Questions: Riesz Representation Theorem for Hilbert Spaces
5 questions to test your understanding
Score: 0 / 5
Question 1 Multiple Choice
A bounded linear functional f: H → ℝ is defined on a Hilbert space H. According to the Riesz Representation Theorem, which statement is correct?
Af(x) = ⟨x, y⟩ for some y ∈ H, but y may not be unique
Bf(x) = ⟨x, y⟩ for a unique y ∈ H, and ‖f‖ = ‖y‖
CThis representation holds only when H is finite-dimensional
Df(x) = ‖x‖ · ‖y‖ for some y ∈ H by the Cauchy-Schwarz inequality
The theorem guarantees both existence and uniqueness of the representing vector y. Uniqueness follows because if f(x) = ⟨x, y₁⟩ = ⟨x, y₂⟩ for all x, then ⟨x, y₁ − y₂⟩ = 0 for all x, which forces y₁ − y₂ = 0. The norm equality ‖f‖ = ‖y‖ makes the map y ↦ f_y an isometry. Option C is a common mistake: the theorem holds for all Hilbert spaces, finite or infinite-dimensional. Option D confuses the Cauchy-Schwarz bound |⟨x,y⟩| ≤ ‖x‖‖y‖ with the functional itself.
Question 2 Multiple Choice
What makes Hilbert spaces special compared to general Banach spaces regarding their dual?
AHilbert spaces are always finite-dimensional, making their dual trivially equal to themselves
BThe norm of a Hilbert space is always defined by an inner product, which forces H ≅ H* isometrically
CBounded linear functionals only exist on Hilbert spaces, not on general Banach spaces
DEvery Banach space is isometrically isomorphic to its dual, just as every Hilbert space is
The inner product is the key. The map y ↦ f_y where f_y(x) = ⟨x, y⟩ is an isometric isomorphism from H onto H*. For general Banach spaces X, the dual X* can be a completely different space — for example, the dual of L¹ is L^∞, not L¹. Self-duality is a special feature of Hilbert space geometry, arising because the inner product provides a canonical way to identify vectors with functionals.
Question 3 True / False
The proof of the Riesz Representation Theorem uses the fact that the kernel of a bounded linear functional is a closed subspace of H.
TTrue
FFalse
Answer: True
True, and this is the pivotal step. Continuity of f (which follows from boundedness) ensures that ker(f) = f⁻¹({0}) is closed. The orthogonal complement ker(f)^⊥ is then non-trivial (since f ≠ 0), and the representing vector y is constructed from a unit vector in ker(f)^⊥. Without closedness, the orthogonal decomposition H = ker(f) ⊕ ker(f)^⊥ would not be valid.
Question 4 True / False
For any Banach space X, there is typically an isometric isomorphism between X and its dual X*.
TTrue
FFalse
Answer: False
False. Hilbert spaces are self-dual (H ≅ H* isometrically) by the Riesz theorem, but this is special. For Banach spaces the dual can be entirely different. The dual of L^p is L^q where 1/p + 1/q = 1 (for p ≠ 2), so (L^p)* ≅ L^q ≇ L^p when p ≠ 2. The dual of L^1 is L^∞, not L^1. Only for p = 2, where L² is a Hilbert space, does self-duality hold.
Question 5 Short Answer
Explain in your own words why the Riesz Representation Theorem implies that a Hilbert space is 'self-dual,' and why this is a special feature not shared by all Banach spaces.
Think about your answer, then reveal below.
Model answer: The Riesz theorem says every bounded linear functional on H has the form f(x) = ⟨x, y⟩ for a unique y ∈ H. This means the map φ: H → H* defined by φ(y) = f_y is a bijection — every element of H gives a functional and every functional comes from an element of H. Since the map is also an isometry (‖f_y‖ = ‖y‖) and conjugate-linear, it is an isometric isomorphism H ≅ H*. This self-duality is special because it requires the rich structure of an inner product. In a general Banach space, the norm does not provide a canonical way to pair vectors with functionals, so X and X* can have completely different structures (e.g., the dual of L¹ is L^∞).
Intuition: the inner product ⟨·, y⟩ is already a bounded linear functional for every y, and every bounded functional arises this way. So H and H* are in perfect one-to-one correspondence. In Banach spaces without inner products, there is no such built-in pairing, and the dual can look nothing like the original space.