Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1

202 5. Further Determinant Theory


=

a 1 a 2 a 3 +a 1 b 3 +a 3 b 2

a 1 a 2 a 3 +a 1 b 3 +a 3 b 2 +a 2 a 3 b 1 +b 1 b 3

.

Each of these fractions can be expressed in the formH 11 /H, whereHis a


tridiagonal determinant:


f 1 =

|a 1 |




1 b 1

− 1 a 1





,

f 2 =





a 1 b 2

− 1 a 2

∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣

1 b 1

− 1 a 1 b 2

− 1 a 2

∣ ∣ ∣ ∣ ∣ ∣

,

f 3 =

∣ ∣ ∣ ∣ ∣ ∣

a 1 b 2

− 1 a 2 b 3

− 1 a 3

∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣

1 b 1

− 1 a 1 b 2

− 1 a 2 b 3

− 1 a 3

∣ ∣ ∣ ∣ ∣ ∣ ∣

.

Theorem 5.9.


fn=

H

(n+1)
11

Hn+1

,

where


Hn+1=





∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣

1 b 1

− 1 a 1 b 2

− 1 a 2 b 3

.
.
.

.

.

.

.

.

.

− 1 an− 2 bn− 1

− 1 an− 1 bn

− 1 an





∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣ ∣

n+1

. (5.5.2)

Proof. Use the method of induction. Assume that


fn− 1 =

H

(n)
11

Hn

,

which is known to be true for small values ofn. Hence, addingbn/anto


an− 1 ,


fn=

K

(n)
11

Kn

, (5.5.3)
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