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In mathematics, a self-adjoint operator on a complex vector space V {\displaystyle V} with inner product ⟨ ⋅ , ⋅ ⟩ {\displaystyle \langle \cdot ,\cdot \rangle } is a linear map A {\displaystyle A} (from V {\displaystyle V} to itself) that is its own adjoint. That is, ⟨ A x , y ⟩ = ⟨ x , A y ⟩ {\displaystyle \langle Ax,y\rangle =\langle x,Ay\rangle } for…
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| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| position | instance of | in which physical observables | 0.80 | text |
| momentum | instance of | in which physical observables | 0.80 | text |
| angular momentum | instance of | in which physical observables | 0.80 | text |
| spin are represented by self-adjoint operators on a Hilbert space | instance of | in which physical observables | 0.80 | text |
| Self-adjoint operator | related to Bounded self-adjoint operators | Let | 0.60 | section |
| Self-adjoint operator | related to Bounded self-adjoint operators | Hilbert | 0.60 | section |
| Self-adjoint operator | related to Bounded self-adjoint operators | Dom | 0.60 | section |
| Self-adjoint operator | related to Bounded self-adjoint operators | According | 0.60 | section |
| Self-adjoint operator | related to Bounded self-adjoint operators | Hellinger | 0.60 | section |
| Self-adjoint operator | related to Bounded self-adjoint operators | Toeplitz | 0.60 | section |
| Self-adjoint operator | related to Bounded self-adjoint operators | Every | 0.60 | section |
| Self-adjoint operator | related to Direct integrals | The | 0.60 | section |
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