Adjoint of a Bra-Ket: Definition & Derivation

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In summary, the adjoint of a bra-ket follows the definition of a sesquilinear form and can also be derived through the action of a linear functional on a vector.
  • #1
Alexis21
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Hello everybody,

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

[itex] < \phi | \psi >^+ = < \psi | \phi >[/itex]

Is it a definition or can it be derived somehow?

Thanks :)
 
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  • #2
The scalar product in a (pre-)Hilbert space is a sesquilinear form, i.e., by definition

[tex]\langle \psi|\phi \rangle = \langle \phi|\psi \rangle^*[/tex]

and

[tex]\langle \psi | \alpha \phi_1 + \beta \phi_2 \rangle = \alpha \langle \psi | \phi_1 \rangle + \beta \langle \psi | \phi_2 \rangle.
[/tex]
 
  • #3
Thank you!
 
  • #4
When [itex]\langle\psi|\phi\rangle[/itex] denotes the inner product (or semi-inner product) of [itex]\psi[/itex] and [itex]\phi[/itex], what vanhees71 said is the complete answer. But if it denotes [itex]\langle\psi|[/itex] acting on [itex]|\phi\rangle[/itex], some elaboration is required. [itex]\langle\psi|[/itex] is defined as a function that takes kets to complex numbers. To be more specific, it's defined as the function such that takes [itex]|\phi\rangle[/itex] to [itex]\big(|\psi\rangle,|\phi\rangle\big)[/itex]. (Here I'm using the [itex](\cdot,\cdot)[/itex] notation for the inner product of two kets, to make things more readable). Now we can prove it like this:
[tex]\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[/tex] 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.
 
  • #5
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.
 

FAQ: Adjoint of a Bra-Ket: Definition & Derivation

1. What is the adjoint of a bra-ket?

The adjoint of a bra-ket is the complex conjugate of the original bra-ket, where the bra and ket are interchanged and the complex conjugate of each element is taken. The adjoint is denoted by a dagger symbol, for example, <A| becomes |A>†.

2. What is the significance of the adjoint of a bra-ket?

The adjoint is an important concept in quantum mechanics as it allows for the calculation of expectation values and probabilities. It also plays a crucial role in the definition of operators and in the derivation of the Schrödinger equation.

3. How is the adjoint of a bra-ket derived?

The adjoint is derived by taking the complex conjugate of the original bra-ket and rearranging the elements. This can be done using the properties of complex conjugation and the definition of the inner product.

4. Are there any properties of the adjoint of a bra-ket?

Yes, there are several properties of the adjoint of a bra-ket. For example, the adjoint of a sum is equal to the sum of the adjoints, and the adjoint of a product is equal to the product of the adjoints in reverse order. These properties can be proven using the definition of the adjoint and the properties of complex conjugation.

5. How is the adjoint of a bra-ket used in quantum mechanics?

The adjoint of a bra-ket is used to calculate expectation values and probabilities in quantum mechanics. It is also used in the definition of operators, which are essential for describing the evolution of quantum systems. The adjoint allows for the calculation of complex amplitudes and probabilities, which are crucial for understanding the behavior of quantum systems.

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