Author Affiliations
1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China2University of Chinese Academy of Sciences, Beijing 100039, China3Department of Physics, Shanghai Normal University, Shanghai 200234, Chinashow less
Fig. 1. (a) Reflected field and (b) spectrum of a pulse with A=2π, τp=5 fs incident on a periodic structure with δ=λ0/2, L=45 μm and ωc=0.05 fs−1. The dashed and dotted lines correspond to the leading and tail parts of the reflected fields, respectively.
Fig. 2. (a) Time evolution of Ω(t) and u(t) in a resonance medium with ωp=ω0. (b) The changing curves of χ′, χ′′, and n versus Δ in the case of (a). (c) Same as that for (b), but for a detuning medium with ωp=2ω0. (d) The reflected spectrum under the same parameters as (c). The other parameters are same as those in Fig. 1.
Fig. 3. A=2π, τp=5 fs, L=45 μm, ωc=0.05 fs−1. The reflected spectra of the periodic structures with δ=kλ0(k=2,1,1/4).
Fig. 4. (a)–(e) The reflected spectra of the periodic structures with δ=kλ0(k=2,1,1/2,1/4,1/8). A=4π, ωc=0.2 fs−1, L=150 μm. The other parameters are same as Fig. 3. The dashed line in (a) indicates the reflected spectrum of a bulk medium. (f) The scaling law of the frequency intervals of the spectral spikes against k.
Fig. 5. Comparison of the reflected spectra of ωc=0.01 fs−1 (solid line) and ωc=0.05 fs−1 (dashed line).