Figure 1

Intensities of the forward- and deflected-diffracted beams (upper) and the interior solutions $\alpha ,\beta$ (lower) as a function of depth inside a thick crystal. A lattice disturbance near the exit couples the two solutions, regenerating $\beta$.Reuse & Permissions

Figure 2

Experimental setup.Reuse & Permissions

Figure 3

Time-resolved anomalous transmission. (a) Experiment: Deflected-diffracted intensity for an incident laser fluence of 35 (solid line), 7 (dashed line), and $2\mathrm{m}\mathrm{J}/{\mathrm{c}\mathrm{m}}^2$ (dot-dashed line). The error bar represents the estimated systematic error in the overall scale. Inset: Streak camera data showing the intensity of the forward-diffracted beam with picosecond resolution at an incident optical fluence of $35\mathrm{m}\mathrm{J}/{\mathrm{c}\mathrm{m}}^2$. (b) Simulation: Deflected-diffracted intensity for an incident laser fluence of 36 (solid line), 8 (dashed line), and $2\mathrm{m}\mathrm{J}/{\mathrm{c}\mathrm{m}}^2$ (dot-dashed line).Reuse & Permissions

Figure 4

(a) Experiment: The relative phase of the Pendellösung oscillations (squares) and the normalized deflected-diffracted intensity at a time delay of 200 ps (circles) as a function of incident optical fluence. (b) Simulation: The calculated relative phase of the Pendellösung oscillations (squares) and the calculated normalized deflected-diffracted intensity at a time delay of 200 ps (circles) as a function of incident optical fluence.Reuse & Permissions