Quantum Computing Asked by Srijita Nandi on July 15, 2021
I can’t seem to understand how to show that the Bell states for a basis. Should I explain that through the circuit and what gates are used or by the basic proof behind proving a set as a basis?
If you are taking the four Bell states
$|Phi^+ rangle = dfrac{1}{sqrt{2}}big(|00rangle + |11rangle big) $
$|Phi^- rangle = dfrac{1}{sqrt{2}}big(|00rangle - |11rangle big) $
$|Psi^+ rangle = dfrac{1}{sqrt{2}}big(|01rangle + |10 rangle big) $
$|Psi^- rangle = dfrac{1}{sqrt{2}}big(|01rangle - |10 rangle big) $
and place them as a column of a matrix $U$, for instance:
begin{align} U &= bigg[ hspace{0.2 cm} |Phi^+ rangle hspace{0.2 cm} bigg| hspace{0.2 cm} |Phi^- rangle hspace{0.2 cm} bigg| hspace{0.2 cm} |Psi^+ rangle hspace{0.2 cm} bigg| hspace{0.2 cm} |Psi^- rangle hspace{0.2 cm}bigg] &= dfrac{1}{sqrt{2}}begin{pmatrix} 1 & 0 & 0 & 1 0 & 1 & 1 & 0 0 & 1 & -1 & 0 1 & 0 & 0 & -1 end{pmatrix} end{align}
Here you can see that $U$ is a unitary matrix. That is, $Ucdot U^*= U^* cdot U = I$ where $U^*$ is the conjugate transpose of $U$. Since $U$ is unitary, its columns must form an orthonormal basis. These columns are the Bell states.
Correct answer by KAJ226 on July 15, 2021
The Bell states form an orthonormal basis of 2-qubit Hilbert space. The way to show it is to come back to the definition of what an orthonormal basis is:
Answered by holl on July 15, 2021
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