Bessel's inequality

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Template:Short description In mathematics, especially functional analysis, Bessel's inequality is a statement about the coefficients of an element x in a Hilbert space with respect to an orthonormal sequence. The inequality is named for F. W. Bessel, who derived a special case of it in 1828.[1]

Conceptually, the inequality is a generalization of the Pythagorean theorem to infinite-dimensional spaces. It states that the "energy" of a vector x, given by x2, is greater than or equal to the sum of the energies of its projections onto a set of perpendicular basis directions. The value |x,ek|2 represents the energy contribution along a specific direction ek, and the inequality guarantees that the sum of these contributions cannot exceed the total energy of x.

When the orthonormal sequence forms a complete orthonormal basis, Bessel's inequality becomes an equality known as Parseval's identity. This signifies that the sum of the energies of the projections equals the total energy of the vector, meaning no energy is "lost." The inequality is a crucial tool for establishing the convergence of Fourier series and other series expansions in Hilbert spaces.

Statement of the inequality

Let H be a Hilbert space and let e1,e2, be an orthonormal sequence in H. Then for any vector x in H, Bessel's inequality states:

k=1|x,ek|2x2

where ⟨·,·⟩ denotes the inner product in the Hilbert space H, and denotes the norm induced by the inner product.[2][3][4]

The terms x,ek are the Fourier coefficients of x with respect to the sequence (ek). The inequality implies that the series of the squared magnitudes of these coefficients converges. This allows for the definition of the vector x, which is the projection of x onto the subspace spanned by the orthonormal sequence:

x=k=1x,ekek

Bessel's inequality guarantees that this series converges. If the sequence (ek) is a complete orthonormal basis, then x=x, and the inequality becomes an equality known as Parseval's identity.

Proof

The inequality follows from the non-negativity of the norm of a vector. For any natural number n, let

xn=k=1nx,ekek

This vector xn is the projection of x onto the subspace spanned by the first n basis vectors. The vector xxn is orthogonal to this subspace, and thus orthogonal to xn itself. By the Pythagorean theorem for inner product spaces, we have x2=xn2+xxn2. The proof proceeds by computing xxn2:

0xk=1nx,ekek2=xk=1nx,ekek,xj=1nx,ejej=x2k=1nx,ekx,ekj=1nx,ejej,x+k=1nj=1nx,ekx,ejek,ej=x2k=1n|x,ek|2j=1n|x,ej|2+k=1n|x,ek|2=x2k=1n|x,ek|2

This holds for any n1. Since the partial sums are non-negative and bounded above by x2, the series k=1|x,ek|2 converges and its sum is less than or equal to x2.

Fourier series

In the theory of Fourier series, in the particular case of the Fourier orthonormal system, we get if f: has period T,

k|0Te2πikt/Tf(t)dt|2T0T|f(t)|2dt.

In the particular case where f:, one has then

|0Tf(t)dt|2+2n=1|0Tcos(2πkt/T)f(t)dt|2+2n=1|0Tsin(2πkt/T)f(t)dt|2T0T|f(t)|2dt.

Non countable case

More generally, if H is a pre-Hilbert space and (eα)αA is an orthonormal system, then for every xH[1]

αA|x,eα|2x2

This is proved by noting that if FA is finite, then

αF|x,eα|2x2

and then by definition of infinite sum

αA|x,eα|2=sup{αF|x,eα|2:FA is finite}x2.

See also

References

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External links

This article incorporates material from Bessel inequality on PlanetMath, which is licensed under the Creative Commons Attribution/Share-Alike License.

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