Boseck Lie Superalgebras & Lie Supergroups I [sharethefiles com]

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Seminar Sophus Lie

1

(1991) 109{122

Lie

Sup

eralgebras

and

Lie

Sup

ergroups,

I

Helmut Boseck

1. Graded Algebras

Let

K

denote the base eld.

K

is assumed to be of characteristic zero.

In the examples

K

is the eld of real or complex numbers.

Let

Z

denote the additive group of the integers. A

Z

-graded linear space

is a

K

-linear space

V

and a family of subspaces

V

k

, (

k

= 0 1 2

:::

) such

that

V

=

M

k

2Z

V

k

:

A

Z

-graded associative algebra

is an associative

K

-algebra

A

, which is

Z

-graded

as a

K

-linear space

A

=

M

k

2Z

A

k

such that

A

k

A

l

A

k

+

`

(

k l

2

Z

)

:

The elements of

A

k

are called

homogeneous of degree

k

.

Example 1

.

Let

V

=

L

k

2Z

V

k

be a

Z

-graded linear space. A linear operator

A

:

V

k

;

!

V

k

+

l

(

k

2

Z

) is called

homogeneous of degree

`

. If

L

`

(

V

) denotes the

space of linear operators of degree

`

, then

L

0

(

V

) =

M

k

2Z

L

k

(

V

)

is a

Z

-graded associative algebra with unit. If

V

is nite dimensional we have

L

(

V

) =

M

k

2Z

L

k

(

V

)

:

Assume

V

to be nite dimensional and

V

k

=

f

0

g

, (

k

=

;

1 2 3

:::

),

V

=

V

0

V

1

:

Then the following relations hold

L

0

(

V

) =

L

(

V

0

)

L

(

V

1

)

L

;1

(

V

) =

L

(

V

1

V

0

)

L

1

(

V

) =

L

(

V

0

V

1

) and

L

k

(

V

) =

f

0

g

(

k

= 2 3

:::

)

:

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110

Boseck

Chosing a basis of homogeneous elements in

V

we may represent the elements

of

L

0

(

V

) by diagonal block matrices

(1)

A

0

0

0

A

1

:

The elements of

L

;1

(

V

) and

L

1

(

V

) become represented by the block matrices

(2)

0

B

1

0 0

and 0 0

B

0

0

respectively.

Example 2

.

Let (

n

) = (

y

1

::: y

n

) denote the exterior or

Grassmann

algebra with

n

generators, which are assumed to be homogeneous of degree 1 .

Put

0

=

K

1

= span

f

y

1

::: y

n

g

k

= span

f

y

i

1

y

i

k

: 1

i

1

<

< i

k

n

g

(

k

= 2

::: n

;

1)

n

= span

f

y

1

y

n

g

`

=

f

0

g

if

`

=

;

1

;

2

:::

or

`

=

n

+ 1

n

+ 2

:::

then we have

(

n

) =

0

1

n

and (

n

) becomes a

Z

-graded associative algebra with unit. The

Z

-graded

algebra (

n

) is (

graded

)

commutative

, i.e., for homogeneous elements

a

k

2

k

,

a

`

2

`

the following equation holds:

a

`

a

k

= (

;

1)

k`

a

k

a

`

:

Example 3

.

Let

A

=

L

k

2Z

A

k

be a

Z

-graded associative algebra with unit.

We dene a new product by

a

k

a

`

] =

a

k

a

`

;

(

;

1)

k`

a

`

a

k

a

k

2

A

k

:

With respect to that multiplication

A

becomes a

Z

-graded

Lie

algebra

A

L

=

M

k

2Z

A

k

:

We have

(3)

a

`

a

k

] =

;

(

;

1)

k`

a

k

a

`

]

and the modied

Jacobi

identity

(4)

(

;

1)

km

a

k

a

`

a

m

]] + (

;

1)

`k

a

`

a

m

a

k

]] + (

;

1)

m`

a

m

a

k

a

`

]] = 0

:

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Boseck

111

A

Z

-graded

Lie

algebra is a

Z

-graded linear space

L

=

L

k

2Z

L

k

with a bracket multiplication compatible with the grading

L

k

L

`

]

L

k

+

`

and

satisfying (3) and (4) for homogeneous elements.

Let

Z

2

=

Z

=

(2) =

f

0 1

g

denote the additive group of two elements. A

Z

2

-graded linear space is a

K

-linear space

V

with two distinguished subspaces

V

0

and

V

1

such that

V

=

V

0

V

1

holds. The elements of

V

0

are called

even

,

those of

V

1

are called

odd

. A homogeneous element is either even or odd.

Every

Z

-graded linear space admits a canonical

Z

2

-gradation by

V

0

=

L

k

2Z

V

2

k

,

V

1

=

L

k

2Z

V

2

k

+1

.

