A global phase multiplies an entire quantum state by one complex number of modulus one. It does not change any measurement probability, unlike a relative phase between components.
A physical unitary gate used without coherent control gives the same quantum channel for V and eiγV:Interleaving any preparations, known operations and measurements preserves this equality. Equivalently, each fixed measurement branch with k uses gains only the overall factor eikγ, which cancels in its probability. Thus unrestricted repeated uncontrolled uses do not determine the common phase of the eigenvalues. A supplied controlled unitary gate is a different resource: ∣0⟩⟨0∣⊗I+∣1⟩⟨1∣⊗V changes by a relative control phase when V is replaced by eiγV. Such controlled access permits quantum phase estimation to measure that phase relative to the identity branch.
(eiγV)ρ(eiγV)†=VρV†.
Ancestors (7)
Incoming links (219)
- Ancilla preparation for the Bernstein-Vazirani algorithm
- Berry-phase interference with a reference path
- Berry phase of a Bloch-sphere latitude
- Clifford group (quantum computing)
- Coherent preparation and incoherent mixing
- Collective dephasing
- Collective-unitary covariance of the two-qubit singlet
- Complex scalar charge operator
- Conditional environment overlap
- Diagonal two-qubit phase entanglement criterion
- Endpoint control of an XX spin chain
- Energy eigenfunction
- Energy eigenspace
- Energy eigenstate
- Energy populations and evolving relative phases
- Equality case of the Heisenberg uncertainty relation
- Exact variational solution in a two-level system
- Expectation value
- Fidelity of quantum states
- Finiteness of the projective Clifford group
- Free-particle momentum convention
- GHZ-assisted quantum teleportation
- Global phase
- Ground-state degeneracy
- Ground-state energy
- Hadamard-conjugated linear oracle
- Hadamard interchange of Y eigenstates
- Half revival in an infinite square well
- Heisenberg coupling matrix for two spins
- Helical minimum of a complex Landau functional
- Heralded Pauli X correction using controlled-Z and measurements
- Liquid-state NMR quantum computing
- Local complementation of a graph state
- Molecular orbital
- Nonadaptive Clifford measurement pattern
- Operator-norm distance between unitary gates
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- Pauli-frame propagation along a measurement wire
- Pauli-string phase by parity computation
- Pauli Y eigenstate
- Perfect quantum state transfer
- Phase oracle
- Probability amplitude
- Projective measurement
- Projector phase rotation
- Pure state
- Pure-state norm distance
- Pure-state realization of a basis measurement distribution
- Quadratic Boolean phase cancellation
- Quantum measurement
- Quantum phase
- Quantum state
- Quantum state continuity at a finite Hamiltonian step
- Quantum state ray
- Quantum system
- Quantum theory
- Qubit precession under a constant Hamiltonian
- Qubit state
- Relative quantum phase
- Relativistic matter-wave velocities
- Repeated projective-measurement survival probability
- Rigid translation from a momentum term in the Hamiltonian
- Rotation about the x-axis
- Single-qubit process tomography
- Stationary state
- Three-qubit bit-flip syndrome table
- Three-vertex graph-state wire
- Time-independent Schrödinger equation
- Trace-overlap gate fidelity
- Two-bit remote state preparation on a graph-state path
- Two-qubit diffusion circuit
- Two-qubit parity phase gate
- Universality transfer by exact gate synthesis
- Vector normalization
- Wave function
- Wavefunction normalization
- Weight of a Pauli operator
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