A norm assigns a nonnegative length to each vector, is zero only at the zero vector, is absolutely homogeneous, and satisfies the triangle inequality.
For a real or complex polynomial p(t)=∑k≥0aktk, this finite sum defines a norm: definiteness follows from uniqueness of polynomial coefficients, absolute homogeneity of a norm follows termwise, and the triangle inequality follows by summing ∣ak+bk∣≤∣ak∣+∣bk∣. On [0,1], its supremum norm satisfies ∥p∥∞≤∥p∥coef,1, since ∣tk∣≤1. The reverse comparison has no constant independent of the degree of a polynomial: for pn(t)=(1−t)n, the two norms are 1 and 2n respectively, by the binomial theorem.
A quasi-norm on a vector space is nonnegative, vanishes only at zero, is absolutely homogeneous, and satisfies a triangle inequality with one constant factor C≥1. For 0<p<1, (∫∣f∣p)1/p on an Lp space is a quasi-norm: ∥f+g∥pp≤∥f∥pp+∥g∥pp gives a quasi-triangle inequality. Measure-preserving composition preserves this quantity even though the Minkowski inequality is unavailable below exponent one.
A dual norm measures how strongly a bounded linear functional can respond to a unit-sized input. If p is a bounded linear functional on a normed vector space X, write ⟨p,x⟩=p(x) and defineIt is the operator norm of p when its scalar output is measured by absolute value. On Rn, represent p(x)=aTx using a coefficient vector a. The unit ball is symmetric, so maximizing ∣aTx∣ gives the same value as maximizing aTx: negate an input whenever its output is negative.[ref]
∥p∥∗=sup∥x∥≤1∣p(x)∣.
Convex Optimization by Stephen Boyd and Lieven Vandenberghe. §A.1.6, printed p. 636: dual norm and scalar operator-norm interpretation
For an original two-coordinate example, fix a=(2,−1)T, so p(x)=2x1−x2. The input norm changes the allowable unit ball and hence the dual norm:Under the L1 norm, ∣2x1−x2∣≤2(∣x1∣+∣x2∣)≤2, and (1,0)T attains the bound. Under the Euclidean norm, the Cauchy-Schwarz inequality gives ∣aTx∣≤∥a∥2∥x∥2≤5, with equality at the displayed normalized vector. Under the maximum norm, each coordinate can reach unit absolute value, so ∣2x1−x2∣≤2+1=3; (1,−1)T attains it. Thus the dual norms of these three vector norms are respectively the maximum norm, the Euclidean norm, and the L1 norm. For 1≤p≤∞, Lp norms on a finite coordinate space pair with their Holder conjugate exponents.[ref]
∥x∥1≤1∥x∥2≤1∥x∥∞≤1:∥p∥∗=2,:∥p∥∗=5,:∥p∥∗=3,x∗=(1,0)T,x∗=(2,−1)T/5,x∗=(1,−1)T.
Convex Optimization by Stephen Boyd and Lieven Vandenberghe. §A.1.6, printed p. 637: Euclidean self-duality and one-, infinity- and p-norm duality; the numerical vector and maximizing points here are independent examples
This geometry explains the usefulness of a dual norm: it translates a bound on inputs into the sharp bound on a linear output. The support function of the unit ball gives its value in the coefficient direction a. Changing the input budget changes the set of possible inputs; the three different answers do not conflict. In finite dimensions a closed unit ball is compact, so a continuous linear functional achieves its maximum absolute value. In an infinite-dimensional normed vector space, the supremum remains the definition and need not be achieved.
Suppose a perturbation δx satisfies ∥δx∥≤ε, with ε≥0. Absolute homogeneity of a norm and the dual norm definition giveFor nonzero δx, divide it by its norm to obtain an input in the unit ball; for zero perturbation the inequality is immediate. This is an exact error bound for a linear functional, for every perturbation in the stated input set.
∣p(x+δx)−p(x)∣=∣p(δx)∣≤∥p∥∗∥δx∥≤ε∥p∥∗.
For p(x)=2x1−x2 and a budget ε=0.1, the sharp output-error bounds are 0.2 for ∥δx∥1≤0.1, 5/10≃0.224 for ∥δx∥2≤0.1, and 0.3 for ∥δx∥∞≤0.1. Scale the maximizing vectors from the preceding example by 0.1 to attain the positive endpoints; their negatives attain the negative endpoints. The L1 norm budget constrains a total absolute error; the maximum norm budget permits each coordinate to have that error separately. These budgets define nested sets and carry different information.