A

Z

2

-graded associative algebra or an associative

superalgebra

is a

K

-

algebra, which is

Z

2

-graded as a linear space

A

=

A

0

A

1

such that the multiplication satises

A

0

A

0

A

0

A

1

A

1

A

0

A

0

A

1

A

1

A

1

A

0

A

1

:

Every

Z

-graded algebra

A

admits a canonical

Z

2

-gradation by

A

0

=

M

k

2Z

A

2

k

A

1

=

M

k

2Z

A

2

k

+1

:

Example 4

.

Let

V

=

V

0

V

1

denote a

Z

2

-graded linear space. A linear

operator

A

on

V

is called

paritiy preserving

or

even

, if it satises

A

:

V

0

!

V

0

and

A

:

V

1

!

V

1

. The operator

A

is called

parity reversing

or

odd

if

A

:

V

0

!

V

1

and

A

:

V

1

!

V

0

. By

L

0

(

V

) and

L

1

(

V

) we denote the linear space of even and

odd linear operators on

V

, respectively.

L

0

(

V

) =

L

0

(

V

)

L

1

(

V

)

is a

Z

2

-graded associative algebra with unit. If

V

is nite dimensional then

L

(

V

) =

L

0

(

V

)

L

1

(

V

)

holds and

L

0

(

V

)

=

L

(

V

0

)

L

(

V

1

)

L

1

=

L

(

V

0

V

1

)

L

(

V

1

V

0

)

:

Choosing a basis of homogeneous elements in

V

, the elements of

L

0

(

V

)

are represented by diagonal block matrices as in (1), while the elements of

L

1

(

V

)

are represented by block matrices of the following type

0

B

1

B

0

0

:

Example 5

.

The

Grassmann

algebra (

n

) admits a canonical

Z

2

-grading

with respect to a chosen system of generators (

n

) =

0

1

with

0

=

0

2

,

1

=

1

3

Now (

n

) is a

Z

2

-graded associative

and (graded) commutative algebra with unit or, equivalently, an associative,

commutative superalgebra with unit.

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112

Boseck

Example 6

.

Let

A

=

A

0

A

1

denote a

Z

2

-graded associative algebra with

unit. We dene brackets by

a b

] =

ab

;

(

;

1)

j

a

jj

b

j

ba

for homogeneous elements

a b

2

A

. Dene the parity

j

a

j

as follows:

j

a

j

=

0 if

a

2

A

0

,

1 if

a

2

A

1

.

With respect to the brackets,

A

becomes a

Z

2

-graded

Lie

algebra or,equivalently,

a

Lie

superalgebra

A

L

=

A

0

A

1

:

For homogeneous elements

a b c

2

A

the

following equations hold:
(4)

b a

] =

;

(

;

1)

j

a

jj

b

j

a b

]

(5)

(

;

1)

j

a

jj

c

j

a

b c

]] + (

;

1)

j

b

jj

a

j

b

c a

]] + (

;

1)

j

c

jj

b

j

c

a b

]] = 0

(the modied

Jacobi

equation). A

Z

2

-graded

Lie

algebra or

Lie

superalgebra

is a

Z

2

-graded linear space

L

=

L

0

L

1

with a bracket multiplication

]

compatible with the gradation

L

0

L

0

]

L

0

L

1

L

1

]

L

0

L

0

L

1

]

L

1

L

1

L

0

]

L

1

and satisfying (4) and (5).

2. L

IE

Superalgebras:

The series A, B, C, D, Q

Let

L

=

L

0

L

1

denote a

Z

2

-graded

Lie

algebra. Its even part

L

0

is

a

Lie

algebra. In view of

L

0

L

1

]

L

1

, multiplication of odd elements by even

ones denes a representation ad

0

of the

Lie

algebra

L

0

on the linear space

L

1

(ad

0

x

0

)

x

1

=

x

0

x

1

]

x

0

2

L

0

x

1

2

L

1

:

ad

0

is called the

adjoint representation of the even part

L

0

on the odd part

L

1

:

A

Z

2

-graded

Lie

algebra

L

=

L

0

L

1

is called

simple

, if there are no

nontrivial

Z

2

-graded ideals: If

I

=

I

0

I

1

denotes a

Z

2

-graded ideal of

L

then

we have

I

=

f

0

g

or

I

=

L

. A simple

Z

2

-graded

Lie

algebra is called

classical

, if

the representation ad

0

is completely reducible. A simple

Z

2

-graded

Lie

algebra

is

classical

i its even part

L

0

is a reductive

Lie

algebra.

