Laser-differential-confocal-technology-based method and device for comprehensively measuring morphological performance parameters of nuclear fusion pellet
A differential confocal and fusion target technology, which is applied in the direction of measuring devices, optical devices, material excitation analysis, etc., can solve the problem of inability to apply process treatment or target shooting experiments, inconsistency of value reference, and non-destructive measurement of internal parameters of the target capsule and other problems, to achieve the effect of suppressing the difference in surface properties and the power drift of the system light source
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Embodiment 1
[0052] Such as image 3 As shown, in the comprehensive measurement method of laser differential confocal nuclear fusion target capsule morphology and performance parameters, the light source system 1 selects a point light source, and the excitation beam emitted by the point light source is collimated into a parallel beam through the collimator lens 2, and the parallel beam is separated by the beam splitter After A3 is reflected, it is reflected by the dichroic beam splitter 21 again to form a reflected illumination beam. The reflected illumination beam is converged into a point by the measurement objective lens 5 to illuminate the fusion target pellet 13. The illumination light is reflected by the fusion target pellet 13 and excited to generate a Raman spectrum. The Raman spectrum carrying the information of the fusion target 13 and the reflected beam pass through the measurement objective lens 5 to form a measurement beam. The Raman spectrum in the measurement beam passes thro...
Embodiment 2
[0066] Such as Figure 4As shown, the comprehensive measurement device for the shape and performance parameters of the laser differential confocal nuclear fusion target pellet includes the light source system 1, the beam splitter A3 placed along the light source exit direction, and the dichroic beam splitter placed along the reflection direction of the beam splitter A3 21. The measuring objective lens 5 is placed sequentially along the reflection direction of the dichroic beamsplitter 21, the differential confocal detection system 6 is located in the opposite direction of the reflection direction of the beamsplitter A3, and is placed in sequence in the opposite direction of the reflection direction of the dichroic beamsplitter 21. The spectrum converging lens 22 and the spectrum detection system 23 are located in the measurement objective lens 5 exit direction and the orthogonal drive system 14 whose rotation axis is coaxial with the measurement optical axis, the rotation drive...
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