In mathematical analysis, Hölder's inequality, named after Otto Hölder, is a fundamental inequality between integrals and an indispensable tool for the study of spaces.
The numbers and above are said to be Hölder conjugates of each other. The special case gives a form of the Cauchy–Schwarz inequality. Hölder's inequality holds even if is infinite, the right-hand side also being infinite in that case. Conversely, if is in and is in, then the pointwise product is in .
Hölder's inequality is used to prove the Minkowski inequality, which is the triangle inequality in the space, and also to establish that is the dual space of for .
Hölder's inequality (in a slightly different form) was first found by . Inspired by Rogers' work, gave another proof as part of a work developing the concept of convex and concave functions and introducing Jensen's inequality, which was in turn named for work of Johan Jensen building on Hölder's work.
The brief statement of Hölder's inequality uses some conventions.
\begin{align} &\left(\intS|f|pd\mu\right)
| ||||
\\ &\left(\intS|g|qd\mu\right)
| ||||
\end{align}
As above, let and denote measurable real- or complex-valued functions defined on . If is finite, then the pointwise products of with and its complex conjugate function are -integrable, the estimate
l|\intSf\bargd\mur|\le\intS|fg|d\mu=\|fg\|1
and the similar one for hold, and Hölder's inequality can be applied to the right-hand side. In particular, if and are in the Hilbert space, then Hölder's inequality for implies
|\langlef,g\rangle|\le\|f\|2\|g\|2,
where the angle brackets refer to the inner product of . This is also called Cauchy–Schwarz inequality, but requires for its statement that and are finite to make sure that the inner product of and is well defined. We may recover the original inequality (for the case) by using the functions and in place of and .
If is a probability space, then just need to satisfy, rather than being Hölder conjugates. A combination of Hölder's inequality and Jensen's inequality implies that
\|fg\|1\le\|f\|p\|g\|q
for all measurable real- or complex-valued functions and on .
For the following cases assume that and are in the open interval with .
For the
n
S
\{1,...,n\}
n | |
\sum | |
k=1 |
|xkyk|\lel(
n | |
\sum | |
k=1 |
p | |
|x | |
k| |
| ||||
r) |
l(
n | |
\sum | |
k=1 |
q | |
|y | |
k| |
| ||||
r) |
forall(x1,\ldots,xn),(y1,\ldots,y
norC | |
n)\inR |
n.
(r,s)\inR+
n | |
l(\sum | |
k=1 |
s | |
|x | |
k| |
r)r+s\lel(
n | |
\sum | |
k=1 |
r+s | |
|x | |
k| |
r)rl(
n | |
\sum | |
k=1 |
r+s | |
|y | |
k| |
r)s.
λi
λa+λb+ … +λz=1
n | |
\sum | |
k=1 |
λa | |
|a | |
k| |
λb | |
|b | |
k| |
…
λz | |
|z | |
k| |
\le
n | |
l(\sum | |
k=1 |
λa | |
|a | |
k|r) |
n | |
l(\sum | |
k=1 |
λb | |
|b | |
k|r) |
…
n | |
l(\sum | |
k=1 |
λz | |
|z | |
k|r) |
.
|a1|:|a2|: … :|an|=|b1|:|b2|: … :|bn|= … =|z1|:|z2|: … :|zn|
If
S=\N
infty | |
\sum | |
k=1 |
|xkyk|\lel(
infty | |
\sum | |
k=1 |
p | |
|x | |
k| |
| ||||
r) |
\left(
infty | |
\sum | |
k=1 |
q | |
|y | |
k| |
| ||||
\right) |
forall(xk)k\inN,(yk)k\inN\inRNorCN.
If
S
\Rn
f
g
S
\intSl|f(x)g(x)r|dx\lel(\intS|f(x)|pdxr)
| ||||
l(\intS|g(x)|qdxr)
| ||||
.
(\Omega,l{F},P),
E
X
Y
\Omega,
E[|XY|]\leqslant\left(El[|X|pr]\right)
| ||||
\left(El[|Y|qr]\right)
| ||||
.
Let
1<r<s<infty
p=\tfrac{s}{r}.
q=\tfrac{p}{p-1}
p.
|X|r
1\Omega
El[|X|rr]\leqslant\left(El[|X|sr]\right)
| ||||
.
In particular, if the th absolute moment is finite, then the th absolute moment is finite, too. (This also follows from Jensen's inequality.)