Denote by Mat(

m n

) the

Z

2

-graded associative algebra with unit con-

sisting of (

m

+

n

)

(

m

+

n

) block matrices with entries from

K

A

0

B

1

B

0

A

1

:

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Boseck

113

We observe Mat(

m n

) = Mat

;1

(

m n

)

Mat

0

(

m n

)

Mat

1

(

m n

) (compare (1)

and (2)).

The

Z

2

-graded

Lie

algebra dened by Mat(

m n

) is denoted by

gl

(

m n

)

or

pl

(

m n

). It is called the

general linear

Lie

superalgebra

.

gl

(

m n

) admits a

Z

-gradation

gl

(

m n

) =

gl

;1

(

m n

)

gl

0

(

m n

)

gl

1

(

m n

)

implying the

Z

2

-gradation in the natural way. We have

gl

0

(

m n

) =

gl

0

(

m n

)

=

gl

(

m

)

gl

(

n

)

gl

1

(

m n

) =

gl

;1

(

m n

)

gl

1

(

m n

)

:

We shall discuss several subalgebras of

gl

(

m n

).

Example 1

.

sl

(

m n

) or

spl

(

m n

) denotes the subalgebra consisting of those

block matrices for which the diagonal blocks have equal trace, i.e., satisfying

the equation Tr(

A

0

) = Tr(

A

1

). It is called the

special linear

Lie

superalgebra.

sl

(

m n

) admits the

Z

-gradation induced by

gl

(

m n

) and the corresponding

Z

2

-

grading. We have

sl

0

(

m n

)

=

sl

(

m

)

sl

(

n

)

K

.

Example 2

.

osp

(

m n

) consists of those block matrices satisfying the follow-

ing relations

A

0

>

+

A

0

= 0

B

1

>

;

I

n

B

0

= 0

A

1

>

I

n

+

I

n

A

1

= 0

:

Here

A

>

denotes the transpose of

A

, and

n

is assumed to be even

n

= 2

`

, and

I

n

=

0

E

`

;

E

`

0

where

E

`

denotes the

`

`

unit matrix. The matrices of

osp

(

m

2

`

) may be

written in the following form

0

@

A

0

B

1

B

2

;

B

2

>

A

1

A

12

B

1

>

A

21

;

A

1

>

1

A

with

A

0

>

=

;

A

0

A

>

12

=

A

12

and

A

>

21

=

A

21

:

Note that

osp

(

m n

) is a

Z

2

-graded

Lie

algebra. It is called the

orthogonal-

symplectic

Lie

superalgebra. For the even part one has

osp

0

(

m n

)

=

o

(

m

)

sp

(

n

)

:

Example 3

.

e

gl

(

m

) consists of those block matrices satisfying

m

=

n

and

A

1

=

A

0

and

B

1

=

B

0

:

It is called the

general linear

Lie

superalgebra of the

second kind

.

e

gl

(

m

) is a

Z

2

-graded

Lie

algebra and we have

e

gl

0

(

m

)

=

gl

(

m

).

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114

Boseck

Example 4

.

e

sl

(

m

) consists of those block matrices satisfying

m

=

n

and

A

1

=

A

0

,

B

1

=

B

0

, and Tr(

B

1

) = 0. It is called the

special linear

Lie

superalgebra of the second kind

.

e

sl

(

m

) is a

Z

2

-graded

Lie

algebra, a subalgebra

of

e

gl

(

m

), and the following relation holds:

e

sl

0

(

m

) =

e

gl

0

(

m

)

=

gl

(

m

).

The

Lie

superalgebra

sl

(

m n

)

is simple if

m

6

=

n

,

m

1

,

n

1

.

The multiples of the unit matrix

f

E

2

m

2

K

g

make up a

Z

2

-graded

ideal of

sl

(

m m

), namely, the center.

The quotient algebra

sl

(

m m

)

=

f

E

2

m

:

2

K

g

is simple if

m >

1.

The

A

-series of simple

Lie

superalgebras is dened in analogy with the

usual classication of simple

Lie

algebras by

A

(

m n

) =

sl

(

m

+ 1

n

+ 1)

m

6

=

n m

0

n

0

:

A

(

m m

) =

sl

(

m

+ 1

m

+ 1)

=

f

E

2

m

+2

:

2

K

g

m >

0

:

The orthogonal-symplectic

Lie

superalgebra

osp

(

m n

)

is simple if

m

1

,

n >

1

.

The series

B C D

are dened as follows

B

(

m n

) =

osp

(2

m

+ 1 2

n

)

m

0

n >

0

:

C

(

n

) =

osp

(2 2

n

;

2)

n

2

:

D

(

m n

) =

osp

(2

m

2

n

)

m

2

n >

0

:

As in

sl

(

m m

), the multiples of unity

f

E

2

m

2

K

g

make up a

homogeneous ideal in

e

sl

(

m

), namely, its center.

