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GHZ witness evaluated as a function of the adiabatic computing step. The GHZ witness is negative for a pure state with a GHZ component, but it may be positive for a mixed state with a GHZ component. Dashed lines are added in this figure and following figures as guides for the eyes.

Journal: Entropy

Article Title: Entropy, Fidelity, and Entanglement During Digitized Adiabatic Quantum Computing to Form a Greenberger–Horne–Zeilinger (GHZ) State

doi: 10.3390/e27090891

Figure Lengend Snippet: GHZ witness evaluated as a function of the adiabatic computing step. The GHZ witness is negative for a pure state with a GHZ component, but it may be positive for a mixed state with a GHZ component. Dashed lines are added in this figure and following figures as guides for the eyes.

Article Snippet: We denote the trace of the product of the GHZ witness operator with the density matrix as the “GHZ witness” (as distinct from the GHZ witness operator).

Techniques:

GHZ witness evaluated as a function of the discretized adiabatic quantum computing step for the Python calculations and the quantum simulators Fake Perth, Fake Aachen, Fake Brisbane, and Fake Sherbrooke. The density matrices from Python calculations and from the simulators clearly incorporate a GHZ component, except for Fake Perth.

Journal: Entropy

Article Title: Entropy, Fidelity, and Entanglement During Digitized Adiabatic Quantum Computing to Form a Greenberger–Horne–Zeilinger (GHZ) State

doi: 10.3390/e27090891

Figure Lengend Snippet: GHZ witness evaluated as a function of the discretized adiabatic quantum computing step for the Python calculations and the quantum simulators Fake Perth, Fake Aachen, Fake Brisbane, and Fake Sherbrooke. The density matrices from Python calculations and from the simulators clearly incorporate a GHZ component, except for Fake Perth.

Article Snippet: We denote the trace of the product of the GHZ witness operator with the density matrix as the “GHZ witness” (as distinct from the GHZ witness operator).

Techniques: