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An approach for characterizing the initial amplitude of a parasitic mode as well as its decay rate away from a grid resolution discontinuity is presented.
Slope/curvature limiting is insufficient to completely remove these modes, especially at low forcing frequencies where the incident wave can act as a carrier of the parasitic mode.
Parameters for the 3W1 source at BSRF were determined in both the dedicated and parasitic mode and their suitability for protein crystallography beamline at BSRF were realized.
Considering the problem of parasitic mode excitation in beam tunnel, a detail analysis is performed for the suppression of these kinds of modes.
This paper illustrates that it is possible, through piezoceramic stack position, to minimize modal coupling between a parasitic mode and the tuned longitudinal mode of vibration for slender ultrasonic devices.
The photon flux from the 3W1 source is about 2×1011 photon/s mA in the wavelength range of 2.0 0.9 Å in parasitic mode and 50 80 times higher in the dedicated mode.
Similar(44)
In addition, approximations developed prevent the appearance of various pathological (with, e.g., spurious, parasitic modes, etc).
Consequently, the solution mixes with parasitic modes which carry power out of the resonance zone.
Both the dedicated and parasitic modes are suitable for macromolecular structure experiments.
The excitation of parasitic modes is a concerning problem for high frequency, high power gyrotrons.
A general analysis of this traveling wave, multilayered, dielectric-loaded accelerating structure is presented including field solutions for both the TM (acceleration) modes and HEM (parasitic) modes.
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