The Pauli X gate interchanges ∣0⟩ and ∣1⟩.
Ancestors (4)
Incoming links (79)
- Ancilla preparation for the Bernstein-Vazirani algorithm
- Bernstein-Vazirani algorithm
- Bit-flip repetition code
- Born rule
- Coherent syndrome extraction for the three-qubit repetition code
- Collisional phase gate
- Deterministic two-qubit entanglement dilution
- Dicke-resource telecloning
- GHZ contradiction for N congruent to 3 modulo 4
- GHZ game
- Heralded Pauli X correction using controlled-Z and measurements
- Logical failure of the three-qubit bit-flip repetition code
- Logical failure of the three-qubit phase-flip repetition code
- Logical Hadamard convention for a phase-flip repetition code
- Measurement-guided Zeno transfer
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- Pauli gate
- Quantum bit-flip channel
- Quantum error correction
- Rotation about the x-axis
- Shor-code phase-flip syndrome
- Singlet-triplet measurement causality obstruction
- Three-qubit bit-flip syndrome table
- Two-outcome LOCC dilution of a Bell pair
- Two-qubit diffusion circuit
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Articles by others on the same topic (1)
The quantum NOT gate swaps the state of ∣0⟩ and ∣1⟩, i.e. it maps:As a result, this gate also inverts the probability of measuring 0 or 1, e.g.
x∣0⟩+y∣y⟩→y∣0⟩+x∣y⟩
- if the old probability of 0 was 0, then it becomes 1
- if the old probability of 0 was 0.2, then it becomes 0.8
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