The quotient algebra

e

sl

(

m

)

=

f

E

2

m

:

2

K

g

is simple if

m

3

.

The

Q

-series is dened by

Q

(

m

) =

e

sl

(

m

+ 1)

=

f

E

2

m

+2

:

2

K

g

m

2

:

The

Lie

superalgebras

Q

(

m

) are often called

the

f

;

d

-algebras of

Michal

and

Radicati

.

The

Lie

superalgebras of the series

A B C D

and

Q

are classical

Lie

superalgebras.

The decomposition of the even parts in a direct product of simple

Lie

algebras is given by the following isomorphisms

A

0

(

m n

)

=

A

(

m

)

A

(

n

)

K m

6

=

n

A

0

(

m m

)

=

A

(

m

)

A

(

m

)

B

0

(

m n

)

=

B

(

m

)

C

(

n

)

C

0

(

m

)

=

C

(

m

;

1)

K

D

0

(

m n

)

=

D

(

m

)

C

(

n

)

Q

0

(

m

)

=

A

(

m

)

:

background image

Boseck

115

3. The G

RASSMANN

-hull

The

Grassmann

-hull is a construction, which enables us to make a

Z

2

-

graded

Lie

algebra into a

Lie

algebra. Let denote a nitely generated

Grass-

mann

algebra and let

L

be a

Z

2

-graded

Lie

algebra. Taking the tensorproduct

L

of

Z

2

-graded algebras we have

(

L

)

0

=

0

L

0

+

1

L

1

(

L

)

1

=

0

L

1

+

1

L

0

:

Writing the elements of

L

for simplicity as

x

, the brackets are de-

ned for homogeneous elements as follows:

x

x

] = (

;

1)

x

x

],

2

Z

2

. If

=

and

=

, then we have

x

x

] = (

;

1)

x

x

]

= (

;

1)

+

+

(

;

1)

x

x

]

=

;

(

;

1)

+

+

+

x

x

]

Since

+

=

+

= 0 we have

x

x

] =

;

x

x

]. The even

part (

L

)

0

of the tensor product

L

is a

Lie

algebra. It is called the

Grassmann

-

hull

of the

Lie

superalgebra

L

.

Let

L

denote one of the

Lie

superalgebras

gl

(

m n

),

sl

(

m n

),

osp

(

m n

),

e

gl

(

m

), or

e

sl

(

m

). The

Grassmann

-hull consists of block matrices

(5)

A

0

(

0

)

B

1

(

1

)

B

0

(

1

)

A

1

(

0

)

:

The entries of the diagonal blocks

A

0

and

A

1

belong to

0

, while the entries

of the matrices

B

0

and

B

1

are from

1

. We denote the

Grassmann

-hulls

by

gl

(

m n

),

sl

(

m n

),

osp

(

m n

),

e

gl

(

m

),

e

sl

(

m

), respectively. Note

that

sl

(

m n

) is the

Lie

algebra of block matrices of type (5) such that

Tr(

A

0

(

0

)) = Tr(

A

1

(

0

)). Further,

osp

(

m

2

l

) is the

Lie

algebra of block

matrices

0

@

A

0

(

0

)

B

1

(

1

)

B

2

(

1

)

;

B

>

2

(

1

)

A

1

(

0

)

A

12

(

0

)

B

>

1

(

0

)

A

21

(

0

)

;

A

>

1

(

0

)

1

A

satisfying the relations

A

>

0

(

0

) =

A

0

(

0

),

A

>

12

(

0

) =

A

12

(

0

),

A

>

21

(

0

) =

A

21

(

0

). Finally,

e

sl

(

m

) consists of block matrices

A

(

0

)

B

(

1

)

B

(

1

)

A

(

0

)

satisfying the relation Tr

B

(

1

) = 0.

background image

116

Boseck

In all of our considerations denotes an arbitrary nitely generated

Grassmann

algebra. Later it will become clear, that it is necessary to assume,

that the number of generators "is not to small" with respect to

m

and

n

.

Let

p

0

:

!

0

=

K

denote the canonical projection of the

Z

-graded

algebra onto its zero component. Then

p

0

denes a canonical projection of

the

Grassmann

-hull (

L

)

0

of a

Lie

superalgebra

L

onto its even part

L

0

.

We denote it once more by

p

0

, so that

p

0

(

x

) =

p

0

(

)

x

. With respect to the

matrix

Lie

algebra

gl

(

m n

) and its subalgebras we have

p

0

A

0

(

0

)

B

1

(

1

)

B

0

(

1

)

A

1

(

0

)

=

A

0

0

0

A

1

with entries from

K

in the diagonal blocks

A

0

and

A

1

.

