Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1
4.8 Hankelians 1 111

4.8.6 Partial Derivatives with Respect toφm.......


InAn, the elementsφm,φ 2 n− 2 −m,0≤m≤n−2, each appear in (m+1)


positions. The elementφn− 1 appears innpositions, all in the secondary


diagonal. Hence,∂An/∂φmis the sum of a number of cofactors, one for


each appearance ofφm. Discarding the suffixn,


∂A

∂φm

=


p+q=m+2

Apq. (4.8.23)

For example, whenn≥4,


∂A

∂φ 3

=


p+q=5

Apq

=A 41 +A 32 +A 23 +A 14.

By a similar argument,


∂Aij

∂φm

=


p+q=m+2

Aip,jq, (4.8.24)

∂Air,js

∂φm

=


p+q=m+2

Airp,jsq. (4.8.25)

Partial derivatives of the scaled cofactorsA


ij
andA

ir,js
can be obtained

from (4.8.23)–(4.8.25) with the aid of the Jacobi identity:


∂A

ij

∂φm

=−


p+q=m+2

A

iq
A

pj
(4.8.26)

=


p+q=m+2





A

ij
A

iq

A

pj









. (4.8.27)

The proof is simple.


Lemma.


∂A

ir,js

∂φm

=


p+q=m+2

∣ ∣ ∣ ∣ ∣ ∣

A

ij
A

is
A

iq

A

rj
A

rs
A

rq

A

pj
A
ps





∣ ∣ ∣ ∣ ∣ ∣

, (4.8.28)

which is a development of (4.8.27).


Proof.


∂A

ir,js

∂φm

=

1

A

2

[

A

∂Air,js

∂φm

−Air,js

∂A

∂φm

]

=

1

A

2


p,q

[

AAirp,jsq−Air,jsApq

]

=


p,q

[

A

irp,jsq
−A

ir,js
A

pq

]

. (4.8.29)
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