minus-Y90 gate
| Identifier | Operator | Example statement |
|---|---|---|
| mY90 | \(Y^{-1/2}\) | mY90 q[0] |
Description
The minus-Y90 gate or mY90 gate, i.e., the complex conjugate (inverse) of the Y90 gate, is an anti-clockwise rotation of \(-\pi/2\) [rad] about the \(\hat{\mathbf{y}}\)-axis and a global phase of \(-\pi/4\) [rad].
It is equal to half the inverse of the \(Y\) rotation: \(Y^{-1/2}\).
Properties
Representation
\[\begin{align}
Y^{-1/2} &= \frac{1}{2}\left(\begin{matrix}
1 - i & 1 - i \\
-1 + i & 1 - i
\end{matrix}\right)
\end{align}\]
Any single-qubit operation in \(U(2)\) (including global phase) can be expressed by 5 parameters in the canonical representation \(R_\hat{\mathbf{n}}\)
\[R_\hat{\mathbf{n}}\left([n_x, n_y, n_z]^T, \theta, \phi\right) = e^{i\phi} \cdot e^{-i\frac{\theta}{2}\left(n_x\cdot\sigma_x + n_y\cdot\sigma_y + n_z\cdot\sigma_z\right)},\]
where \(\hat{\mathbf{n}}=[n_x, n_y, n_z]^T\) denotes the axis of rotation, \(\theta\in(-\pi, \pi]\) the angle of rotation [rad], and \(\phi\in[0,2\pi)\) the global phase angle [rad].
The minus Y90 gate is given by:
\[\begin{align}
Y^{-1/2} &= R_\hat{\mathbf{n}}\left([0, 1, 0]^T, -\frac{\pi}{2}, -\frac{\pi}{4}\right) = e^{-i\frac{\pi}{4}} \cdot e^{i\frac{\pi}{4}\sigma_y}, \\
\\
Y^{-1/2} &= \frac{1}{2}\left(\begin{matrix}
1 - i & 1 - i \\
-1 + i & 1 - i
\end{matrix}\right).
\end{align}\]
In the Hadamard basis \(\{|+\rangle, |-\rangle\}\), the minus Y90 gate \(Y^{-1/2}_H\) is given by:
\[Y^{-1/2}_H = HY^{-1/2}H = \frac{1}{2}\left(\begin{matrix}
1 - i & -1 + i \\
1 - i & 1 - i
\end{matrix}\right)=(Y^{-1/2})^T.\]
Operation examples
Standard basis
\[\begin{align}
Y^{-1/2}\,|0\rangle &= \frac{1 - i}{2}|0\rangle + \frac{-1 + i}{2}|1\rangle \\
\\
Y^{-1/2}\,|1\rangle &= \frac{1 - i}{2}|0\rangle + \frac{1 - i}{2}|1\rangle \\
\end{align}\]
Hadamard basis
\[\begin{align}
Y^{-1/2}\,|+\rangle &= \frac{1 - i}{2}|+\rangle + \frac{1 - i}{2}|-\rangle \\
\\
Y^{-1/2}\,|-\rangle &= \frac{-1 + i}{2}|+\rangle + \frac{1 - i}{2}|-\rangle \\
\end{align}\]