Dual norms give exact worst-case errors for the same linear functional
. Original bounds for p(x)=2x1−x2. Lines show the sharp error magnitude as the stated input norm budget increases. The right panel gives the full possible error intervals at ε=0.1; these are the full feasible intervals for the stated deterministic bounds. Details.The coordinates must use the stated scale and units. Rescaling one coordinate changes both its coefficient in a and the meaning of its input budget. For a nonlinear differentiable function with scalar values, its Fréchet derivative at the base point is a linear functional governing the first-order response. An exact finite-perturbation error bound additionally needs control of the Taylor remainder or of the Fréchet derivative along the path.
On the real space of sequences converging to zero c0, use the supremum norm and define the linear functionalThe geometric series gives ∣p(x)∣≤∥x∥∞, so p is a bounded linear functional and ∥p∥∗≤1. The sequence with its first N entries equal to one and all later entries zero belongs to c0, has unit supremum norm, and gives p(x)=1−2−N. Hence ∥p∥∗=1. But if ∥x∥∞≤1 and xn→0, not all coordinates can equal one or all equal minus one. Since every weight 2−n is positive, −1<p(x)<1. The supremum is approached but never attained on the unit ball.
p(x)=∑n=1∞2−nxn.
The block mixed norm sums the ℓq norm of each block, for q≥1. Its dual norm is ∥p∥q′,∞=maxi∥pi∥q′, where q′=q/(q−1) for q>1 and q′=∞ for q=1. Apply Holder inequality blockwise and choose a norming block to attain equality. Absolute values are essential for signed components.
For λ≥0 and a linear map A between finite-dimensional real inner product spaces,Thus the penalty is the support function of the compact convex set A∗{p:maxi∥pi∥q′≤λ}. The Moreau decomposition makes its proximal operator the identity minus the Euclidean projection onto a convex set.
λ∥Au∥q,1=supmaxi∥pi∥q′≤λ⟨A∗p,u⟩.
Definiteness says that a norm vanishes only at the zero vector. The box norm on a nonempty finite Cartesian product is definite because its defining sum of squares includes equal-column terms, each of which is the square of an average of squares. Omitting repeated coordinates would destroy this proof and can produce a different quantity.
Absolute homogeneity is the norm axiom ∥av∥=∣a∣∥v∥ for every scalar a and vector v. It distinguishes a norm from a merely homogeneous expression of a different degree; for example the fourth root in the box norm converts a degree-four expression into a degree-one norm.
On a real vector space, suppose B contains zero, is convex, and meets every line Rv, v=0, in the finite symmetric open segment {tv:∣t∣<λ(v)} with λ(v)>0. Then its Minkowski functional is a norm, with pB(v)=1/λ(v) and B={x:pB(x)<1}. Absolute homogeneity follows by rescaling the segment. If s>pB(x) and t>pB(y), convexity puts (x+y)/(s+t) in B, giving pB(x+y)<s+t; passing to the infima proves the triangle inequality. Conversely the open unit ball uniquely determines any norm by the displayed formula. No prior topology on the vector space is needed for these radial hypotheses.
On a uniform d-dimensional spatial grid, the discrete L2 norm weights the squared Euclidean norm by the cell volume. It approximates the continuous L2 norm and is induced by the discrete L2 inner product. A contraction bound in this norm with a mesh-independent constant proves stability of a numerical method for the spatially discretized evolution.
