In functional analysis, the dual norm is a measure of size for a continuous linear function defined on a normed vector space.
Definition
Let
be a normed vector space with norm
and let
denote its continuous dual space. The
dual norm of a continuous linear functional
belonging to
is the non-negative real number defined
by any of the following equivalent formulas:
where
and
denote the supremum and infimum, respectively.
The constant
map is the origin of the vector space
and it always has norm
If
then the only linear functional on
is the constant
map and moreover, the sets in the last two rows will both be empty and consequently, their
will equal
instead of the correct value of
Importantly, a linear function is not, in general, guaranteed to achieve its norm
which holds for all x and z.[This inequality is tight, in the following sense: for any x there is a z for which the inequality holds with equality. (Similarly, for any z there is an x that gives equality.)] The dual of the dual norm is the original norm: we have \|x\|_{**} = \|x\| for all x. (This need not hold in infinite-dimensional vector spaces.)
The dual of the Euclidean norm is the Euclidean norm, since
\sup\{z^\intercal x : \|x\|_2 \leq 1 \} = \|z\|_2.
(This follows from the Cauchy–Schwarz inequality; for nonzero z, the value of x that maximises z^\intercal x over \|x\|_2 \leq 1 is \tfrac{z}{\|z\|_2}.)
The dual of the \ell^\infty -norm is the \ell^1-norm:
\sup\{z^\intercal x : \|x\| _\infty \leq 1\} = \sum_{i=1}^n |z_i| = \|z\| _1,
and the dual of the \ell^1-norm is the \ell^\infty-norm.
More generally, Hölder's inequality shows that the dual of the Lp spaces is the \ell^q-norm, where q satisfies \tfrac{1}{p} + \tfrac{1}{q} = 1, that is, q = \tfrac{p}{p-1}.
As another example, consider the \ell^2- or spectral norm on \R^{m\times n}. The associated dual norm is
\|Z\| _{2*} = \sup\{\mathbf{tr}(Z^\intercal X) : \|X\|_2 \leq 1\},
which turns out to be the sum of the singular values,
\|Z\| _{2*} = \sigma_1(Z) + \cdots + \sigma_r(Z) = \mathbf{tr} (\sqrt{Z^\intercal Z}),
where r = \mathbf{rank} Z. This norm is sometimes called the nuclear operator.
Lp and ℓp spaces
For
p \in 1,, -norm (also called
\ell_p-norm) of vector
\mathbf{x} = (x_n)_n is
\|\mathbf{x}\|_p ~:=~ \left(\sum_{i=1}^n \left|x_i\right|^p\right)^{1/p}.
If p, q \in 1, satisfy 1/p+1/q=1 then the \ell^p and \ell^q norms are dual to each other and the same is true of the L^p and L^q norms, where (X, \Sigma, \mu), is some measure space.
In particular the Euclidean norm is self-dual since p = q = 2.
For \sqrt{x^{\mathrm{T}}Qx}, the dual norm is \sqrt{y^{\mathrm{T}}Q^{-1}y} with Q positive definite.
For p = 2, the \|\,\cdot\,\|_2-norm is even induced by a canonical inner product \langle \,\cdot,\,\cdot\rangle, meaning that \|\mathbf{x}\|_2 = \sqrt{\langle \mathbf{x}, \mathbf{x} \rangle} for all vectors \mathbf{x}. This inner product can expressed in terms of the norm by using the polarization identity.
On \ell^2, this is the defined by
\langle \left(x_n\right)_{n}, \left(y_n\right)_{n} \rangle_{\ell^2} ~=~ \sum_n x_n \overline{y_n}
while for the space L^2(X, \mu) associated with a measure space (X, \Sigma, \mu), which consists of all square-integrable functions, this inner product is
\langle f, g \rangle_{L^2} = \int_X f(x) \overline{g(x)} \, \mathrm dx.
The norms of the continuous dual spaces of \ell^2 and \ell^2 satisfy the polarization identity, and so these dual norms can be used to define inner products. With this inner product, this dual space is also a Hilbert space.
Properties
Given normed vector spaces
X and
Y, let
L(X,Y)[Each L(X,Y) is a vector space, with the usual definitions of addition and scalar multiplication of functions; this only depends on the vector space structure of Y, not X.] be the collection of all
Bounded operator (or ) of
X into
Y. Then
L(X,Y) can be given a canonical norm.
