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--- zero-state [June 12, 2026 at 22:31] – Ivan Janevski
+++ zero-state [Unknown date] (current) – removed - external edit (Unknown date) 127.0.0.1
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-# $\lvert 0\rangle$ (Zero state)
-The **zero state** $\lvert 0\rangle$ is one of the two computational basis states of a qubit. It is the quantum analogue of a classical `0` bit, and it is the standard initial state used in most quantum circuits. The other computational basis state is [[one-state|$\lvert 1\rangle$]].
-$$\lvert 0\rangle = \begin{pmatrix}1\\0\end{pmatrix}$$
-On the [[bloch-sphere]], $\lvert 0\rangle$ corresponds to the north pole at coordinates $(0, 0, 1)$. It is an eigenstate of the Pauli-Z gate with eigenvalue $+1$, meaning $Z\lvert 0\rangle = \lvert 0\rangle$. Applying the [[h-gate|Hadamard gate]] to $\lvert 0\rangle$ produces the equal superposition state $\lvert +\rangle = (\lvert 0\rangle + \lvert 1\rangle)/\sqrt{2}$.
-## Applying gates
-*See also*: [[applying-gates-to-zero-state]]
-^ Gate ^ Result ^ Comment ^
-| [[i-gate]] | $I\lvert 0\rangle = \lvert 0\rangle$ | The identity gate leaves $\lvert 0\rangle$ unchanged. |
-| [[x-gate]] | $X\lvert 0\rangle = \lvert 1\rangle$ | Flips $\lvert 0\rangle$ to $\lvert 1\rangle$; quantum analogue of classical NOT. |
-| [[y-gate]] | $Y\lvert 0\rangle = i\lvert 1\rangle$ | Bit flip with an imaginary phase factor. |
-| [[z-gate]] | $Z\lvert 0\rangle = \lvert 0\rangle$ | $\lvert 0\rangle$ is an eigenstate of $Z$ with eigenvalue $+1$. |
-| [[h-gate]] | $H\lvert 0\rangle = \lvert +\rangle$ | Rotates the north pole to the $+x$ equatorial point of the Bloch sphere. |
-| [[s-gate]] | $S\lvert 0\rangle = \lvert 0\rangle$ | Phase only affects the $\lvert 1\rangle$ component; $\lvert 0\rangle$ is unchanged. |
-| [[t-gate]] | $T\lvert 0\rangle = \lvert 0\rangle$ | Phase only affects the $\lvert 1\rangle$ component; $\lvert 0\rangle$ is unchanged. |
-| [[rx-gate|$R_x(\theta)$]] | $R_x(\theta)\lvert 0\rangle = \cos\tfrac{\theta}{2}\lvert 0\rangle - i\sin\tfrac{\theta}{2}\lvert 1\rangle$ | Tilts the state from $\lvert 0\rangle$ toward $\lvert 1\rangle$ with an imaginary phase on the $\lvert 1\rangle$ component. |
-| [[ry-gate|$R_y(\theta)$]] | $R_y(\theta)\lvert 0\rangle = \cos\tfrac{\theta}{2}\lvert 0\rangle + \sin\tfrac{\theta}{2}\lvert 1\rangle$ | Real amplitudes; at $\theta=\pi/2$ gives $\lvert +\rangle$, the same result as the Hadamard gate up to global phase. |
-| [[rz-gate|$R_z(\theta)$]] | $R_z(\theta)\lvert 0\rangle = e^{-i\theta/2}\lvert 0\rangle$ | Global phase only; $\lvert 0\rangle$ is on the $z$-axis so a $z$-rotation has no observable effect. |
-| [[u-gate|$U(\theta,\phi,\lambda)$]] | $U\lvert 0\rangle = \cos\tfrac{\theta}{2}\lvert 0\rangle + e^{i\phi}\sin\tfrac{\theta}{2}\lvert 1\rangle$ | $\lambda$ drops out; every single-qubit state is reachable from $\lvert 0\rangle$ with appropriate $(\theta,\phi)$. |
-| [[cnot-gate|CNOT]] (as control) | $\text{CNOT}\lvert 0\rangle\lvert t\rangle = \lvert 0\rangle\lvert t\rangle$ | Control is off; target qubit $\lvert t\rangle$ is always left unchanged. |
-| [[cnot-gate|CNOT]] (as target) | $\text{CNOT}\lvert c\rangle\lvert 0\rangle = \lvert c\rangle\lvert c\rangle$ | Flipped to $\lvert 1\rangle$ only when the control qubit is $\lvert 1\rangle$. |
-| [[swap-gate|SWAP]] | $\text{SWAP}\lvert 0\rangle\lvert\psi\rangle = \lvert\psi\rangle\lvert 0\rangle$ | Exchanges the two qubit states; the $\lvert 0\rangle$ moves to the second register. |
-| [[iswap-gate|iSWAP]] | $\text{iSWAP}\lvert 00\rangle = \lvert 00\rangle$; $\text{iSWAP}\lvert 01\rangle = i\lvert 10\rangle$ | Adds a phase of $i$ when states are exchanged; trivial when both qubits are $\lvert 0\rangle$. |
-| [[toffoli-gate|Toffoli]] (as control) | $\text{CCX}\lvert 0\rangle\lvert c_2\rangle\lvert t\rangle = \lvert 0\rangle\lvert c_2\rangle\lvert t\rangle$ | Control is off; target is always unchanged regardless of the second control. |
