of R m +1 . Any maximal antipodal set of ( S 1 m × S 2 m ) / Z 2

is congruent to { [ e 1 , ± f 1 ] , . . . , [ e m +1 , ± f m +1 ] }

and # 2 ( S 1 m × S 2 m ) / Z 2 = 2( m + 1).

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3. Maximal antipodal sets of G 2 and G 2 /SO (4) G 2 : a compact connected Lie group whose

root system is of type G 2 e : the identity element

F ( s e , G 2 ) = { e } ∪ M 1 + , M 1 + = ∼ G 2 /SO (4) o ∈ M 1 +

F ( s o , M 1 + ) = { o } ∪ M 1 + , 1 , M 1 + , 1 = (S ∼ 2 × S 2 ) / Z 2

G : a compact Lie group s x ( y ) = xy − 1 x ( x, y ∈ G )

A ⊂ G : a maximal antipodal set

e ∈ A ⇒ A : a subgroup = ∼ Z 2 × · · · × Z 2

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By Proposition 1 :

Theorem 3 (1) A maximal antipodal set of G 2 /SO (4) is congruent to { o } ∪ A for a max- imal antipodal set A of M 1 + , 1 = (S ∼ 2 × S 2 ) / Z 2

given in Lemma 2. Hence { o } ∪ A is a great antipodal set and # 2 G 2 /SO (4) = 7.

(2) A maximal antipodal subgroup of G 2 is conjugate to { e } ∪ A ′ for a maximal antipo- dal set A ′ of M 1 + = ∼ G 2 /SO (4) given in (1).

Hence { e }∪ A ′ is a great antipodal subgroup

and # 2 G 2 = 8.

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4. Explicit descriptions of maximal antipo- dal sets

O : the octonions

O = H × H , ( m, a ) , ( n, b ) ∈ O ( m, a )( n, b ) = ( mn − ¯ ba, a ¯ n + bm ) H , → O , H ∋ m 7→ ( m, 0) ∈ O

Aut( O )

= { α ∈ GL R ( O ) | α ( xy ) = ( αx )( αy ) , x, y ∈ O} :

a compact connected Lie group of type G 2

G 2 = Aut( id O )

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Sp (1) = { p ∈ H | | p | = 1 }

ψ : Sp (1) × Sp (1) → GL R ( O )

ψ ( p, q )( m, a ) := ( qm q, pa ¯ q ¯ )

( p, q ∈ Sp (1) , m, a ∈ H ) (Yokota) ψ is a homomorphism, Im ψ ⊂ G 2

The following is showed by Yokota :  

・ Im ψ = Z ψ (1 , − 1) ( G 2 ) : the centralizer

・ Z ψ (1 , − 1) ( G 2 ) = ( ∼ Sp (1) × Sp (1)) / {± (1 , 1) } ∼ = SO (4)

Im ψ = id SO (4)

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F ( s e , G 2 ) = { e } ∪ M 1 +

ψ (1 , − 1) 2 = e , i.e., s e ( ψ (1 , − 1)) = ψ (1 , − 1) M 1 + = { g ψ (1 , − 1) g − 1 | g ∈ G 2 } ∼ = G 2 /SO (4)

o = ψ (1 , − 1) ∈ M 1 +

F ( s o , M 1 + ) = { o } ∪ M 1 + , 1

M 1 + , 1 = { ψ ( p, q ) | p 2 = q 2 = − 1 }

M 1 + , 1 = ( ∼ S 2 × S 2 ) / Z 2 where S 2 = { x ∈ Sp (1) |

x 2 = − 1 }

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A maximal antipodal set of M 1 + , 1 is congru- ent to { ψ ( i , ± i ) , ψ ( j , ± j ) , ψ ( k , ± k ) } where i , j , k

are elements of the standard basis of H .

A maximal antipodal set of M 1 + is congru- ent to { ψ (1 , − 1) , ψ ( i , ± i ) , ψ ( j , ± j ) , ψ ( k , ± k ) } .

A maximal antipodal subgroup of G 2 is con-

jugate to { ψ (1 , ± 1) , ψ ( i , ± i ) , ψ ( j , ± j ) , ψ ( k , ± k ) } ( = ∼

Z 2 × Z 2 × Z 2 ) ⊂ SO (4).

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5. G 2 /SO (4) as an oriented real Grassmann manifold

H : a quaternion subalgebra of O

{ 1 } ⊥ in H is a canonically oriented 3-plane in Im O = Im H × H = ∼ R 7 , called an associative 3-plane.

G ˜ ass : the set of associative 3-planes in Im O G ˜ ass ⊂ G ˜ 3 ( R 7 ) : totally geodesic

G ˜ ass = ∼ G 2 /SO (4) (Harvey-Lawson)

M 1 + = ˜ ∼ G ass by ξ 7→ V ( ξ ) = { x ∈ Im O | ξx = x }

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The classification of maximal antipodal sets of G ˜ 3 ( R 7 ) is given by Tasaki.

[7] = { 1 , 2 , 3 , 4 , 5 , 6 , 7 }

(

[7]

3

)

= { α ⊂ [7] | | α | = 3 }

A ⊂ [7] : an antipodal set def ⇔ ∀ α, β ∈

(

[7] 3

)

, | α \ β | : even

A ⊂

(

[7] 3

)

: a maximal antipodal set

e 1 , . . . , e 7 : an orthonormal basis of R 7

⇒ {±⟨ e α

1

, e α

2

, e α

3

⟩ R | { α 1 , α 2 , α 3 } ∈ A } is a max- imal antipodal set of G ˜ 3 ( R 7 ), and vice versa.

The set of maximal antipodal sets of

(

[7]

3

)

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coincides with the set of lines of the Fano plane under the actions of permutations.

1

2

3

4

5 7

6

A maximal antipodal set of M 1 + = G 2 /SO (4)

↔ a maximal antipodal set A of G ˜ ass

→ a maximal antipodal set {± α | α ∈ A } of G ˜ 3 ( R 7 )

↔ the set of lines of the Fano plane

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Thank you for your kind attention.

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