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Figure 4
Computed echo oscillations (intensity coded) as function of wavelength (λ in °) and coding asymmetry δ in T m. At the true symmetry point δ = 0 the intensity modulation phase does not depend on λ. |
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Figure 4
Computed echo oscillations (intensity coded) as function of wavelength (λ in °) and coding asymmetry δ in T m. At the true symmetry point δ = 0 the intensity modulation phase does not depend on λ. |