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The International Journal Of Engineering And Science (IJES) || Volume || 4 || Issue || 6 || Pages || PP.63-77|| June - 2015 || ISSN (e): 2319 1813 ISSN (p): 2319 1805 www.theijes.com The IJES Page 63 Combinatorial Identities Related To Root Supermultiplicities In Some Borcherds Superalgebras N.Sthanumoorthy * and K.Priyadharsini The Ramanujan Institute for Advanced study in Mathematics University of Madras, Chennai - 600 005, India. ------------------------------------------------------------- ABSTRACT--------------------------------------------------------- In this paper, root supermultiplicities and corresponding combinatorial identities for the Borcherds superalgebras which are extensions of 2 B and 3 B are found out. Keywords: Borcherds superalgebras, Colored superalgebras, Root supermultiplicities. ---------------------------------------------------------------------------------------------------------------------------------------- Date of Submission: 10-June-2015 Date of Accepted: 25-June-2015 ---------------------------------------------------------------------------------------------------------------------------------------- I. INTRODUCTION The theory of Lie superalgebras was constructed by Kac in 1977. The theory of Lie superalgebras can also be seen in Scheunert(1979) in a detailed manner. The notion of Kac-Moody superalgebras was introduced by Kac(1978) and therein the Weyl-Kac character formula for the irreducible highest weight modules with dominant integral highest weight which yields a denominator identity when applied to 1-dimensional representation was also derived. Borcherds(1988, 1992) proved a character formula called Weyl-Borcherds formula which yields a denominator identity for a generalized Kac-Moody algebra.Kang developed homological theory for the graded Lie algebras in 1993a and derived a closed form root multiplicity formula for all symmetrizable generalized Kac-Moody algebras in 1994a. Miyamoto(1996) introduced the theory of generalized Lie superalgebra version of the generalized Kac-Moody algebras(Borcherds algebras). Kim and Shin(1999) derived a recursive dimension formula for all graded Lie algebras. Kang and Kim(1999) computed the dimension formula for graded Lie algebras. Computation of root multiplicities of many Kac-Moody algebras and generalized Kac-Moody algebras can be seen in Frenkel and Kac(1980), Feingold and Frenkel(1983),Kass et al.(1990), Kang(1993b, 1994b,c,1996), Kac and Wakimoto(1994), Sthanumoorthy and Uma Maheswari(1996b), Hontz and Misra(2002), Sthanumoorthy et al.(2004a,b) and Sthanumoorthy and Lilly(2007b). Computation of root multiplicities of Borcherds superalgebras was found in Sthanumoorthy et al.(2009a). Some properties of different classes of root systems and their classifications for Kac-Moody algebras and Borcherds Kac-Moody algebras were studied in Sthanumoorthy and Uma Maheswari(1996a) and Sthanumoothy and Lilly(2000, 2002,2003,2004, 2007a). Also, properties of different root systems and complete classifications of special, strictly, purely imaginary roots of Borcherds Kac-Moody Lie superalgebras which are extensions of Kac-Moody Lie algebras were explained in Sthanumoorthy et al.(2007,2009b) and Sthanumoorthy and Priyadharsini(2012, 2013). Moreover, Kang(1998) obtained a superdimension formula for the homogeneous subspaces of the graded Lie superalgebras, which enabled one to study the structure of the graded Lie superalgebras in a unified way. Using the Weyl-Kac-Borcherds formula and the denominator identity for the Borcherds superalgerbas, Kang and Kim(1997) derived a dimension formula and combinatorial identities for the Borcherds superalgebras and found out the root multiplicities for Monstrous Lie superalgebras. Borcherds superalgebras which are extensions of Kac Moody algebras 2 A and 3 A were considered in Sthanumoorthy et al.(2009a) and therein dimension formulas were found out.In Sthanumoorthy and Priyadharsini(2014), we have computed combinatorial identities for 2 A and 3 A and root super multiplicities for some hyperbolic Borcherds superalgebras. The aim of this paper is to compute dimensional formulae, root supermultiplicities and corresponding combinatorial identities for the Borcherds superalgebras which are extensions of Kac-Moody algebras 2 B and 3 B .

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Page 1: Combinatorial Identities Related To Root Supermultiplicities In Some Borcherds Superalgebras

The International Journal Of Engineering And Science (IJES)

|| Volume || 4 || Issue || 6 || Pages || PP.63-77|| June - 2015 ||

ISSN (e): 2319 – 1813 ISSN (p): 2319 – 1805

www.theijes.com The IJES Page 63

Combinatorial Identities Related To Root Supermultiplicities In

Some Borcherds Superalgebras

N.Sthanumoorthy * and K.Priyadharsini The Ramanujan Institute for Advanced study in Mathematics

University of Madras, Chennai - 600 005, India.