-| [[toffoli-gate|Toffoli]] (as target) | $\text{CCX}\lvert 1\rangle\lvert 1\rangle\lvert 0\rangle = \lvert 1\rangle\lvert 1\rangle\lvert 1\rangle$ | Flipped to $\lvert 1\rangle$ only when both controls are $\lvert 1\rangle$. |
-## Relationship with other states
-^ State ^ Gates ^ Comment ^
-| $\lvert 0\rangle$ | $I \lvert 0\rangle = \lvert 0\rangle$ | The identity gate leaves $\lvert 0\rangle$ unchanged |
-^ State ^ Relationship ^
-| $\lvert 0\rangle$ | This state. The north pole of the [[bloch-sphere|Bloch sphere]] at $(0,0,1)$, with vector $\begin{pmatrix}1\\0\end{pmatrix}$. It is an eigenstate of $Z$ with eigenvalue $+1$, and measuring it always yields outcome $0$ with probability $1$. |
-| [[one-state|$\lvert 1\rangle$]] | The other computational basis state, at the south pole of the Bloch sphere. $\lvert 0\rangle$ and $\lvert 1\rangle$ are orthogonal ($\langle 0\vert 1\rangle = 0$) and together span the qubit Hilbert space. The X gate (quantum NOT) swaps them: $X\lvert 0\rangle = \lvert 1\rangle$ and $X\lvert 1\rangle = \lvert 0\rangle$. |
-| [[plus-state|$\lvert +\rangle$]] | The equal superposition $\tfrac{1}{\sqrt{2}}(\lvert 0\rangle + \lvert 1\rangle)$, produced by the Hadamard gate: $H\lvert 0\rangle = \lvert +\rangle$. The Bloch vector moves from the north pole to the $+x$ equatorial point. In reverse, $\lvert 0\rangle = \tfrac{1}{\sqrt{2}}(\lvert +\rangle + \lvert -\rangle)$ — the symmetric superposition of both X-basis eigenstates. |
-| [[minus-state|$\lvert -\rangle$]] | Obtained by the two-gate sequence $ZH$: Hadamard maps $\lvert 0\rangle$ to $\lvert +\rangle$, then $Z$ flips the relative phase to give $\lvert -\rangle = \tfrac{1}{\sqrt{2}}(\lvert 0\rangle - \lvert 1\rangle)$. Like $\lvert +\rangle$, it carries equal weight on $\lvert 0\rangle$ and $\lvert 1\rangle$; the sign is the only difference. |
-| [[i-state|$\lvert +i\rangle$]] | The $+y$ pole of the Bloch sphere, $\lvert +i\rangle = \tfrac{1}{\sqrt{2}}(\lvert 0\rangle + i\lvert 1\rangle)$. Prepared from $\lvert 0\rangle$ by $SH$: the Hadamard rotates to the $+x$ equatorial point, and $S$ then rotates 90° around the $z$-axis to reach the $+y$ pole. |
-| [[minus-i-state|$\lvert -i\rangle$]] | The $-y$ pole, $\lvert -i\rangle = \tfrac{1}{\sqrt{2}}(\lvert 0\rangle - i\lvert 1\rangle)$. Prepared by $S^\dagger H\lvert 0\rangle$ — the same two steps with the inverse phase rotation. $\lvert 0\rangle = \tfrac{1}{\sqrt{2}}(\lvert +i\rangle + \lvert -i\rangle)$, so $\lvert 0\rangle$ has equal overlap with both Y-basis eigenstates. |
-| [[phi-plus-state|$\lvert\Phi^+\rangle$]] | The Bell state $\tfrac{1}{\sqrt{2}}(\lvert 00\rangle + \lvert 11\rangle)$, created from two $\lvert 0\rangle$ qubits by applying $H$ to one and then CNOT. Measuring either qubit and finding $\lvert 0\rangle$ collapses the other to $\lvert 0\rangle$ — the qubits are maximally correlated in the $Z$ basis. |
-| [[phi-minus-state|$\lvert\Phi^-\rangle$]] | The Bell state $\tfrac{1}{\sqrt{2}}(\lvert 00\rangle - \lvert 11\rangle)$, created from $\lvert 00\rangle$ by $H\otimes I$, CNOT, then $Z$ on one qubit. Measuring either qubit and finding $\lvert 0\rangle$ still collapses the other to $\lvert 0\rangle$ — same $Z$-basis correlation as $\lvert\Phi^+\rangle$, but with a relative minus sign between the branches. |
-| [[psi-plus-state|$\lvert\Psi^+\rangle$]] | The Bell state $\tfrac{1}{\sqrt{2}}(\lvert 01\rangle + \lvert 10\rangle)$, created from $\lvert 01\rangle$ by $H\otimes I$ then CNOT. Measuring qubit 1 and finding $\lvert 0\rangle$ collapses qubit 2 to $\lvert 1\rangle$ — anti-correlated, opposite to the $\Phi$ Bell states. |
-| [[psi-minus-state|$\lvert\Psi^-\rangle$]] | The singlet Bell state $\tfrac{1}{\sqrt{2}}(\lvert 01\rangle - \lvert 10\rangle)$. Measuring qubit 1 and finding $\lvert 0\rangle$ collapses qubit 2 to $\lvert 1\rangle$, the same anti-correlation as $\lvert\Psi^+\rangle$, but the relative minus sign makes this state antisymmetric under qubit exchange. |
-## List of code implementations
-- [[zero-state-qiskit|Qiskit]]