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AFM image of recorded grating is shown in Fig. 8.
PL participated in the study of magnetic properties of recorded grating surface relief.
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Diffraction efficiency of recorded gratings was ~7% in transmission on 650 nm wavelength, absolute values.
The spatial frequency of grooves in the recorded grating is 740 mm−1, and the profile depth is 200 nm.
Fig. 7 Scheme of diffraction grating recording: DPSS laser; SF and L collimator; BS beam splitter; M flat mirrors; S registering media (sample); LD LED; PD registering unit Fig. 8 AFM image of recorded holographic grating using As2S3 Mn Se nanomultilayers.
Close examination of recorded looping (stationary black/white grating; Movie S1) revealed that each occurrence of looping was preceded by several instances of CN, and that the slow phase of CN and subsequent looping had the same direction (Figure 3A and 3B).
One can see that the relaxation process of the recording grating is almost the same as the pumping pulse that proves the dynamical nature of the grating.
Dependence of holographic grating recording on polarization of recording beams when using nanomultilayer structures on the base of chalcogenide glasses was also observed for other compositions of nanomultilayer structures [25, 27].
Successive recordings partially erase the previous recorded holographic gratings; therefore, the recording-erasure dynamics of the fiber hologram is evaluated.
Further investigations are necessary for the optimization of multilayer nanostructure parameters and conditions of grating recording.
AFM image and profile of a diffraction grating recorded in Ge25Se75 layer by using the method of interference lithography with photoinduced etching and the profile of its grooves.
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