-------------------------------------------------------------ABSTRACT---------------------------------------------------------

In this paper, root supermultiplicities and corresponding combinatorial identities for the Borcherds

superalgebras which are extensions of 2

B and 3

B are found out.

Keywords: Borcherds superalgebras, Colored superalgebras, Root supermultiplicities.

----------------------------------------------------------------------------------------------------------------------------------------

Date of Submission: 10-June-2015 Date of Accepted: 25-June-2015

----------------------------------------------------------------------------------------------------------------------------------------

I. INTRODUCTION The theory of Lie superalgebras was constructed by Kac in 1977. The theory of Lie superalgebras can

also be seen in Scheunert(1979) in a detailed manner. The notion of Kac-Moody superalgebras was introduced

by Kac(1978) and therein the Weyl-Kac character formula for the irreducible highest weight modules with

dominant integral highest weight which yields a denominator identity when applied to 1-dimensional

representation was also derived. Borcherds(1988, 1992) proved a character formula called Weyl-Borcherds

formula which yields a denominator identity for a generalized Kac-Moody algebra.Kang developed homological

theory for the graded Lie algebras in 1993a and derived a closed form root multiplicity formula for all

symmetrizable generalized Kac-Moody algebras in 1994a. Miyamoto(1996) introduced the theory of

generalized Lie superalgebra version of the generalized Kac-Moody algebras(Borcherds algebras). Kim and

Shin(1999) derived a recursive dimension formula for all graded Lie algebras. Kang and Kim(1999) computed

the dimension formula for graded Lie algebras. Computation of root multiplicities of many Kac-Moody algebras

and generalized Kac-Moody algebras can be seen in Frenkel and Kac(1980), Feingold and Frenkel(1983),Kass

et al.(1990), Kang(1993b, 1994b,c,1996), Kac and Wakimoto(1994), Sthanumoorthy and Uma

Maheswari(1996b), Hontz and Misra(2002), Sthanumoorthy et al.(2004a,b) and Sthanumoorthy and

Lilly(2007b). Computation of root multiplicities of Borcherds superalgebras was found in Sthanumoorthy et

al.(2009a). Some properties of different classes of root systems and their classifications for Kac-Moody algebras

and Borcherds Kac-Moody algebras were studied in Sthanumoorthy and Uma Maheswari(1996a) and

Sthanumoothy and Lilly(2000, 2002,2003,2004, 2007a). Also, properties of different root systems and complete

classifications of special, strictly, purely imaginary roots of Borcherds Kac-Moody Lie superalgebras which are

extensions of Kac-Moody Lie algebras were explained in Sthanumoorthy et al.(2007,2009b) and Sthanumoorthy

and Priyadharsini(2012, 2013). Moreover, Kang(1998) obtained a superdimension formula for the homogeneous

subspaces of the graded Lie superalgebras, which enabled one to study the structure of the graded Lie

superalgebras in a unified way. Using the Weyl-Kac-Borcherds formula and the denominator identity for the

Borcherds superalgerbas, Kang and Kim(1997) derived a dimension formula and combinatorial identities for the

Borcherds superalgebras and found out the root multiplicities for Monstrous Lie superalgebras. Borcherds

superalgebras which are extensions of Kac Moody algebras 2

A and 3

A were considered in Sthanumoorthy et

al.(2009a) and therein dimension formulas were found out.In Sthanumoorthy and Priyadharsini(2014), we have

computed combinatorial identities for 2

A and 3

A and root super multiplicities for some hyperbolic Borcherds

superalgebras.

The aim of this paper is to compute dimensional formulae, root supermultiplicities and

corresponding combinatorial identities for the Borcherds superalgebras which are extensions of Kac-Moody

algebras 2

B and 3

B .

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II. PRELIMINARIES In this section, we give some basic concepts of Borcherds superalgebras as in Kang and Kim (1997).

Definition 2.1: Let I be a countable (possibly infinite) index set. A real square matrix Ijiij

aA,

)(= is called

Borcherds-Cartan matrix if it satisfies:

(1) 2=ii

a or 0ii

a for all Ii ,

(2) 0ij

a if ji and Zij

a if 2=ii

a ,

(3) 0=0=jiij

aa

We say that an index i is real if 2=ii

a and imaginary if 0ii

a . We denote by

0}.|{=2},=|{=ir

ii

m

ii

eaIiIaIiI

Let }|{=0>

Iimmi

Z be a collection of positive integer such that 1=i

m for all e

Iir

. We call m a

charge of A .

