Multi-index notation

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Short description: Mathematical notation

Multi-index notation is a mathematical notation that simplifies formulas used in multivariable calculus, partial differential equations and the theory of distributions, by generalising the concept of an integer index to an ordered tuple of indices.

Definition and basic properties

An n-dimensional multi-index is an n-tuple

α=(α1,α2,,αn)

of non-negative integers (i.e. an element of the n-dimensional set of natural numbers, denoted 0n).

For multi-indices α,β0n and x=(x1,x2,,xn)n, one defines:

Componentwise sum and difference
α±β=(α1±β1,α2±β2,,αn±βn)
Partial order
αβαiβii{1,,n}
Sum of components (absolute value)
|α|=α1+α2++αn
Factorial
α!=α1!α2!αn!
Binomial coefficient
(αβ)=(α1β1)(α2β2)(αnβn)=α!β!(αβ)!
Multinomial coefficient
(kα)=k!α1!α2!αn!=k!α! where k:=|α|0.
Power
xα=x1α1x2α2xnαn.
Higher-order partial derivative
α=1α12α2nαn, where iαi:=αi/xiαi (see also 4-gradient). Sometimes the notation Dα=α is also used.[1]

Some applications

The multi-index notation allows the extension of many formulae from elementary calculus to the corresponding multi-variable case. Below are some examples. In all the following, x,y,hn (or n), α,ν0n, and f,g,aα:n (or n).

Multinomial theorem
(i=1nxi)k=|α|=k(kα)xα
Multi-binomial theorem
(x+y)α=να(αν)xνyαν. Note that, since x + y is a vector and α is a multi-index, the expression on the left is short for (x1 + y1)α1⋯(xn + yn)αn.
Leibniz formula
For smooth functions f and g,α(fg)=να(αν)νfανg.
Taylor series
For an analytic function f in n variables one has f(x+h)=α0nαf(x)α!hα. In fact, for a smooth enough function, we have the similar Taylor expansion f(x+h)=|α|nαf(x)α!hα+Rn(x,h), where the last term (the remainder) depends on the exact version of Taylor's formula. For instance, for the Cauchy formula (with integral remainder), one gets Rn(x,h)=(n+1)|α|=n+1hαα!01(1t)nαf(x+th)dt.
General linear partial differential operator
A formal linear N-th order partial differential operator in n variables is written as P()=|α|Naα(x)α.
Integration by parts
For smooth functions with compact support in a bounded domain Ωn one has Ωu(αv)dx=(1)|α|Ω(αu)vdx. This formula is used for the definition of distributions and weak derivatives.

An example theorem

If α,β0n are multi-indices and x=(x1,,xn), then αxβ={β!(βα)!xβαifαβ,0otherwise.

Proof

The proof follows from the power rule for the ordinary derivative; if α and β are in {0,1,2,}, then

dαdxαxβ={β!(βα)!xβαifαβ,0otherwise.

 

 

 

 

(1)

Suppose α=(α1,,αn), β=(β1,,βn), and x=(x1,,xn). Then we have that αxβ=|α|x1α1xnαnx1β1xnβn=α1x1α1x1β1αnxnαnxnβn.

For each i in {1,,n}, the function xiβi only depends on xi. In the above, each partial differentiation /xi therefore reduces to the corresponding ordinary differentiation d/dxi. Hence, from equation (1), it follows that αxβ vanishes if αi>βi for at least one i in {1,,n}. If this is not the case, i.e., if αβ as multi-indices, then dαidxiαixiβi=βi!(βiαi)!xiβiαi for each i and the theorem follows. Q.E.D.

See also

References

  1. Reed, M.; Simon, B. (1980). Methods of Modern Mathematical Physics: Functional Analysis I (Revised and enlarged ed.). San Diego: Academic Press. p. 319. ISBN 0-12-585050-6. 
  • Saint Raymond, Xavier (1991). Elementary Introduction to the Theory of Pseudodifferential Operators. Chap 1.1 . CRC Press. ISBN 0-8493-7158-9