Beyond-rotating-wave corrections accumulate across long composite Ramsey pulse trains, hiding the small tensor shift that the sequence was designed to measure.
Ω rf τ / 2 = π/ 2) has phase φ in = 0, while the fi- nal π/ 2-pulse has a phase φ fin
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Theory of composite Ramsey sequences of radiofrequency pulses beyond the rotating wave approximation
Beyond-rotating-wave corrections accumulate across long composite Ramsey pulse trains, hiding the small tensor shift that the sequence was designed to measure.