Definition 2.2: A Borcherds-Cartan matrix A is said to be symmetrizable if there exists a diagonal matrix

);(d= IiiagDi

with )(0> Iii

such that DA is symmetric.

Let Ijiij

cC,

)(= be a complex matrix satisfying 1=jiij

cc for all Iji , . Therefore, we have 1= ii

c

for all Ii . We call Ii an even index if 1=ii

c and an odd index if 1= ii

c .

We denote by ven

Ie

( )o dd

I the set of all even (odd) indices.

Definition 2.3: A Borcherds-cartan matrix Ijiij

aA,

)(= is restricted (or colored) with respect to C if it

satisfies:

If 2=ii

a and 1= ii

c then ij

a are even integers for all Ij . In this case, the matrix C is called a

coloring matrix of A .

Let )()(=iIiiIi

dh CCh

be a complex vector space with a basis };,{ Iidhii

, and for each

Ii , define a linear functional *hi

by

)1.2......(...........=)(,=)( Ijallfordahijjijiji

If A is symmetrizable, then there exists a symmetric bilinear form (|) on *h satisfying

jijijijiaa ==)|( for all Iji , .

Definition 2.4: Let iIi

Q Z

= and iIi

Q 0

= Z ,

QQ = . Q is called the root lattice.

The root lattice Q becomes a (partially) ordered set by putting if and only if

Q .

The coloring matrix Ijiij

cC,

)(= defines a bimultiplicative form X

CQQ : by

,,f=),( Ijalliorcijji

),,(),(=),(

),(),(=),(

for all Q ,, . Note that satisfies

)2.2....(..........,,f1=),(),( Qorall

since 1=jiij

cc for all Iji , . In particular 1=),( for all Q .

We say Q is even if 1=),( and odd if 1=),( .

Definition 2.5: A -colored Lie super algebra is a Q -graded vector space

LLQ

= together with a

bilinear product LLL :][, satisfying

,,

LLL

],,)[,(=, xyyx

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]],[,)[,(]],,[[=,, zxyzyxzyx

for all Q , and LzLyLx ,,

.

In a -colored Lie super algebra

LLQ

= , for

Lx , we have 0=],[ xx if is even and

0=]],[,[ xxx if is odd.

Definition 2.6: The universal enveloping algebra )( LU of a -colored Lie super algebra L is defined to be

JLT )/( , where )( LT is the tensor algebra of L and J is the ideal of )( LT generated by the elements

xyyxyx ),(],[ ),(

LyLx .

Definition 2.7: The Borcherds superalgebra ),,(= CmAgg associated with the symmetrizable Borcherds-

Cartan matrix A of charge );(= Iimmi

and the coloring matrix Ijiij

cC,

)(= is the -colored Lie

super algebra generated by the elements ),1,2,=,(,),(,iikikii

mkIifeIidh with defining

relations:

0=0=,=,

,2=0=)(=)(

=,

,=,,=,

,=,,=,

0,=,=,=,

11

ijjlikjlik

iijl

ija

ikjl

ija

ik

iklijjlik

jlijjlijlijjli

jlijjlijlijjli

jijiji

aifffee

jiandaiffadfeade

hfe

ffdeed

fafheaeh

dddhhh

for ji

mlmkIji ,1,=,,1,=,, .

The abelian subalgebra )()(=iIiiIi

dh CCh

is called the Cartan subalgebra of g and the linear

functionals )( Iii

*h defined by (2.1) are called the simple roots of g . For each e

Iir

, let

)(h*GLri be the simple reflection of *h defined by

).()(=)( h* iii

hr

The subgroup W of )(h*GL generated by the i

r ’s )(re

Ii is called the Weyl group of the Borcherds super

algebra g .

The Borcherds superalgebra ),,(= CmAgg has the root space decomposition

ggQ

= , where

}.)(=],[|{= hgg hallforxhxhx

Note that i

miii

ee,,1

= CCg

and i

miii

ff,,1

= CCg

We say that X

Q is a root of g if 0

g . The subspace

g is called the root space of g attached to

. A root is called real if 0>)|( and imaginary if 0)|( .

In particular, a simple root i

is real if 2=ii

a that is if e

Iir

and imaginary if 0ii

a that is if m

Iii

.

Note that the imaginary simple roots may have multiplicity 1> . A root 0> ( 0< ) is called positive

(negative). One can show that all the roots are either positive or negative. We denote by

, and

the set

of all roots, positive roots and negative roots, respectively. Also we denote 0

(1

) the set of all even (odd)

roots of g . Define the subspaces

gg

= .

