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Dynamic light scattering (DLS) at a detection angle of 90° relative to the incident beam detected hydrodynamic radii between 10 and 100 μm in samples of mature fibrils.
The detection angle of the detector was 35°.
It shifts toward shorter wavelengths with the increase of detection angle (Figure 9).
DLS measurements were performed at 25°C with a detection angle of 90°.
The group counted outgoing protons while varying both the detection angle and photon energy, and they found hallmarks of quarks.
The spectral shape and intensity of defect-related fluorescence can be controlled by variation of detection angle.
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The Ga 3d core-level spectra for S1 S3 at different photoelectron detection angles are depicted in Fig. 1a c, respectively.
One major advantage is that the optimum detection angles can be decided after the image scan, not before as required with scintillator detectors.
Table 1 summarizes the BEs of Ga 3d and Al 2p at different detection angles for all the samples, with the error of ± 0.1 eV.
It is demonstrated that the self-fluorescence of silica material can be enhanced at certain detection angles, near the spectral edges of the photonic stop zone.
The spectral position of photonic dip in the fluorescence can be described well with Equation 1. Figure 9 Fluorescence spectra of sample 2 measured at different detection angles.
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