Critical unstable qubits exhibit indefinite anharmonic oscillations and coherence-decoherence cycles in a co-decaying frame, with first-time explicit geometric constructions for pure and mixed state trajectories on the Bloch sphere.
Rembieli´ nski and P
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A quasilinear evolution equation is introduced to replace von Neumann projection in selective quantum measurements, preserving ensemble equivalence and no-signaling without invoking apparatus states.
A quasilinear continuous evolution is introduced that reproduces the final states of von Neumann rank-one projective measurement while preserving no-signaling and ensemble equivalence.
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Trajectories of Critical Unstable Qubits in and on the Bloch Sphere
Critical unstable qubits exhibit indefinite anharmonic oscillations and coherence-decoherence cycles in a co-decaying frame, with first-time explicit geometric constructions for pure and mixed state trajectories on the Bloch sphere.
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Quasilinear evolution versus von Neumann selective measurement
A quasilinear evolution equation is introduced to replace von Neumann projection in selective quantum measurements, preserving ensemble equivalence and no-signaling without invoking apparatus states.
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Quantum selective measurement as a quasilinear evolution
A quasilinear continuous evolution is introduced that reproduces the final states of von Neumann rank-one projective measurement while preserving no-signaling and ensemble equivalence.