Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1

284 6. Applications of Determinants in Mathematical Physics


=


r


s

crcsArs. (6.9.13)

The determinantsA,B,P, andQ, their cofactors, and their complex


conjugates are related as follows:


B=Qn+1,n+2;n+1,n+2, (6.9.14)

A=B+Qn+1,n+1, (6.9.15)

A


=(−1)

n
(B−Qn+1,n+1), (6.9.16)

Pn+1,n+2=Qn+1,n+2, (6.9.17)

P


n+1,n+2=(−1)

n+1
Qn+2,n+1, (6.9.18)

Pn+2,n+2=Qn+2,n+2+Q, (6.9.19)

P


n+2,n+2=(−1)

n+1
(Qn+2,n+2−Q). (6.9.20)

The proof of (6.9.14) is obvious. Equation (6.9.15) can be proved as follows:


B+Qn+1,n+1=

∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣

1

1

···

[bij]n ···

···

1

− 1 − 1 ··· − 11

∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣

n+1

. (6.9.21)

Note the element 1 in the bottom right-hand corner. The row operations


R


i=Ri−Rn+1,^1 ≤i≤n, (6.9.22)

yield


B+Qn+1,n+1=

∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣






0

0

···

[bij+1]n ···

···

0

− 1 − 1 ··· − 11

∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣






n+1

. (6.9.23)

Equation (6.9.15) follows by applying (6.9.7) and expanding the determi-

nant by the single nonzero element in the last column. Equation (6.9.16) can


be proved in a similar manner. ExpressQn+1,n+1−Bas a bordered deter-


minant similar to (6.9.21) but with the element 1 in the bottom right-hand


corner replaced by−1. The row operations


R


i=Ri+Rn+1,^1 ≤i≤n, (6.9.24)

leave a single nonzero element in the last column. The result appears after


applying the second line of (6.9.8).

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