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The discrepancies to the experiment results in this work can be mainly explained by the rather large energy degradation of the proton beam (using niobium), from the initial 72 MeV to ~10 15 MeV, resulting in a beam with a broad spread of energies at diminished intensities.
It is desirable to have a Stokes beam with a broad spectrum for fast spectrum generation.
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The study is carried out using three-dimensional finite element modeling of simply supported I-shaped cellular steel beams with a broad spectrum of cross-sectional dimensions, span lengths and web perforation configurations.
In this case, a beam pattern with a broader main lobe (as shown in the right side of Figure 5) to approximately encompass all the positions of the acoustic events has been designed.
The use of the dichroic mirror that collinearly adds the Stokes beam with the pump beam will give a broad, excitable tunable wave number (cm-1) range between 700 cm-1 and 3700 cm-1.
An electrostatic closed electron Hall drift thruster with a broad beam size was used as an ion source.
Alternatively, a relatively large area of sample may be illuminated simultaneously with a broad beam (a macroprobe), and the emission imaged onto a detector with lateral resolution, e.g. a pixelated detector such as a charge coupled device (CCD) [6,14-18], sometimes with energy resolution on each pixel [19,20].
However, a single-shot CARS spectrum can be achieved with a broad Stokes beam and a narrow pump beam.
A broad laser beam with a top-hat profile was used to carry out the laser microwelding work.
Cross-sections of the samples were embedded in epoxy, frozen to - 60°C and polished with a broad ion beam (BIB).
In fluorescence imaging, this is followed by illumination of the subject, usually with a broad light beam passing through a filter tuned to the excitation wavelength of the fluorophore of interest.
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