Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1

4 Particular Determinants


4.1 Alternants............................


4.1.1 Introduction


Any function ofnvariables which changes sign when any two of the vari-


ables are interchanged is known as an alternating function. It follows that


an alternating function vanishes if any two of the variables are equal.


Any determinant function which possess these properties is known as an


alternant.


The simplest form of alternant is

|fj(xi)|n=

∣ ∣ ∣ ∣ ∣ ∣ ∣

f 1 (x 1 ) f 2 (x 1 ) ··· fn(x 1 )

f 1 (x 2 ) f 2 (x 2 ) ··· fn(x 2 )

............................

f 1 (xn) f 2 (xn) ··· fn(xn)

∣ ∣ ∣ ∣ ∣ ∣ ∣ n

. (4.1.1)

The interchange of any twox’s is equivalent to the interchange of two rows


which gives rise to a change of sign. If any two of thex’s are equal, the


determinant has two identical rows and therefore vanishes.


The double or two-way alternant is

|f(xi,yj)|n=

∣ ∣ ∣ ∣ ∣ ∣ ∣

f(x 1 ,y 1 ) f(x 1 ,y 2 ) ··· f(x 1 ,yn)

f(x 2 ,y 1 ) f(x 2 ,y 2 ) ··· f(x 2 ,yn)

...................................

f(xn,y 1 ) f(xn,y 2 ) ··· f(xn,yn)

∣ ∣ ∣ ∣ ∣ ∣ ∣ n

. (4.1.2)
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