Effect of magnetic beach on rf power absorption in ion cyclotron resonance
Effect of magnetic beach on RF power absorption in ion cyclotron resonance
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Effect of magnetic beach on RF power absorption in ion cyclotron resonance
Plasma acceleration by microwaves near electron cyclotron resonance without collisions, comparing theory and experiment
Pulsed grid modulation for ion cyclotron resonance spectrometer
Large signal saturation effects in cyclotron resonance oscillators, using helical electron beam-cavity interaction model
RF propagation and absorption calorimetric measurements in magnetoplasma near electron cyclotron resonance, noting power conversion
Ion mass spectrometry of D layer, using magnetic fields and cyclotron resonance principle
A new detector using an extremelly driven tuned circuit has been developed for use in ion cyclotron resonance spectroscopy experiments. Based on the Q-meter circuit, this detector will operate at frequencies greater than 1 MHz at rf levels less than 1 mV. Operation in the frequency range 1-15 MHz allows the use of higher magnetic fields for more efficient storage of low mass ions in the trapping mode of operation. In the frequency range 2-6 MHz electrons can be detected in the ion cyclotron resonance cell by their resonant motion in the trapping plane.
Flame analysis - ionization in cyanogen flames at reduced pressures by the cyclotron resonance method
Acetonitrile ion-molecule chemistry using ion cyclotron resonance, discussing reaction of vibrationally excited methyl ions from electron impact
Ion cyclotron resonance spectroscopy technique for determining electrons photodetachment energy from negative ions in gas phase
Electron cyclotron resonance (ECR) microwave plasma CVD has been developed at low pressures (0.0001 - 0.01 torr) and at ambient and high substrate temperatures (up to 750 C), to achieve large-area (greater than 4 in. diameter) depositions of diamondlike amorphous carbon (a - C:H) films. The application of a RF bias to the substrate stage, which induces a negative self-bias voltage, is found to play a critical role in determining carbon bonding configurations and in modifying the film morphology. There are two distinct types of ECR-deposited diamondlike films. One type of diamondlike film exhibits a Raman spectrum consisting of broad and overlapping, graphitic D (1360/cm, line width = 280/cm) and G (1590/cm, line width 140/cm) lines, and the other type has a broad Raman peak centered at appoximately 1500/cm. Examination of plasma species by optical emission spectroscopy shows no correlation between the CH-asterisk emission intensity and the deposition rate of diamondklike films.
Two distribution functions in the investigation of electron conductivity in a plasma at cyclotron resonance
The production of energetic ions with conical pitch angle distributions along the auroral field lines is a subject of considerable current interest. There are several theoretical treatments showing the acceleration (heating) of the ions by ion cyclotron waves. The quasi-linear theory predicts no acceleration when the ions are nonresonant. In the present investigation, it is demonstrated that the cyclotron resonances are not crucial for the transverse acceleration of ions by ion cyclotron waves. It is found that transverse energization of ionospheric ions, such as He(+), He(++), O(++), and O(+), is possible by an Electrostatic Hydrogen Cyclotron (EHC) wave even in the absence of cyclotron resonance. The mechanism of acceleration is the nonresonant stochastic heating. However, when there are resonant ions both the total energy gain and the number of accelerated ions increase with increasing parallel wave number.
Interaction of energetic electrons with bounded electromagnetic waves near cyclotron resonance, noting plasma diagnostics, maser and gain mechanism
Spatial waveform of azimuthal electric field of Faraday shielded Stix coils for ion cyclotron resonance heating of plasma to thermonuclear temperatures
Small signal and saturation characteristics for X band cyclotron resonance oscillator, discussing device design and configuration
Ion-molecule reaction rate constants measurement by ion cyclotron resonance, assuming no ion and neutral gas molecules collisions
Ion-molecule reactions produced in phosphine by ion cyclotron resonance