A subset of a normed space is bounded if and only if it lies in some multiple of the unit sphere; thus \|f\| < \infty for every f \in L(X,Y) if \alpha is a scalar, then (\alpha f)(x) = \alpha \cdot f x so that
\|\alpha f\| = |\alpha| \|f\|.
The triangle inequality in Y shows that
\begin{align}
\| \left(f_1 + f_2\right) x \| ~&=~ \|f_1 x + f_2 x\| \\
&\leq~ \|f_1 x\| + \|f_2 x\| \\
&\leq~ \left(\|f_1\| + \|f_2\|\right) \|x\| \\
&\leq~ \|f_1\| + \|f_2\|
\end{align}
for every x \in X satisfying \|x\| \leq 1. This fact together with the definition of \| \cdot \| ~:~ L(X, Y) \to \mathbb{R} implies the triangle inequality:
\|f + g\| \leq \|f\| + \|g\|.
Since \{ |f(x)| : x \in X, \|x\| \leq 1 \} is a non-empty set of non-negative real numbers, \|f\| = \sup \left\{ |f(x)| : x \in X, \| x \| \leq 1 \right\} is a non-negative real number.
If f \neq 0 then f x_0 \neq 0 for some x_0 \in X, which implies that \left\|f x_0\right\| > 0 and consequently \|f\| > 0. This shows that \left( L(X, Y), \| \cdot \|\right) is a normed space.
Assume now that Y is complete and we will show that ( L(X, Y), \| \cdot \|) is complete. Let f_{\bull} = \left(f_n\right)_{n=1}^{\infty} be a Cauchy sequence in L(X, Y), so by definition \left\|f_n - f_m\right\| \to 0 as n, m \to \infty. This fact together with the relation
\left\|f_n x - f_m x\right\| = \left\| \left( f_n - f_m \right) x \right\| \leq \left\|f_n - f_m\right\| \|x\|
implies that \left(f_nx \right)_{n=1}^{\infty} is a Cauchy sequence in Y for every x \in X. It follows that for every x \in X, the limit \lim_{n \to \infty} f_n x exists in Y and so we will denote this (necessarily unique) limit by f x, that is:
f x ~=~ \lim_{n \to \infty} f_n x.
It can be shown that f: X \to Y is linear. If \varepsilon > 0, then \left\|f_n - f_m\right\| \| x \| ~\leq~ \varepsilon \|x\| for all sufficiently large integers and . It follows that
\left\|fx - f_m x\right\| ~\leq~ \varepsilon \|x\|
for sufficiently all large m. Hence \|fx\| \leq \left( \left\|f_m\right\| + \varepsilon \right) \|x\|, so that f \in L(X, Y) and \left\|f - f_m\right\| \leq \varepsilon. This shows that f_m \to f in the norm topology of L(X, Y). This establishes the completeness of L(X, Y).
When Y is a scalar field (i.e. Y = \Complex or Y = \R) so that L(X,Y) is the dual space X^* of X.
Let B ~=~ \sup\{ x \in X ~:~ \| x \| \le 1 \}denote the closed unit ball of a normed space X.
When Y is the scalar field then L(X,Y) = X^* so part (a) is a corollary of Theorem 1. Fix x \in X. There exists y^* \in B^* such that
\langle{x,y^*}\rangle = \|x\|.
but,
|\langle{x,x^*}\rangle| \leq \|x\|\|x^*\| \leq \|x\|
for every x^* \in B^*. (b) follows from the above. Since the open unit ball U of X is dense in B, the definition of \|x^*\| shows that x^* \in B^* if and only if |\langle{x,x^*}\rangle| \leq 1 for every x \in U. The proof for (c) now follows directly.
As usual, let d(x, y) := \|x - y\| denote the canonical metric induced by the norm on X, and denote the distance from a point x to the subset S \subseteq X by
d(x, S) ~:=~ \inf_{s \in S} d(x, s) ~=~ \inf_{s \in S} \|x - s\|.
If f is a bounded linear functional on a normed space X, then for every vector x \in X,
|f(x)| = \|f\| \, d(x, \ker f),
where \ker f = \{k \in X : f(k) = 0\} denotes the kernel of f.
See also
Notes
External links