Then we have the triangular decomposition of g : .=

ghgg

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Definition 2.8:(Sthanumoorthy et al.(2009b)) We define an indefinite nonhyperbolic Borcherds - Cartan

matrix A, to be of extended-hyperbolic type, if every principal submatrix of A is of finite, affine, or hyperbolic

type Borcherds - Cartan matrix. We say that the Borcherds superalgebra associated with a Borcherds - Cartan

matrix A is of extended-hyperbolic type, if A is of extended-hyperbolic type.

Definition 2.9: A g -module V is called h -diagonalizable, if it admits a weight space decomposition

,=

VV h

where .)(=|= h hallvforhvhVvV

If 0,

V then is called a weight of V , and

Vdim is called the multiplicity of in V .

Definition 2.10: A h -diagonalizable g -module V is called a highest weight module with highest weight

,

h if there is a nonzero vector Vv

such that

1. 0,=

veik for all Ii ,

imk ,1,= ,

2.

vhvh )(= for all hh and

3.

vUV )(= g .

The vector

v is called a highest weight vector.

For a highest weight module V with highest weight , we have

(i)

vUV

)(= g ,

(ii)

vVVV C=,=

and

(iii) <dim

V for all .

Definition 2.11: Let )(VP denote the set of all weights of V . When all the weights spaces are finite

dimensional, the character of V is defined to be ,)dim(=c

eVhV

*h

where

e are the basis elements of the group ][h*C with the multiplication given by

eee = for

*h , . Let

gh=b be the Borel subalgebra of g and

C be the 1-dimensional

b -module

defined by )1(=10,=1 hh

g for all .hh The induced module

Cg)(

)(=)(

bU

UM is

called the Verma module over g with highest weight . Every highest weight g -module with highest weight

is a homomorphic image of )(M and the Verma module )(M contains a unique maximal submodule

)(J . Hence the quotient )()/(=)( JMV is irreducible.

Let

P be the set of all linear functionals *h satisfying

m

i

dde

i

e

i

Iiallorh

IIiallorh

Iiallorh

i

or

0

r

0

f0)(

f2)(

f)(

Z

Z

The elements of

P are called the dominant integral weights.

Let *h be the C -linear functional satisfying iii

ah2

1=)( for all Ii . Let T denote the set of all

imaginary simple roots counted with multiplicities, and for ,TF we write ,F if 0=)(i

h for all

.Fi

Definition 2.12:[Kang and Kim (1997)] Let J be a finite subset of e

Ir

. We denote by

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JJjJjJ

=),(= Z and .\=)(

J

J Let

(2.3),=)(

0

ghg

J

J

and

.=

)(

)(

gg

J

J

Then )(

0

Jg is the restricted Kac-Moody super algebra (with an extended Cartan subalgebra) associated with the

Cartan matrix JjiijJ

aA,

)(= and the set of odd indices dddd

IJJoo

=

1}=|{= jj

cJj

Then the triangular decomposition of g is given by .=)()(

0

)( JJJ

gggg

Let JjrWjJ

|= be the subgroup of W generated by the simple reflections ),( Jjrj

and let

)(|=)( JWwJWw

where 0}.(2.4)<|{=1

w

w

Therefore J

W is the Weyl group of the restricted Kac-Moody super algebra )(

0

Jg and )( JW is the set of right

coset representatives of J

W in .W That is ).(= JWWWJ

The following lemma given in Kang and Kim (1999), proved in Liu (1992), is very useful in actual computation

of the elements of W(J).

Lemma 2.13: Suppose j

rww = and 1.)(=)( wlwl Then )( JWw if and only if )( JWw and

).()( JwJ

Let 0,1)=(=,

iJiJi

and 0,1).=(\=)(,

iJJiii

Here )(

10

denotes the set of all

positive or negative even (resp., positive or negative odd) roots of g .

The following proposition, proved in Kang and Kim (1997), gives the denominator identity for Borcherds

superalgebras.

Proposition 2.14: [Kang and Kim (1997)]. Let J be a finite subset of the set of all real indices e

Ir

. Then

)))(((c1)(=

)(1

)(1

||)(

)(

dim

)(1

dim

)(0

FswhV

e

e

J

Fwl

TF

JWw

J

J

g

g

where )( J

V denotes the irreducible highest weight module over the restricted Kac-Moody super algebra

)(

0

Jg with highest weight and where F runs over all the finite subsets of T such that any two elements of

F are mutually perpendicular. Here )( wl denotes the length of ||, Fw the number of elements in F , and

)( Fs the sum of the elements in F .