For two σ-finite measure spaces and define the product measure space by
S=S1 x S2, \Sigma=\Sigma1 ⊗ \Sigma2, \mu=\mu1 ⊗ \mu2,
where is the Cartesian product of and, the arises as product σ-algebra of and, and denotes the product measure of and . Then Tonelli's theorem allows us to rewrite Hölder's inequality using iterated integrals: If and are real- or complex-valued functions on the Cartesian product , then
\int | |
S1 |
\int | |
S2 |
|f(x,y)g(x,y)|\mu2(dy)\mu1(dx)
\le\left(\int | |
S1 |
\int | |
S2 |
p\mu | |
|f(x,y)| | |
2(dy)\mu |
| ||||
1(dx)\right) |
\left(\int | |
S1 |
\int | |
S2 |
q\mu | |
|g(x,y)| | |
2(dy)\mu |
| ||||
1(dx)\right) |
.
This can be generalized to more than two measure spaces.
Let denote a measure space and suppose that and are -measurable functions on, taking values in the -dimensional real- or complex Euclidean space. By taking the product with the counting measure on, we can rewrite the above product measure version of Hölder's inequality in the form
\intS
n|f | |
\sum | |
k(x)g |
k(x)|\mu(dx)\le\left(\intS\sum
p\mu(dx)\right) | |
k(x)| |
| ||||
\left(\intS\sum
q\mu(dx)\right) | |
k(x)| |
| ||||
.
If the two integrals on the right-hand side are finite, then equality holds if and only if there exist real numbers, not both of them zero, such that
\alpha\left
p | |
(|f | |
n(x)| |
\right)=\beta\left
q | |
(|g | |
n(x)| |
\right),
for -almost all in .
This finite-dimensional version generalizes to functions and taking values in a normed space which could be for example a sequence space or an inner product space.
There are several proofs of Hölder's inequality; the main idea in the following is Young's inequality for products.
Alternative proof using Jensen's inequality:
We could also bypass use of both Young's and Jensen's inequalities. The proof below also explains why and where the Hölder exponent comes in naturally.
Assume that and let denote the Hölder conjugate. Then for every,
\|f\|p=max\left\{\left|\intSfgd\mu\right|:g\inLq(\mu),\|g\|q\le1\right\},
where max indicates that there actually is a maximizing the right-hand side. When and if each set in the with contains a subset with (which is true in particular when is), then
\|f\|infty=\sup\left\{\left|\intSfgd\mu\right|:g\inL1(\mu),\|g\|1\le1\right\}.
p=infty
A
\sigma
\Sigma
B\in\Sigma
0<\mu(B)<infty.
\sigma
\Sigma
S,
\mu
\mu(S)=infty.
1A
\|1A\|infty=1,
g\inL1(\mu)
\mu
A,
\Sigma
g
\mu
1A
p=infty,
S=N,\Sigma=l{P}(N)
\mu
\begin{cases}f:N\toR\ f(n)=
n-1 | |
n |
\end{cases}
Then
\|f\|infty=1.
g\inL1(\mu,N)
0<\|g\|1\leqslant1,
m
g(m) ≠ 0.
\left|\intSfgd\mu\right|\leqslant
m-1 | |
m |
infty|g(n)| | |
|g(m)|+\sum | |
n=m+1 |
=
\|g\| | ||||
|
\kappaf(g)=\intSfgd\mu, g\inLq(\mu).
The extremal equality (when true) shows that the norm of this functional as element of the continuous dual space coincides with the norm of in (see also the article).
Assume that and such that
n | |
\sum | |
k=1 |
1{p | |
k} |
=
1r | |
where 1/∞ is interpreted as 0 in this equation. Then for all measurable real or complex-valued functions defined on,
n | |
\left\|\prod | |
k=1 |
fk\right\|r\le
n | |
\prod | |
k=1 |
\left\|fk\right\|
pk |
where we interpret any product with a factor of ∞ as ∞ if all factors are positive, but the product is 0 if any factor is 0.
In particular, if
fk\in
pk | |
L |
(\mu)
k\in\{1,\ldots,n\}
n | |
\prod | |
k=1 |
fk\inLr(\mu).
Note: For
r\in(0,1),
Proof of the generalization:
Let and let denote weights with . Define
p
1p | |
= |
n | |
\sum | |
k=1 |
\thetak | |
pk |
.
