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Clear fused quartz (CFQ) may be considered a suitable material for electron and gamma dose measurements using electron spin resonance (ESR) technique.
It can be done by mapping the nanoresonator frequencies in the array, which could be compiled either before or after the measurements using electron beam imaging (to determine with high precision the nanoresonators' geometries) and finite element simulations.
Measurements using electron energy-loss spectroscopy show that the energy of the bulk low-loss plasmon in the nanoshells is significantly higher than that of amorphous carbon, lying just below that for annealed graphite.
Measurements using electron paramagnetic resonance (EPR) with spin-labels report on lifetimes of motional states that are in the range of ∼0.1 100 ns, times characteristic of backbone and side chain fluctuations of proteins in solution.
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This assumption is tested by a direct orientation measurement using Electron Back Scattering Patterns (EBSP).
In the present approach this is achieved, by a combination of crystal orientation measurement using electron backscatter diffraction (EBSD) and simulation of electron channelling patterns.
AB-P1 fraction was subjected to thin layer chromatography (TLC) and a phytoandrogenic triterpenoid fraction TLC4-5 was recovered for molecular mass measurement using electron spray ionization-mass spectroscopy (ESI-MS).
Parks and co-workers [21] showed that for Ag nanoparticles of 55 atoms in size, the ideal Mackay icosahedron is the most energetically preferred structure; these measurements were made using electron diffraction in situ over Ag55+/− ionized clusters selected by mass.
The measurements obtained using β-rays are verified to be consistent with the measurements using an electron beam.
Additional measurements using scanning electron microscopy and differential scanning calorimetry were carried out to obtain information for possible performance explanations.
Thin samples of uranium carbide were prepared for thermal conductivity measurements using an electron beam to heat the sample and an optical pyrometer to observe the thermal radiation.
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