Definition 2.15: A basis elements of the group algebra ][å

hC by defining .),(=

eE

Also define the super dimension

gDim of the root space

g by

(2.5)...........................dim),(=

ggDim

Since ))(( Fsw is an element of

Q , all the weights of the irreducible highest weight )(

0

Jg -module

)))((( FswVJ

are also elements of

Q .

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Hence one can define the super dimension

DimV of the weight space

V of )))((( FswVJ

in a

similar way. More generally, for an h -diagonalizable )(

0

Jg -module

VVå

h

= such that QVP )( , we

define the super dimension

DimV of the weight space

V to be

(2.6)dim),(=

VDimV

For each 1k , let

(2.7)..........................)))(((=

|=|)(

)(

)(

FswVHJ

kFwl

TF

JWw

J

k

and define the homology space )( J

H of )( J

g to be

(2.8),=1)(=)(

3

)(

2

)(

1

)(1

1=

)(

JJJJ

k

k

k

JHHHHH

an alternating direct sum of the vector spaces.

For

Q , define the super dimension )( J

DimH

of the -weight space of )( J

H to be

)(1)(=)(1

1=

)( J

k

k

k

JDimHDimH

)))(((1)(=

|=|)(

)(

1

1=

FswDimVJ

kFwl

TF

JWw

k

k

2.9)........(..........)))(((1)(=1||)(

1||)(

)(

FswDimVJ

Fwl

Fwl

TF

JWw

Let

(2.10)...................0dim|)(=)()()(

JJHJQHP

and let ,,,,321 be an enumeration of the set )(

)( JHP . Let

)(=)(

J

i

DimHiD

.

Remark: The elements of )()( J

HP can be determined by applying the following proposition, proved in Kac

(1990).

Proposition 2.16: (Kang and Kim, 1997)

Let .

P Then }•|.{=)(

torespectwithatenondegenerisPWP .

Now for ),( JQ

one can define

(2.11).......................,=,|)(==)(01

)(

iiiii

JnnnnT

Z

which is the set of all partitions of into a sum of i

’s. For ),()(

JTn use the notations

inn |=| and

!=!i

nn .

Now, for ),( JQ

the Witt partition function )()(

JW is defined as

(2.12).......................)(!

1)!|(|=)(

)()(

)( in

JTn

JiD

n

nW

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Now a closed form formula for the super dimension

gDim of the root space ))(( J

g is given by

the following theorem. The proof is given in Kang and Kim(1997).

Theorem 2.17: Let J be a finite subset of e

Ir

. Then, for )( J

, we have

dWd

dDim

J

d

)(

|

)(1

=g

.(2.13)..........)(!

1)!|(|)(

1=

)(|

in

d

JTn

d

iDn

nd

d

where is the classical Möbius function. Namely, for a natural number ,n )( n is defined as follows:

freesquarenotisitf

primesistinctppppnor

nor

nkk

k

i0

),d:,,(=f1)(

1,=f1

=)(11

and, for a positive integer |, dd denotes d= for some

Q , in which case d

= .

In the following sections 3.1 and 3.2, we find root supermultiplicities of Borcherds superalgebras which are the

Extensions of Kac-Moody Algebras 2

B and 3

B (with multiplicity 1 ) and the corresponding combinatorial

identities using Kang and Kim(1997).

III. Root supermultiplicities of some Borcherds superalgebras which are the Extensions of Kac

Moody Algebras and the corresponding combinatorial identities

3.1 Superdimension formula and the corresponding combinatorial identity for the extended-hyperbolic

Borcherds superalgebra which is an extension of 2

B

Below, we find the dimension formulae and combinatorial identities for the Borcherds superalgebras which are

extension of .2

B (for a same set re

J ) by solving )()(

JT in two different method.

Consider the extended-hyperbolic Borcherds superalgebra ),,(= CmAgg associated with the extended-

hyperbolic Borcherds-Cartan super matrix,

22

12=

b

a

bak

A and the corresponding coloring matrix C=

1

1

1

1

3

1

2

3

1

1

21

cc

cc

cc

with .,,321

XCccc

Let {1,2,3}=I be the index set for the simple roots of .g Here 1

is the imaginary odd simple root with

multiplicity 1 and 32

, are the real even simple roots.