In the case of

osp

(

m n

) the matrices

A

0

make up the

Lie

algebra

o

(

m

) while the matrices

A

1

are the matrices of

sp

(

n

).

In the same way we may dene the

Grassmann

-hull of a

Z

2

-graded

associative algebra. The

Grassmann

-hull of the matrix algebra Mat(

m n

) is

denoted by Mat(

m n

) = (

Mat(

m n

))

0

, the elements are the block matrices

(5).

4. G

RASSMANN

L

IE

groups

The series GL, SL, OSp,

f

GL,

f

SL. We dene matrix

Lie

groups

corresponding to the

Grassmann

-hulls of matrix

Lie

superalgebras. First we

answer the question of invertibility of a matrix (5) from Mat(

m n

).

A block matrix of type

(5)

is invertible i the matrices

A

0

=

p

0

(

A

0

(

0

))

and

A

1

=

p

0

(

A

1

(

0

))

are invertible.

It follows that the diagonal blocks

A

0

(

0

) and

A

1

(

0

) are invertible for

invertible block matrices. The inverse of a block matrix is written

A

(;1)

0

(

0

)

B

(;1)

1

(

1

)

B

(;1)

0

(

1

)

A

(;1)

1

(

0

)

satisfying the equations

A

(;1)

0

(

0

) = (

A

0

(

0

)

;

B

1

(

1

)

A

1

(

0

)

;1

B

0

(

1

))

;1

A

(;1)

1

(

0

) = (

A

1

(

0

)

;

B

0

(

1

)

A

0

(

0

)

;1

B

1

(

1

))

;1

B

(;1)

1

(

1

) =

;

A

0

(

0

)

;1

B

1

(

1

)(

A

1

(

0

)

;

B

0

(

1

)

A

0

(

0

)

;1

B

1

(

1

))

;1

B

(;1)

0

(

1

) =

;

A

1

(

0

)

;1

B

0

(

1

)(

A

0

(

0

)

;

B

1

(

1

)

A

1

(

0

)

;1

B

0

(

1

))

;1

:

Let GL(

m n

) denote the group of units in Mat(

m n

). It consists

of the invertible block matrices of type (5) which for simplicity are written

A

() =

A

0

()

B

1

()

B

0

()

A

1

()

:

background image

Boseck

117

The

superdeterminant

or

Berezin

ian

of

A

is dened by sdet

A

() =

det

;

A

0

()

;

B

1

()

A

1

()

;1

B

0

()

det

A

;1

1

(). The superdeterminant is dened

on the

Grassmann Lie

group GL(

m n

). It is multiplicative, i.e., sdet is a

homomorphism of GL(

m n

) into the group of units

K

of .

Also, SL(

m n

) is the subgroup of GL(

m n

) dened by

sdet

A

() = 1

or, equivalently, by

det(

A

0

()

;

B

1

()

A

1

()

;1

B

0

()) = det

A

1

()

:

Using the projection

p

0

:

!

K

we get

det

A

0

=

p

0

(det

A

0

()) =

p

0

(det

A

1

()) = det

A

1

:

We observe that GL(

m n

) and SL(

m n

) are the -matrix groups

corresponding to the -matrix

Lie

algebras

gl

(

m n

) and

sl

(

m n

), respec-

tively.

OSp(

m n

) is the subgroup of GL(

m n

) dened by the following

relations

A

0

()

>

A

0

()

;

B

0

()

>

I

n

B

0

() =

E

m

A

0

()

>

B

1

()

;

B

0

()

>

I

n

A

1

() = 0

B

1

()

>

B

1

() +

A

1

()

>

I

n

A

1

() =

I

n

:

Applying the projection

p

0

to these equations, we get

A

>

0

A

0

=

E

m

and

A

>

1

I

n

A

1

=

I

n

hence

p

0

:OSp(

m n

)

!

O(

m

)

Sp(

n

).

OSp(

m n

) is the -matrix group corresponding to the -matrix

Lie

algebra

osp

(

m n

). The projection

p

0

is a homomorphism mapping the

Grassmann Lie

group OSp(

m n

) onto the

Lie

group O(

m

)

Sp(

n

) corre-

sponding to the even part of

osp

(

m n

).