Given measurable real- or complex-valued functions
fk
\left\|
\theta1 | |
|f | |
1| |
…
\thetan | |
|f | |
n| |
\right\|p\le
\theta1 | |
\left\||f | |
1| |
\right\| | ||||
|
… \left\|
\thetan | |
|f | |
n| |
\right\| | ||||
|
=\|f1\|
\theta1 | |
p1 |
… \|fn\|
\thetan | |
pn |
.
In particular, taking
f1= … =fn=:f
\|f\|p\leqslant
n | |
\prod | |
k=1 |
\thetak | |
\|f\| | |
pk |
.
Specifying further and, in the case
n=2,
An application of Hölder gives
Both Littlewood and Lyapunov imply that if
f\in
p0 | |
L |
\cap
p1 | |
L |
f\inLp
p0<p<p1.
Assume that and that the measure space satisfies . Then for all measurable real- or complex-valued functions and on such that for all,
\|fg\|1\geqslant
\|f\| | ||||
|
\|g\| | ||||
|
.
If
\|fg\|1<infty and
\|g\| | ||||
|
>0,
then the reverse Hölder inequality is an equality if and only if
\exists\alpha\geqslant0 |f|=
| ||||
\alpha|g| |
\mu-almosteverywhere.
Note: The expressions:
\|f\| | ||||
|
\|g\| | ||||
|
,
are not norms, they are just compact notations for
\left
| ||||
(\int | ||||
S|f| |
d\mu\right)p and \left
| ||||
(\int | ||||
S|g| |
d\mu\right)-(p-1).
The Reverse Hölder inequality (above) can be generalized to the case of multiple functions if all but one conjugate is negative.That is,
Let
p1,...,pm-1<0
pm\inR
m | |
\sum | |
k=1 |
1 | |
pk |
=1
0<pm<1
fk
k=1,...,m
m | |
\left\|\prod | |
k=1 |
fk\right\|1\ge
m | |
\prod | |
k=1 |
\left\|fk\right\|
pk |
.
This follows from the symmetric form of the Hölder inequality (see below).
It was observed by Aczél and Beckenbach[2] that Hölder's inequality can be put in a more symmetric form, at the price of introducing an extra vector (or function):
Let
f=(f(1),...,f(m)),g=(g(1),...,g(m)),h=(h(1),...,h(m))
f(i)g(i)h(i)=1
i
p,q,r
1 | + | |
p |
1 | + | |
q |
1 | |
r |
=0
\|f\|p\|g\|q\|h\|r\ge1
p,q,r
\|f\|p\|g\|q\|h\|r\le1
p,q,r
The standard Hölder inequality follows immediately from this symmetric form (and in fact is easily seen to be equivalent to it). The symmetric statement also implies the reverse Hölder inequality (see above).
The result can be extended to multiple vectors:
Let
f1,...,fn
n
Rm
f1(i)...fn(i)=1
i
p1,...,pn
1 | +...+ | |
p1 |
1 | |
pn |
=0
\|f1\|
p1 |
...\|fn\|
pn |
\ge1
pi
\|f1\|
p1 |
...\|fn\|
pn |
\le1
pi
As in the standard Hölder inequalities, there are corresponding statements for infinite sums and integrals.
Let be a probability space, a, and Hölder conjugates, meaning that . Then for all real- or complex-valued random variables and on ,
El[|XY||l{G}r]\lel(El[|X|p|l{G}r]r)
| ||||
l(El[|Y|q|l{G}r]r)
| ||||
P-almostsurely.
Remarks:
E[Z|l{G}]=\supn\inNE[min\{Z,n\}|l{G}] a.s.
Proof of the conditional Hölder inequality:
Let be a set and let
F(S,C)
F(S,C),
f,g\inF(S,C)
\foralls\inS f(s)\geqslantg(s)\geqslant0 ⇒ N(f)\geqslantN(g).
Then:
\forallf,g\inF(S,C) N(|fg|)\leqslantl(N(|f|p)r)
| ||||
l(N(|g|q)r)
| ||||
,
where the numbers
p
q
Remark: If is a measure space and
N(f)
|f|
Hölder inequality can be used to define statistical dissimilarity measures[4] between probability distributions. Those Hölder divergences are projective: They do not depend on the normalization factor of densities.