Adjoint of a Bra-Ket: Definition & Derivation

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Discussion Overview

The discussion centers around the adjoint of a bra-ket in quantum mechanics, specifically examining its definition and potential derivation. Participants explore the properties of the inner product in the context of (pre-)Hilbert spaces and the mathematical implications of these definitions.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the adjoint of a bra-ket is a definition or can be derived.
  • Another participant states that the scalar product is a sesquilinear form, providing a definition that relates the inner product of two states.
  • A further contribution clarifies that if the bra-ket denotes an inner product, the previous explanation suffices, but if it denotes a linear functional acting on a ket, additional elaboration is necessary.
  • This participant provides a detailed proof involving the properties of the inner product and the definition of the bra-ket notation.
  • Another participant asserts that the bra-ket notation is not merely a scalar product but represents the action of a linear functional on a vector, resulting in a scalar.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the bra-ket notation and its relationship to the scalar product, indicating that multiple competing interpretations remain without consensus.

Contextual Notes

Some assumptions regarding the definitions of inner products and linear functionals are not fully explored, and the discussion does not resolve the implications of these definitions on the adjoint operation.

Alexis21
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Hello everybody,

why is the adjoint of a bra-ket like this:

< \phi | \psi >^+ = < \psi | \phi >

Is it a definition or can it be derived somehow?

Thanks :)
 
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The scalar product in a (pre-)Hilbert space is a sesquilinear form, i.e., by definition

\langle \psi|\phi \rangle = \langle \phi|\psi \rangle^*

and

\langle \psi | \alpha \phi_1 + \beta \phi_2 \rangle = \alpha \langle \psi | \phi_1 \rangle + \beta \langle \psi | \phi_2 \rangle.<br />
 
Thank you!
 
When \langle\psi|\phi\rangle denotes the inner product (or semi-inner product) of \psi and \phi, what vanhees71 said is the complete answer. But if it denotes \langle\psi| acting on |\phi\rangle, some elaboration is required. \langle\psi| is defined as a function that takes kets to complex numbers. To be more specific, it's defined as the function such that takes |\phi\rangle to \big(|\psi\rangle,|\phi\rangle\big). (Here I'm using the (\cdot,\cdot) notation for the inner product of two kets, to make things more readable). Now we can prove it like this:
\langle\psi|\phi\rangle^* =\big(\langle\psi|\big(|\phi\rangle\big)\big)^* =\big(|\psi\rangle,|\phi\rangle\big)^* =\big(|\phi\rangle,|\psi\rangle\big) =\langle\phi|\big(|\psi\rangle\big) =\langle\phi|\psi\rangle The equality in the middle is the same identity that vanhees71 mentioned. As he said, it's part of the definition of an inner product.
 
The bra-ket is not a scalar product, but a short-hand for the action of a linear functional on a vector which yields a complex/real scalar.
 

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