Let us consider the root .=332211

Qkkk We have .1)(=),(2

1k

Hence is an even

root(resp. odd root) if 1

k is even integer(resp. odd integer). Also }{=1

T and the subset TF is either

empty or }.{1

Take re

J as {3}.=J By Lemma 2.13, this implies that }.{1,=)(2

rJW From the

equations(2.7) and (2.8), the homology space can be written as

)()(=21

)(

1

JJ

JVVH

)1)((=21

)(

2 aVH

J

J

30=)(

kHJ

k

)(

2

)(

1

)(=

JJJHHHTherefore

)1)(()()(=2121

aVVVJJJ

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with 1=1;=)(

(0,1,0)

)(

(1,0,0)

JJDimHDimH

.1=1;=)(

1)(1,1,

)(

(1,1,1)

J

a

JDimHDimH

We take 1)}.(1,1,(1,1,1),(0,1,0),{(1,0,0),=)()(

aHPJ

Let ,==321 Quqp with .),,(

000 ZZZtqp Then by proposition.(2.16)

we get )}.,,(=1)(1,1,(1,1,1)(0,1,0)(1,0,0)|),,,{(=)(43214321

)(uqpassssssssT

J

This implies psss =431

qsss =432

usas =1)(43

We have 41

= asups

42

= asuqs

43

1)(= saus

])1

[,,(0=4

a

uqpmintos

Applying 4321

,,, ssss in Witt partition formula(eqn.(2.12)), we have,

...(3.1.1)..........!)!1)(()!()!(

1)(1)!(=)(

444

4

4

])1

[,,(

0=4

)(

ssauasuqqp

asqupW

asqupa

uqpmin

s

J

From eqn(2.13), the dimension of

g is

dWd

dDim

J

d

)(

|

)(1

=g

,)(!

1)!|(|)(

1=

)(|

in

d

JTn

d

iDn

nd

d

Substituting the value of )()(

JW from eqn. (3.1.1) in the above dimension formula, we have,

)2.1.3..(...........

)!/()!1)(

()!()!(

1)(1)!(

)(1

=

444

/4

///

4

])1)(

[,,(

0=4

|dss

d

a

d

us

d

a

d

u

d

q

d

q

d

p

sd

a

d

q

d

u

d

p

dd

Dim

dasdqdudp

ad

t

d

q

d

pmin

sd

g

If we solve the same ),()( J

HP using partition and substituting this partition in )()(

JT , we have

},,1)(,),{(=)(221

)( auuqpT

J

where 1

is the partition of u ` with parts 1)(1, a of length ‘u’ and 2

is the partition of 4

s with parts upto

min ])1

[,,(a

uqp . Applying )(

)(

JT in Witt partition formula(eqn.(2.12)), we have

.1.3)........(3..........!)!1)(()!()!(

1)(1)!(=)(

221

1

1

)()(

2,

1

)(

auuqp

upW

up

JT

J

From eqn.(2.13), the dimension of

g is

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dWd

dDim

J

d

)(

|

)(1

=g

,)(!

1)!|(|)(

1=

)(|

in

d

JTn

d

iDn

nd

d

Substituting the value of )()(

JW from eqn. (3.1.2) in the above dimension formula, we have

)!/())!/1)((()!()!(

1)(1)!(

)(1

=

22

1

/1

//1

)()(

2,

1)(|

ddad

u

d

u

dd

q

d

p

dd

u

d

p

dd

Dim

ddudp

JT

d

JTn

d

g

Which gives another form of dimension of

g.

Applying the value of s4 in (3.1.1), we get

!)!1)(()!()!(

1)(1)!(=)(

444

4

4

])1

[,,(

0=4

)(

ssauasuqqp

asqupW

asqupa

uqpmin

s

J

)!()!()!(

1)(1)!(

uuqqp

qupqup

])1/[,,min(.......!1))!1(()!()!(

1)(1)!(

auqpuptoauauqqp

aqupaqup

.!)!1)(()!()!(

1)(1)!(=

221

1

1

)()(

2,

1

auuqp

upup

JT

where 1

is the partition of u ` with parts )(1, a of length ‘4

asu ’ and 2

is the partition of 4

s with parts

upto min ])1

[,,(a

uqp .

Hence, we get the following theorem.

Theorem 3.1.1: For the extended-hyperbolic Borcherds superalgebra ),,(= CmAgg associated with the

extended-hyperbolic Borcherds-Cartan super matrix

22

12=

b

a

bak

A with charge {1,1,1},=m

consider the root

.=321 Quqp Then the dimension of

g is

.

)!/()!1)(

()!()!(

1)(1)!(

)(1

=

444

/4

///

4

])1)(

[,,(

0=4

|dss

d

a

d

us

d

a

d

u

d

q

d

q

d

p

sd

a

d

q

d

u

d

p

dd

Dim

dasdqdudp

ad

t

d

q

d

pmin

sd

g

Moreover the following combinatorial identity holds:

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4).....(3.1.!)!1)(()!()!(

1)(1)!(=

!)!1)(()!()!(

1)(1)!(

221

1

1

)()(

2,

1444

4

4

])1

[,,(

0=4

auuqp

up

ssauasuqqp

asqupup

JT

asqupa

uqpmin

s

where 1

is the partition of u ` with parts )(1, a of length ‘4

asu ’ and 2

is the partition of 4

s with parts

upto min ])1

[,,(a

uqp .