We observe that

f

GL(

m

) denotes the group of block matrices

e

A

() =

A

()

B

()

B

()

A

()

with

A

() =

A

(

0

) and

B

() =

B

(

1

).

f

SL(

m

) is the subgroup of

f

GL(

m

) consisting of those block matrices

e

A

() satisfying

g

sdet

e

A

= 1. Here the

superdeterminant of the second kind

g

sdet

is dened on the

Grassmann Lie

group

f

GL(

m

) by

(6)

g

sdet

e

A

() = 1 + Trlog(

E

m

+

A

()

;1

B

())

:

background image

118

Boseck

The relation (6) may be rewritten by

Trlog(

E

m

+

A

()

;1

B

()) =

X

1

2

+ 1 Tr(

A

()

;1

B

())

2

+1

= 0

:

Notice that the entries of the product matrix

A

()

;1

B

() belong to

1

which

implies that the series of the logarithm is nite.

The superdeterminant of the second kind is multiplicative. Thus

g

sdet is

a homomorphism of

f

GL(

m

) into the group

K

of units in . The projection

p

0

maps the

Grassmann Lie

group

f

SL(

m

) onto the

Lie

group GL(

m

) which

corresponds to the even part of

e

sl

(

m

).

f

GL(

m

) and

f

SL(

m

) are the -matrix groups corresponding to the

-matrix

Lie

algebras

e

gl

(

m

) and

e

sl

(

m

), respectively.

The center of the -matrix group

f

SL(

m

) consists of the even multiples

of the unit matrix, and the quotient

f

SL(

m

+ 1)

=

f

0

E

2

m

+2

:

0

2

0

g

is a

Grassmann Lie

group, which corresponds to the

Grassmann

-hull of the

Lie

superalgebra

Q

(

m

).

5. H

OPF

Superalgebras

Let

H

=

H

0

H

1

denote a

Z

2

-graded

Hopf

algebra. Here

H

is a

Z

2

-

graded associative algebra with unit|the product and the unit are considered

as linear mappings

:

H

H

!

H

and

:

K

!

H

, respectively|endowed

with a coproduct :

H

!

H

H

, a counit

"

:

H

!

K

, and an antipode

:

H

!

H

. Here and

"

are homomorphisms of the corresponding

Z

2

-graded

algebras,

is an antiautomorphism of

H

. The following relations are satised

(

id

H

)

= (id

H

)

, called the

coassociativity

of the coproduct,

(

"

id

H

)

= id

H

= (id

H

"

)

, and

(

id

H

)

=

"

=

(id

H

)

.

Let

:

H

H

!

H

H

denote the

twist

homomorphism given by

(

h

1

h

2

) =

(

;

1)

j

h

1

jj

h

2

j

h

2

h

1

for homogeneous elements

h

1

and

h

2

in

H

. Then

H

is called

commutative

or

cocommutative

if the relations

=

or

=

hold, respectively.

Example 1 .

Put

H

=

K

X

1

::: X

m

]

(

Y

1

::: Y

n

). Then we have

H

0

=

K

X

1

::: X

m

]

0

(

Y

1

::: Y

n

)

H

1

=

K

X

1

::: X

m

]

1

(

Y

1

::: Y

n

)

:

Now

H

is a

Hopf

algebra with respect to the usual product, the usual

unit , the coproduct (

X

) = 1

X

+

X

1, (

Y

) = 1

Y

+

Y

1,

(1) = 1

1, the counit

"

(

X

) =

"

(

Y

) = 0,

"

(1) = 1, and the antipode

(

X

) =

;

X

,

(

Y

) =

;

Y

,

(1) = 1, for

= 1

::: m

,

= 1

::: n

. The

Hopf

superalgebra

H

is commutative and cocommutative.

background image

Boseck

119

Example 2 .

Let

G

= GL(

m n

) denote the -matrix group dened in

Section 4. We dene a block matrix of

commuting

and

anticommuting variables

by

X

=

X Y

0

Y X

0

:

We assume

X

= (

X

ij

)

i

=1

:::m

j

=1

:::m

Y

0

= (

Y

0

i`

)

i

=1

::: m

`

=1

::: n

Y

= (

Y

kj

)

k

=1

::: n

j

=1

:::m

X

0

= (

X

0

k`

)

k

=1

::: n

`

=1

::: n

:

Put

H

(

G

) =

K

X

ij

x X

0

k`

x

0

]

(

Y

0

i`

Y

kj

)

=

(

x

det

j

X

ij

j

;

1

x

0

det

j

X

0

k`

j

;

1)

then

H

(

G

) is an associative and commutative

Z

2

-graded algebra with unit.

