Cyclotron and bounce resonance scattering of electrons trapped in the earth's magnetic field
Cyclotron and bounce resonance scattering of electrons trapped in earth magnetic field
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Cyclotron and bounce resonance scattering of electrons trapped in earth magnetic field
Comparison of Alouette-2 and OGO-5 observation of turbulence of magnetospheric electrostatic electron cyclotron harmonic waves
Electron-cyclotron wave resonance in inductively coupled HF ring discharges
Low and high linear energy transfer /LET/ cyclotron-accelerated alpha particles effects on Drosophila melanogaster longevity
Ion-molecule collision charge transfer and momentum transfer relaxation rates, using ion cyclotron resonance heterodyning method
Ion cyclotron resonance application to propanol ion structure formed in double McLafferty rearrangement, demonstrating direct enol ion formation instead of by isomerization or ketonization
Gas phase ion-molecule phosphine reactions in pure and binary mixtures by ion cyclotron resonance spectroscopy, considering acidity and basicity
Negative ions photodetachment by continuously tunable laser and ion cyclotron resonance spectrometer
Large signal saturation effects in cyclotron resonance oscillators, using helical electron beam-cavity interaction model
Ion cyclotron resonance power absorption theory application to reactive and nonreactive ions line shapes, using Wobschall-Graham-Malone phenomenological equation of motion
Ion cyclotron resonance spectroscopy, discussing fundamentals, instrumentation and ion-molecule chemistry applications
Ion cyclotron resonance power absorption, deriving expression for average ion kinetic energy at saturation in steady state limit
Magnetic drift waves near proton cyclotron frequency, noting magnetic field gradient role in plasma instability
The reactions studied which produce I-123 directly were Sb-121(He-4,2n) I-123, Sb-121(He-3,n) I-123, Te-122(d,n) I-123, Te-122(He-4,p2n) I-123, Te-122(He-3,pn) I-123, and Te-123(He-3,p2n) I-123. Reactions which produce I-123 indirectly through the positron decay of 2.1-hour Xe-123 were Te-122(He-4,3n) Xe-123, Te-122(He-3,2n) Xe-123 and Te-123(He-3,3n) Xe-123. Use of the gas flow I-123 cyclotron target assembly is recommended for the production of I-123 with radiochemical purity greater than 99.995%.
The use of the various nuclear reactions is described by which I-123,a low radiation dose radiopharmaceutical, can be cyclotron-produced. Methods of directly producing I-123 and those which indirectly produce the radionuclide through the beta (+) decay of its nautral precursor, Xe-123. It is impossible to separate from the radioiodine contaminants, notably I-124, which occur in the direct method. Thus, it is preferable to produce pure I-123 from Xe-123 which is easily separated from the radioiodines. Among the characteristics of I-123 is the capability of reducing the patient dose in a thyroid uptake measurement to a very small percentage of that delivered by the more commonly used I-131.
An experimental study has been made of an ion-cyclotron-wave apparatus operated in the RF-sustained mode. This is a mode in which the Stix RF coil both propagates the waves and maintains the plasma. Problems associated with this method of operation are presented. Some factors that are important to the coupling of RF power are noted. In general, the wave-propagation and wave-damping data agree with theory. Some irregularities in wave fields are observed. Maximum ion temperature is 870 eV at a density of 5 times 10 to the 12th power per cubic centimeter and RF power of 90 kW. Coupling efficiency is 70 percent.
A theory of plasma beam cyclotron instability is developed on the basis of computer simulation experiments. The theory holds that at certain turbulence levels, electron cross-field diffusion which supresses the electron gyroresonances is created by turbulent wave-particle interactions in a plasma beam after a period of quasi-linear exponential development of turbulence. The stabilizing effect of Landau ion damping is noted. The behavior of cold and hot ions is discussed.
It is argued that the cyclotron drift instability (coupled ion waves and electron Bernstein modes) can explain many structural features of the weak electrostatic turbulence observed in bow shock magnetic-field gradients and thus that it provides a more attractive speculation than the ion acoustic or Buneman instabilities previously suggested as weak turbulence sources.