= Grover search with a nonzero reflection label
{c}
{title2=$G_y=T_yGT_y,\quad T_y|x\rangle=(-1)^{x\cdot y}|x\rangle$}
Let $|s\rangle=H^{\otimes n}|0^n\rangle$, let $U_f$ be the <marked-state phase oracle>, and replace reflection about $|0^n\rangle$ by reflection about a known <computational basis> vector $|y\rangle$. Define $T_y=\bigotimes_{j=0}^{n-1}Z_j^{y_j}$, so $T_y|x\rangle=(-1)^{x\cdot y}|x\rangle$ and $H^{\otimes n}|y\rangle=T_y|s\rangle$. The resulting Grover iterate obeys
$$
G_y=(2|s_y\rangle\langle s_y|-I)U_f=T_yGT_y,\qquad |s_y\rangle=T_y|s\rangle,
$$
because the two diagonal operators $T_y,U_f$ commute. Thus the good and bad uniform vectors are replaced by their signed vectors $T_y|g\rangle,T_y|b\rangle$, with exactly the same <Grover rotation angle>. Initializing in $H^{\otimes n}|y\rangle$ gives $G_y^r|s_y\rangle=T_yG^r|s\rangle$. Computational-basis measurement probabilities are unchanged because $T_y$ only multiplies amplitudes by signs.
Back to article page
