Mathematical Principles of Theoretical Physics

(Rick Simeone) #1

3.5.SU(N)REPRESENTATION INVARIANCE 163


3.5.4 Intrinsic Riemannian metric onSU(N)


By Theorem3.31,Gab(A)andgabare symmetric. We now show that bothGabandgabare
positive definite, and consequentlyGab(A)is an intrinsic Riemannian metric onSU(N).


Theorem 3.32.For the 2-order SU(N)tensors gabandGab, the following assertions hold
true:


1) The tensor{gab}given by (3.5.30) is positive definite; and

2) For each point A∈SU(N), there is a coordinate system in whereGab(A) =gab. There-
foreGab(A)is a Riemannian metric on SU(N).

Proof.First, we prove Assertion (1). As a 2-order covariant tensor,gabtransforms as


(3.5.35) ( ̃gab) =X(gab)XT, X= (xab)as in( 3. 5. 22 ).


Hence, if for a given basis{τa| 1 ≤a≤K}ofTeSU(N)we can verify thatgab= 41 Nλadcλcbd
is positive definition, then by (3.5.35) we derive Assertion (1). In the following, we proceed
first forSU( 2 )andSU( 3 ), then for the generalSU(N).
ForSU( 2 ), we take the Pauli matrices


(3.5.36) σ 1 =


(


0 1


1 0


)


, σ 2 =

(


0 −i
i 0

)


, σ 3 =

(


1 0


0 − 1


)


as the generator basis ofSU( 2 ). The structure constantsλabc of (3.5.36) are as follows


(3.5.37) λabc= 2 εabc, εabc=









1 if(abc)is even,
−1 if(abc)is odd,
0 if otherwise.

Based on (3.5.37), direct calculation shows that


gab=

1


8


λadcλcbd=δab.

Namely(gab) =Iis identity.
ForSU( 3 ), we can take the following Gell-Mann matrices as the generator basis of
SU( 3 ):


λ 1 =



0 1 0


1 0 0


0 0 0



, λ 2 =



0 −i 0
i 0 0
0 0 0


, λ 3 =



1 0 0


0 −1 0


0 0 0



,


λ 4 =



0 0 1


0 0 0


−1 0 0



, λ 5 =



0 0 −i
0 0 0
i 0 0


, λ 6 =



0 0 0


0 0 1


0 1 0



(3.5.38) ,


λ 7 =



0 0 0


0 0 −i
0 i 0


, λ 8 =√^1
3



1 0 0


0 1 0


0 0 − 2



.

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