Example 3.1.2: For the Borcherds-Cartan super matrix ,

22

121

1

=

b

bk

A consider a root

(5,4,3)== with a=1.

Substituting 1=(5,4,3),== a in eqn(3.1.1), we have

!)!1)(()!()!(

1)(1)!(=)(

444

4

4

])1

[,,(

0=4

)(

ssauasuqqp

asqupW

asqupa

uqpmin

s

J

!)!2(3)!3(44)!(5

1)(1)!43(5=

444

4435

4

])2

3[(5,4,

0=4

sss

ssmin

s

2500.=3.4.5.6.74.5=1!2!1!1!

1)(7!

1!1!3!

1)(5!=

76

Substituting 1=(5,4,3),== a in eqn(3.1.3), we have

!)!1)(()!()!(

1)(1)!(=)(

221

1

1

)()(

2,

1

)(

auuqp

upW

up

JT

J

2500.=1!2!1!1!

1)(7!

1!1!3!

1)(5!=

76

Hence the equality (3.1.4) holds.

3.2.Dimension Formula and combinatorial identity for the Borcherds superalgebra which is an extension

of 3

B

Here we are finding the superdimension Formula and combinatorial identity for the Borcherds superalgebra

which is an extension of 3

B using the same re

J and solving )()(

JT in two different ways.

Consider the extended-hyperbolic Borcherds superalgebra ),,(= CmAgg associated with the extended-

hyperbolic Borcherds-Cartan super matrix

220

121

012=

c

b

a

cbak

A and the corresponding coloring

matrix C=

1

1

1

1

1

6

1

5

1

3

6

1

4

1

2

54

1

1

321

ccc

ccc

ccc

ccc

with .,,,4321

XCcccc

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Let {1,2,3,4}=I be the index set with charge {1,1,1,1}.=m

Let us consider the root .=44332211

Qkkkk We have .1)(=),(2

1k

Hence is

an even root(resp. odd root) if 1

k is even integer(resp. odd integer). Also }{=1

T and the subset TF is

either empty or }.{1

Take re

J as {2,3}.=J By Lemma 2.13, this implies that }.{1,=)(4

rJW

From the equations (2.7) and (2.8),the homological space can be written as

))(())(1(=41

)(

1 rVVH

JJ

J

)()(=41

JJ

VV

)1)((=)(412

cVJHJ

30=)(

kHJ

k

)1)(()()(==4141

)(

1

)( cVVVHThereforeH

JJJ

JJ!

with

1;=1;=1;=)(

(1,1,1,0)

)(

(1,1,0,0)

)(

(1,0,0,0)

JJJDimHDimHDimH

1=1;=)(

1)(1,1,1,

)(

(1,1,1,1)

J

c

JDimHDimH

Hence we have

1)}.(1,1,1,(1,1,1,1),(1,1,1,0),(1,1,0,0),,{(1,0,0,0)=)()(

cHPJ

Let ,==4321 Qvuqp with .),,,(

0000 ZZZZvuqp Then by

proposition.(2.16), we get

(1,1,1,0)(1,1,0,0)(1,0,0,0)|),,,,{(=)(32154321

)(ssssssssT

J

)}.,,,(=1)(1,1,1,(1,1,1,1)54

vuqpcss

This implies pssss =4321

qssss =5432

usss =543

.=1)(54

vscs

We have 51

= csvqps

uqs =2

53

= csvus

54

= spqs

]).1

[,,,(0=5

c

vuqpmintos

Applying 54321

,,,, sssss in Witt partition formula(eqn.2.12), we have

...(3.2.1)..........!)!()!()!()!(

1)(1)!(=)(

5555

])1

[,,,(

0=5

)(

sspqcsvuuqcsvqp

qW

qc

vuqpmin

s

J

From equation(2.13), the dimension

g is

dWd

dDim

J

d

)(

|

)(1

=g

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,)(!