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- Past exam of the year 1 of the computer science course of the University of Oxford / 2022 / Discrete mathematics, continuous mathematics and probability resit / 3 / d / Solution
- Past exam of the year 1 of the computer science course of the University of Oxford / 2023 / Digital systems, linear algebra and introduction to formal proof / 4 / g / Solution
- Penalized least-squares estimator
- Phase-gate discretization error
- Physics normalization of anyon diagrams
- Planar nematic divergence-elasticity identity
- Poincare inequality with a boundary trace
- Poincare inequality with a partial Dirichlet boundary
- Point evaluation functional
- Point-evaluation kernel is not closed in the integral norm
- Poisson convergence on expanding balls in a homogeneous Sobolev space
- Polarization sum for a massive vector boson
- Polynomial coefficient sum norm
- Polynomial construction of hydrogen S states
- Positive-definite bilinear form
- Positive definiteness of a Gram matrix
- Positive semidefinite Hermitian form
- Power iteration convergence for a diagonalizable matrix
- Power iteration direction error
- Practical stability of a finite difference scheme
- Prime-restriction metric for pretentious distance
- Pseudospectrum
- Pure state on a C-star algebra
- Pythagorean theorem in an inner-product space
- QR decomposition
- QR decomposition by Givens rotations
- Quadratic arch expansion in half-integer cosine modes
- Quadratic form of a positive quantum Hamiltonian
- Quadratic-norm proof of the Heisenberg uncertainty relation
- Quadratic uniformity of a set
- Quantum equilibrium
- Quantum state continuity at a finite Hamiltonian step
- Quantum state ray
- Quantum superposition
- Quantum theory
- Quasi-norm
- Qubit state
- Quotient norm on an irreducible Banach module
- Radial Dirichlet spectrum in three dimensions
- Radial profile
- Radial retraction of a punctured ball
- Rashba spin texture
- Rayleigh quotient
- Reaction contribution in backward Euler energy dissipation
- Real-valued function
- Rectangular corner algebra from a partial isometry
- Regularization of an inverse problem
- Relative state of a bipartite vector
- Renorming a bounded multiplicative semigroup
- Renorming a separately continuous Banach algebra
- Reproducing kernel Hilbert space
- Residual of an inverse problem
- Resolvent components in a closed unital subalgebra
- Restriction-to-rectangle overlap principle
- Retraction of a Hilbert ball onto its sphere
- Riemannian metric
- Riesz-Fischer theorem for an orthonormal system
- Riesz-Thorin theorem
- Runge-Kutta contractivity identity
- Scalar-valued function
- Schauder approximation lemma
- Schilder theorem
- Schur test
- Score test under a simple null
- Seminorm
- Sharp Rademacher second-moment inequality
- Shift domination criterion for a Banach limit
- Sine sequence is not Cauchy in the integral norm
- Single-qubit interference with conditional environment states
- Singular value decomposition
- Smooth convergence on a compact interval
- Sobolev norm
- Space of continuous functions on a compact space
- Spatially homogeneous Boltzmann equation
- Spectral essential range in Borel functional calculus
- Spectral projection of the Stokes operator
- Spectral values attained by C-star states
- Spectrum of a polynomial-generated Banach subalgebra
- Sphere in a normed vector space
- Spherical mean of a Poisson solution outside its source
- Spin expectation value
- Spin ladder operator
- Square-root Lasso
- Stable construction of a Givens rotation
- Standard unit sequences in the real countable product
- Star-algebra
- Star-subalgebra
- State on a C-star algebra
- States and finite-support GNS models of convergent sequences
- Stone's theorem on one-parameter unitary groups
- Strict convexity separates uniqueness from existence in best approximation
- Strong continuity of functional calculus through resolvents
- Strong stability preserving Runge-Kutta method
- Structure theorem for functions of bounded variation
- Sum of Lp spaces
- Swap test
- Symmetric preconditioning as energy geometry
- Test-function seminorm
- Tikhonov regularization
- Topological vector space
- Topology determines norm equivalence
- Total differential
- Total variation under opposite smooth flows
- Translation continuity in Lp
- Transverse one-photon physical quotient
- Triangle counting with one box-uniform pair and constant opposite degree
- Triangle inequality
- Triangle inequality for pretentious distance
- Two-channel scattering with flux normalization
- Two-dimensional partial-wave scattering formula
- Two-pair component of polarization-entangled down-conversion
- Two-particle antisymmetrization
- Unbounded operator
- Unbounded torsion obstructs uniform control of four-term progressions
- Uniform noise bound for relaxed Landweber iteration
- Unital versus nonunital generation by a normal element
- Unitary highest-weight termination
- Unitary operator
- Unitary time evolution
- Unit-circle spectrum of a unitary operator
- Unitization of an algebra
- Unitization of the vanishing-at-zero ideal on an interval
- Unit sphere net from ball covering
- Unit vector
- Unit-width box kernel
- Upwind finite difference scheme
- Vacuum energy density
- Vector
- Vector measure
- Vector normalization is not linear
- Vector state on a C-star algebra
- Vector-valued function
- Velocity vector
- Virasoro Verma module
- Von Neumann algebra
- Wavelet coefficient decay for Hölder functions
- Weak holomorphy implies norm holomorphy
- Weak lower semicontinuity
- Weakly holomorphic Banach-valued function
- Weak mixed Poisson problem
- Weak operator topology
- Weak-star fixed point theorem for an adjoint operator
- Weak-type operator
- Weighted Euclidean inner product
- Weighted Hilbert structure of velocity-reset relaxation
- Weighted holomorphic norm on a shrinking time domain
- Weighted linear projection of a quadratic monomial
- Weighted linear projection of a semicircle profile
- Weighted Neumann heat kernel with constant drift
- Weighted norm
- Weighted permutation unitarity criterion
- Weighted summable sequence space isometry
- Wiener algebra
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