Using the matrix product we dene the coproduct as follows:

(

X

ij

) =

m

X

j

0

=1

X

ij

0

X

j

0

j

+

n

X

`

0

=1

Y

0

i`

0

Y

`

0

`

(

X

0

k`

) =

m

X

j

0

=1

Y

kj

0

Y

0

j

0

`

+

n

X

`

0

=1

X

0

k`

0

X

0

`

0

l

(

Y

0

i`

) =

m

X

j

0

=1

X

ij

0

Y

0

j

0

`

+

n

X

`

0

=1

Y

0

i`

0

X

0

`

0

`

(

Y

kj

) =

m

X

j

0

=1

Y

kj

0

X

j

0

j

+

n

X

`

0

=1

X

0

k`

0

Y

`

0

j

(

x

) =

x

x

(

x

0

) =

x

0

x

0

:

For short we may write (

X

) =

X

X

. The counit is given by

"

(

X

ij

) =

ij

"

(

X

0

k`

) =

kl

"

(

Y

0

i`

) = 0

:

"

(

Y

kj

) = 0

"

(

x

) = 1

"

(

x

0

) = 1

:

For short we may write

"

(

X

) =

E

m

+

n

. The coproduct in

H

(

G

) mirrors the

matrix product, i.e., the product in the group

G

, the counit represents the

evaluation at the unit matrix, i.e., the evaluation at the identity of the group

G

. Now we dene the antipode, which mirrors the inverse of matrices or group

elements

(

X

) = (

X

;

Y

0

X

0;1

Y

)

;1

(

X

0

) = (

X

0

;

Y X

;1

Y

0

)

;1

(

Y

0

) =

;

X

;1

Y

0

(

X

(

Y

) =

;

X

0;1

Y

(

X

0

)

(

x

) = det

X

(

x

0

) = det

X

0

:

background image

120

Boseck

For short we may write

(

X

) =

X

;1

. Now

H

(

G

) is a commutative and not

cocommutative

Hopf

superalgebra, which we shall denote by

P

(

m n

)

:

Example 3 .

Assume

G

= SL(

m n

). Put

H

(

G

) =

P

(

m n

)

=

(sdet

X

;

1)

=

P

(

m n

)

=

(det(

X

;

Y

0

X

0;1

Y

)

;

det

X

0

)

:

It follows from sdet(

X

1

X

2

) = sdet

X

1

sdet

X

2

that the homogeneous ideal gener-

ated by sdet

X

;

1 is a coideal, too. We have

(sdet

X

;

1) = sdet

X

;

1

1

= sdet(

X

X

)

;

1

1

= sdet

X

sdet

X

;

1

1

= sdet

X

sdet

X

;

sdet

X

1 + sdet

X

1

;

1

1

= sdet

X

(sdet

X

;

1) + (sdet

X

;

1)

1

:

Moreover,

"

(sdet

X

) = 1 and

(sdet

X

) = sdet

X

;1

, i.e., the ideal generated

by sdet

X

;

1 is contained in the kernel of

"

and invariant under

. Hence it

is possible to factorize ,

"

,

, and

H

(

G

) becomes a commutative and not

cocommutative

Hopf

superalgebra, which is denoted by

S

P

(

m n

).

A -matrix group, i.e, a subgroup of GL(

m n

) is called

algebraic

, if

it is the annihilator set of a

Z

2

;

graded

ideal of

P

(

m n

).

Let

G

denote an algebraic

-matrix group, and let

I

(

G

)

denote its an-

nihilator ideal in

P

(

m n

)

, then

H

(

G

) =

P

(

m n

)

=I

(

G

)

is a

Hopf

superalgebra.

The coproduct, the counit, and the antipode of

H

(

G

)

are induced by factoriza-

tion of the coproduct, the counit, and the antipode of

P

(

m n

)

. The annihilator

ideal

I

(

G

)

is a coideal of

P

(

m n

)

, it is contained in the kernel of

"

, and it is

invariant under

.

Example 4 .

The -matrix group OSp(

m n

) is an algebraic -matrix

group. Its annihilator ideal is generated by the \polynomials"

X

>

X

;

Y

>

I

n

Y

;

E

m

,

X

>

Y

0

;

Y I

n

X

0

, and

Y

0>

Y

0

+

X

0>

I

n

X

0

;

I

n

. The corresponding

Hopf

superalgebra is denoted by

O S

p

P

(

m n

).

Example 5 .

The -matrix group

f

GL(

m

) is an algebraic -matrix group.

Its

Hopf

superalgebra is denoted by

e

P

(

m

):

e

P

(

m

)

=

K

X

ij

x

]

(

Y

ij

)

=

(

x

det

j

X

ij

j

;

1)

:

Example 6 .

The -matrix group

f

SL(

m

) is an algebraic -matrix group.

Its

Hopf

superalgebra is denoted by

g

S

P

(

m

)

:

A

Hopf

superalgebra

H

=

H

0

H

1

is called

ane

if it is commutative

and nitely generated.

background image

Boseck

121

The

Hopf

superalgebra

H

(

G

) =

P

(

m n

)

=I

(

G

)

of an algebraic

-matrix

group

G

is ane.

