Conceptually, the inequality is a generalization of the Pythagorean theorem to infinite-dimensional spaces. It states that the "energy" of a vector , given by , is greater than or equal to the sum of the energies of its projections onto a set of perpendicular basis directions. The value represents the energy contribution along a specific direction , and the inequality guarantees that the sum of these contributions cannot exceed the total energy of .
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 be a Hilbert space and let be an orthonormal sequence in . Then for any vector in , Bessel's inequality states:
where ⟨·,·⟩ denotes the inner product in the Hilbert space , and denotes the norm induced by the inner product.[2][3][4]
The terms are the Fourier coefficients of with respect to the sequence . The inequality implies that the series of the squared magnitudes of these coefficients converges. This allows for the definition of the vector , which is the projection of onto the subspace spanned by the orthonormal sequence:
The inequality follows from the non-negativity of the norm of a vector. For any natural number , let
This vector is the projection of onto the subspace spanned by the first basis vectors. The vector is orthogonal to this subspace, and thus orthogonal to itself. By the Pythagorean theorem for inner product spaces, we have . The proof proceeds by computing :
This holds for any . Since the partial sums are non-negative and bounded above by , the series converges and its sum is less than or equal to .
Fourier series
In the theory of Fourier series, in the particular case of the Fourier orthonormal system, we get if has period ,
In the particular case where , one has then
Non countable case
More generally, if is a pre-Hilbert space and is an orthonormal system, then for every [1]
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