SOLVED: Resonance, the evolution operator U(t) in the rotating frame given by 5.5.6 The rotating-wave approximation in NMR Instead of the rotating field of (5.22), We shall use field B(t) parallel to: iw I(0,cos δ, sin δ) exp U(t) = exp B(t) = 2B cos(ωt + φ) rotation operator of angle about an axis of components We define the state vector |F(t)) in the rotating frame with angular velocity IWu[ Ie(θ) I(θ) sin θ n=0 Iz(θ) Ie(θ) = 0 Thus the angle θ allows one to choose the rotation axis.
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SOLVED: Resonance, the evolution operator U(t) in the rotating frame given by 5.5.6 The rotating-wave approximation in NMR Instead of the rotating field of (5.22),
SOLVED: Resonance, the evolution operator U(t) in the rotating frame ...
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