Definition and basic properties
An n-dimensional multi-index is an
-tuple

of non-negative integers (i.e. an element of the
-dimensional set of natural numbers, denoted
).
For multi-indices
and
, one defines:
- Componentwise sum and difference

- Partial order

- Sum of components (absolute value)

- Factorial
- !=\alpha _{1}!\cdot \alpha _{2}!\cdots \alpha _{n}!}

- Binomial coefficient
- !}{\beta !(\alpha -\beta )!}}}

- Multinomial coefficient
- !}}}
where
.
- Power
.
- Higher-order partial derivative
where
(see also 4-gradient). Sometimes the notation
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,
(or
),
, and
(or
).
- Multinomial theorem

- Multi-binomial theorem
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
and
,
- Taylor series
- For an analytic function
in
variables one has !}}h^{\alpha }}.}
In fact, for a smooth enough function, we have the similar Taylor expansion !}}h^{\alpha }}+R_{n}(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 !}}\int _{0}^{1}(1-t)^{n}\partial ^{\alpha }f(x+th)\,dt.}

- General linear partial differential operator
- A formal linear
-th order partial differential operator in
variables is written as 
- Integration by parts
- For smooth functions with compact support in a bounded domain
one has
This formula is used for the definition of distributions and weak derivatives.
An example theorem
If
are multi-indices and
, then
!}{(\beta -\alpha )!}}x^{\beta -\alpha }&{\text{if}}~\alpha \leq \beta ,\\0&{\text{otherwise.}}\end{cases}}}

Proof
The proof follows from the power rule for the ordinary derivative; if α and β are in
, then
!}{(\beta -\alpha )!}}x^{\beta -\alpha }&{\hbox{if}}\,\,\alpha \leq \beta ,\\0&{\hbox{otherwise.}}\end{cases}}}
 | | 1 |
Suppose
,
, and
. Then we have that

For each
in
, the function
only depends on
. In the above, each partial differentiation
therefore reduces to the corresponding ordinary differentiation
. Hence, from equation (1), it follows that
vanishes if
for at least one
in
. If this is not the case, i.e., if
as multi-indices, then
for each
and the theorem follows. Q.E.D.
References
- ↑ 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
This article incorporates material from multi-index derivative of a power on PlanetMath, which is licensed under the Creative Commons Attribution/Share-Alike License.