Space–time cloaks through birefringent Goos–Hänchen shifts

Fig. 2. Birefringent reflection and transmission versus $θ$ , such that $γ_{e, 1} = 1 γ$ , $γ_{b} = 0.02 γ$ , $Ω_{c} = 1.5 γ$ , $Δ_{p} = 0 γ$ , $φ_{1} = π / 2$ , $φ (φ_{2, c}) = 0$ , $x = 0.5$ .

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Fig. 3. Birefringent reflection and transmission versus $θ$ , such that $γ_{e, 1} = 1 γ$ , $γ_{b} = 0.02 γ$ , $θ = π / 3$ , $Δ_{p} = 0 γ$ , $φ_{1} = π / 2$ , $φ (φ_{2, c}) = 0$ , $x = 0.5$ .

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Fig. 4. Birefringence shifts in the reflection beam versus $θ$ , such that $γ_{e, 1} = 1 γ$ , $γ_{b} = 0.02 γ$ , $Ω_{c} = 1.5 γ$ , $Δ_{p} = 0 γ$ , $φ_{1} = π / 2$ , $φ (φ_{2, c}) = 0$ , $x = 0.5$ .

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Fig. 5. Birefringence GH shifts in the transmission beam versus $θ$ , such that $γ_{e, 1} = 1 γ$ , $γ_{b} = 0.02 γ$ , $θ = π / 3$ , $Δ_{p} = 0 γ$ , $φ_{1} = π / 2$ , $φ (φ_{2, c}) = 0$ , $x = 0.5$ .

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Fig. 6. Normalized input intensity versus $t / τ_{0}$ and $y / w$ , $τ_{0} = 1.5 μ s$ , $w = 30 λ_{p}$ .

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Fig. 7. Normalized transmission and reflection pulses intensities versus $t / τ_{0} a n d y / w$ , such that $γ_{e, 1} = 1 γ$ , $γ_{b} = 0.02 γ$ , $θ = π / 3$ , $Δ_{p} = 0 γ$ , $φ_{1} = π / 2$ , $φ (φ_{2, c}) = 0$ , $x = 0.5$ , $Ω_{c} = 1.5 γ$ , $τ_{0} = 1.5 μs$ , $w = 30 λ_{p}$ .