IEEE Transactions on Plasma Science · 2014 · 16 citations · 26 references
Natural SciencesNuclear EngineeringPhysicsNuclear PhysicsPlasma PhysicsRadiation PhysicsAlpha DecayNuclear DecayPlasma SimulationRadar Wave PropagationRadiation Transport In MatterRadioactive DecayElectromagnetic Wave Energy PropagationElectromagnetic Wave ScatteringElectron DensityElectron Density ProfilesFinite Difference Time Domain ModelingFinite Difference Time Domain SimulationRadioactivity MeasurementRadionuclide Decay Modeling
At the different radioactivity, temperature, pressure, heights, and incident angles, the influences of the electromagnetic wave propagating in the α-decay radionuclide layer (RNL) coated on a perfect electric conductor system were simulated by the finite-difference time-domain method. The maximum electron density ionized by 5.45-MeV α-particles is ~1.8 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">11</sup> per cubic centimeter when the radioactivity is 10 Ci/cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> . The decrease of the reflectivity at altitude is much better than at ground and the decreasing amplitudes could reach 1-20 dB in the frequency range from 300 MHz to 40 GHz at an altitude of 10000 m. In addition, the same RNL would significantly reduce the back scattering bistatic radar cross section (RCS) of the platform. The decrease of RCS along the direction of the originally strongest reflection wave is nearly 25.5 dB when the incident angle is 60°.
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The propagation of electromagnetic waves in plasmas
V. C. A. Ferraro · Planetary and Space Science · 1971 · 740 citations
Average energy required to produce an ion pair
W. H. Henry · Nuclear Instruments and Methods · 1980 · 106 citations