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Rigged Hilbert space

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x↦eix, is an eigenfunction of the differential operator (H, Φ) with Φ is given a topological vector space structure for which the inclusion map H, the adjoint to Φ and *</sup>"}},"i":0}}]}'/>Φ is then compatible with the inner product on u∈Φ⊂H and v (physics convention), and conjugate-linear (complex anti-linear) in the other variable.

The triple Φ is isomorphic to *</sup>"}},"i":0}}]}'/>Φ (via Riesz representation) if it happens that i* Φ which carries a finer topology, that is one for which the natural inclusion H for the Hilbert norm. We consider the inclusion of dual spaces *</sup>"}},"i":0}}]}'/>H in *</sup>"}},"i":0}}]}'/>Φ. The latter, dual to ϕ↦⟨v,ϕ⟩ for Φ dense).

Now by applying the Riesz representation theorem we can identify *</sup>"}},"i":0}}]}'/>H with Φ is a nuclear space; this comment is an abstract expression of the idea that Φ and its dual 𝒮′(ℝ), respectively, rigging the Hilbert space of square-integrable functions. As such, the rigged Hilbert space is given by H=L2(ℝn), Φ=Hs(ℝn), Φ∗=H−s(ℝn), where 0"}}'>s>0.

See also

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Notes

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Krasnoholovets, Volodymyr; Columbus, Frank H. (2004). New Research in Quantum Physics. Nova Science Publishers. p. 79. ISBN 978-1-59454-001-1.
  • Gel'fand & Vilenkin 1964, pp. 103–105.
  • ↑ de la Madrid Modino 2001, pp. 66–67.
  • ↑ van der Laan 2019, pp. 21–22.
  • ↑ de la Madrid Modino 2001, p. 72.
  • References

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