The

Hopf

superalgebras

P

(

m n

)

,

S

P

(

m n

)

,

O S

p

P

(

m n

)

,

e

P

(

m

)

, and

g

S

P

(

m

)

are ane

Hopf

superalgebras.

We mention the following

Structure Theorem.

Let

H

denote an ane

Hopf

superalgebra. Then

there exists an ane

Hopf

algebra

H

0

and odd elements

W

1

::: W

s

such that

H

=

H

0

(

W

1

::: W

s

)

. The isomorphism is an isomorphism of commutative

superalgebras. The following relations hold:

(

p

p

)

=

0

p

"

=

"

0

p

p

=

0

p:

Here

p

denotes the canonical projection annihilating all odd elements of

H

, i.e.,

p

:

H

!

H

0

, and

0

"

0

,

0

denote the coproduct, the counit, and the antipode

of the

Hopf

algebra

H

0

, respectively.

The ane

Hopf

algebra

H

0

is the algebra of polynomial functions of an

(ane) algebraic group

G

0

.

Example 2 (continued).

Assume

G

= GL(

m n

),

H

=

H

(

G

) =

P

(

m n

).

Then one has

H

0

=

K

X

ij

x X

0

k`

x

0

]

=

(

x

det

j

X

ij

j

;

1

x

0

det

j

X

0

kl

j

;

1)

and

G

0

= GL(

m

)

GL(

n

) =

p

0

(GL(

m n

))

:

Example 3 (continued).

Assume

G

= SL(

m n

)

H

=

H

(

G

) =

S

P

(

m n

).

Then one has

H

0

=

K

X

ij

x X

0

k`

x

0

]

=

(

x

det

j

X

ij

j

;

1

x

0

det

j

X

0

k`

j

;

1 det

j

X

ij

j

;

det

j

X

0

k`

j

)

and

G

0

= SL(

m

)

SL(

n

)

K

=

p

0

(SL(

m n

)

:

Example 4 (continued).

Assume

G

= OSp(

m n

),

H

=

H

(

G

) =

O S

p

P

(

m n

)

:

Then one has

H

0

=

K

X

ij

X

0

k`

]

=I

0

and the ideal

I

0

is generated by

m

X

i

0

=1

X

i

0

i

X

i

0

j

;

ij

n

0

;1

X

k

0

=0

(

X

0

n

;

k

0

k

X

0

k

0

+1

`

;

X

0

n

0

;

k

0

k

X

0

n

0

+

k

0

+1

`

;

k`

) (

n

= 2

n

0

)

:

This implies

G

0

= O(

m

)

Sp(

n

) =

p

0

(OSp(

m n

)).

background image

122

Boseck

Example 5 (continued).

Assume

G

=

f

GL(

m

),

H

=

H

(

G

) =

e

P

(

m

).

Then one has

H

0

=

K

X

ij

x

]

=

(

x

det

j

X

ij

j

;

1)

and

G

0

= GL(

m

) =

p

0

(

f

GL(

m

))

:

Example 6 (continued).

Assume

G

=

f

SL(

m

),

H

=

H

(

G

) =

g

S

P

(

m

).

Then one has

H

0

=

K

X

ij

x

]

=

(

x

det

j

X

ij

j

;

1)

and

G

0

= GL(

m

) =

p

0

(

f

SL(

m

))

:

Notice that the isomorphism of superalgebras stated in the structure

theorem is not a canonical one. In some sense it is the choice of a coordinate

system.

Example

6

(continued once more).

We have

g

S

P

(

m

)

=

K

X

ij

x

]

(

Y

ij

)

=I

(

f

SL(

m

))

:

The annihilator ideal

I

(

f

SL(

m

)) is generated by

x

det

j

X

ij

j ;

1 and Trlog(

E

m

+

X

;1

Y

) =

P

1

2

+1

Tr(

X

;1

Y

)

2

+1

. Choosing instead of the

Y

ij

new odd vari-

ables

W

ij

dened by the matrix equation

W

=

X

;1

Y

, then using the second

relation it is possible to eliminate one of the odd variables. In this case we have

s

=

m

2

;

1.

The last two sections, namely, Section 6, \Ane algebraic Supergroups"

and Section 7, \The

Hopf

dual. Representations", as well as the list of references

are postponed to the next seminar.

References

References to the literature will be given in the sequel to this article:

1]

Boseck, H.,

Lie superalgebras and Lie supergroups, II

, Seminar Sophus

Lie (Heldermann Verlag Berlin)

2

(1992), to appear.

Fachrichtungen Mathematik/Informatik

Ernst-Moritz-Arndt-UniversitatGreifswald

Friedrich Ludwig Jahn-Strae 15a

O-2200 Greifswald, Germany

Received July 31, 1991


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