1)!|(|)(

1=

)(|

in

d

JTn

d

iDn

nd

d

Substituting the value of )()(

JW from eqn. (3.3.1) in the above dimension formula, we have,

!)!()!()!()!(

1)(1)!(

)(1

=

5555

/])1)(

[,/,/,/(

0)5

(

0=5

|

d

s

d

s

d

p

d

q

d

sc

d

v

d

u

d

u

d

q

d

sc

d

v

d

q

d

p

d

q

dd

Dim

dq

cd

vdudqdpmin

svu

sd

g

If we solve the same )()( J

HP using partition and substituting the partition, we have

},,,,,{=)(2121

)( upquqqpT

J

where 1

is partition of v with parts upto 1)(1, c and of length v and 2

is the partition of 5

s with parts

of 5

s of length .5

s

Applying )()(

JT in Witt partition formula (eqn.(2.12))

.2.2)........(3..........|!|)()!()!()!(

1)(1)!(=)(

2121)()(

)(

upquqqp

qW

q

JT

J

From equation(2.13), the dimension

g is

dWd

dDim

J

d

)(

|

)(1

=g

,)(!

1)!|(|)(

1=

)(|

in

d

JTn

d

iDn

nd

d

Substituting the value of )()(

JW from eqn. (3.2.2) in the above dimension formula, we have,

|!|)/()!//()!//()!//(

1)(1)!/()(

1=

2121

/

)()(

2,

1|

dudpdqdudqdqdp

dqd

dDim

dq

JT

d

g

Now consider the equation

.!)!()!()!()!(

1)(1)!(

5555

])1

[,,,(

0=5

sspqcsvuuqcsvqp

qqc

vuqpmin

s

)!()!()!()!(

1)(1)!(=

pqvuuqvqp

qq

1)!1!()!()!()!(

1)(1)!(

pqcvuuqcvqp

qq

2)!2!()!2()!()!2(

1)(1)!(

pqcvuuqcvqp

qq

3)!3!()!3()!()!3(

1)(1)!(

pqcvuuqcvqp

qq

]).1

[,,,(=.......5

c

vuqpminsupto

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|!|)()!()!()!(

1)(1)!(=

2121)()(

2,

1

upquqqp

qq

JT

where 1

is partition of v with parts upto 1)(1, c and of length v and 2

is the partition of 5

s with parts

of 5

s of length .5

s

Hence we proved the following theorem.

Theorem 3.2.1: For the extended-hyperbolic Borcherds superalgebra ),,(= CmAgg associated with the

extended-hyperbolic Borcherds-Cartan super matrix

220

121

012=

c

b

a

cbak

A let us consider

Qvuqp

4321== . Then the dimension of

g is

.

!)!()!()!()!(

1)(1)!(

)(1

=

5555

/])1)(

[,/,/,/(

0)5

(

0=5

|

d

s

d

s

d

p

d

q

d

sc

d

v

d

u

d

u

d

q

d

sc

d

v

d

q

d

p

d

q

dd

Dim

dq

cd

vdudqdpmin

svu

sd

g

Moreover the following combinatorial identity holds:

)3.2.3.(..........|!|)()!()!()!(

1)(1)!(

=!)!()!()!()!(

1)(1)!(

2121)()(

2,

1

5555

])1

[,,,(

0=5

upquqqp

q

sspqcsvuuqcsvqp

q

q

JT

qc

vuqpmin

s

where 1

is partition of v with parts upto )(1, c and of length v and 2

is the partition of 5

s with parts of

5s of length .

5s

Example 3.2.2: For the Borcherds-Cartan super matrix ,

220

121

0121

1

=

c

b

cbk

A

consider the root = = ),,,(=(7,6,4,3) vuqp with c=1. Applying in equation (3.2.1), we have

!)!()!()!()!(

1)(1)!(

5555

])1

[,,,(

0=5

sspqcsvuuqcsvqp

qqc

vuqpmin

s

!)!7(6)!3(44)!(6)!36(7

1)(1)!(6=

5555

61

0=5

sssss

5!2!0!0!1!

(1)5!

4!2!1!0!

(1)5!=

3.=2

1

2

5=

Consider the root = as (7,6,4,3) with c=1. Applying in equation (3.2.2), we have

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7)!1!(61)!3(44)!(61)!36(7

1)(1)!(6

7)!0!(63)!(44)!(63)!6(7

1)(1)!(6=

|!|)()!()!()!(

1)(1)!(

66

2121)()(

2,

1

upquqqp

qq

JT

3.=2

1

2

5=

Hence the equality (3.2.3) holds.

Remark: In the above two sections 3.1 and 3.2., the identities (3.1.4) and (3.2.3) hold for any root, because we

have derived the identities by simply solving the )()(

JT in two different ways.

Remark: It is hoped that, in general, superdimensions of roots and the corresponding combinatorial identities

for Borcherds Superalgebras which are extensions of all finite dimensional Kac-Moody algebras and

superdimensions for all other categories can also be found out.

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