Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1

50 3. Intermediate Determinant Theory


=−

n

q=1

n

s=1

vqysAqs.

Similarly,


Bn+1,n+2=+

n

p=1

n

s=1

upysAps,

Bn+2,n+1=+

n

q=1

n

r=1

vqxrAqr,

Bn+2,n+2=−

n

p=1

n

r=1

upxrApr.

Note the variations in the choice of dummy variables. Hence, (3.7.3)


becomes


BA=

n

p,q,r,s=1

upvqxrys





Apr Aps

Aqr Aqs





.

The theorem appears after applying the Jacobi identity and dividing


byA. 


Exercises


1.Prove the Cauchy expansion formula forAij, namely

Aij=apqAip,jq−

n

r=1

n

s=1

apsarqAipr,jqs,

where (p, q)=(i, j) but are otherwise arbitrary. Those terms in which

r=iorpor those in whichs=jorqare zero by the definition of

higher cofactors.

2.Prove the generalized Cauchy expansion formula, namely

A=Nij,hkAij,hk+


1 ≤p≤q≤n


1 ≤r≤s≤n

Nij,rsNpq,hkAijpq,rshk,

where Nij,hk is a retainer minor and Aij,hk is its complementary

cofactor.
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