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American Journal of Physics

Antilinear operators in Dirac’s bra–ket notation

Antoine Royer

Published Aug 1, 1994• 1 citation
Publisher

Abstract

A notation is introduced which makes the manipulation of antilinear operators within Dirac’s bra–ket notation as efficient as that of linear operators.
DOI
10.1119/1.17506

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According to Dirac's bra-ket notation, in an inner-product space, the inner product ⟨x ∣ y⟩\langle x\,|\,y\rangle⟨x∣y⟩ of vectors x,yx,yx,y can be viewed as an application of the bra ⟨x∣\langle x|⟨x∣ to the ket ∣y⟩|y\rangle∣y⟩. Here ⟨x∣\langle x|⟨x∣ is the linear functional ∣y⟩↦⟨x ∣ y⟩|y\rangle \mapsto \langle x\,|\,y\rangle∣y⟩↦⟨x∣y⟩ and ∣y⟩|y\rangle∣y⟩ is the vector yyy. But often -- though not always -- there are advantages in seeing ∣y⟩|y\rangle∣y⟩ as the function a↦a⋅ya \mapsto a\cdot ya↦a⋅y where aaa ranges over the scalars. For example, the outer product ∣y⟩⟨x∣|y\rangle\langle x|∣y⟩⟨x∣ becomes simply the composition ∣y⟩∘⟨x∣|y\rangle \circ \langle x|∣y⟩∘⟨x∣. It would be most convenient to view kets sometimes as vectors and sometimes as functions, depending on the context. This turns out to be possible. While the bra-ket notation arose in quantum mechanics, this note presupposes no familiarity with quantum mechanics.