To attain efficiencies of over 10% obviously requires elimination of the electron beam losses in the vacuum diode.
Based on the results, pulsed diode lasers at optimal wavelengths can be chosen for clinically adapted equipment.
The diode impedance dependence of the generation frequency was weak and the microwave efficiency remained stable over a wide range of electron beam powers.
The motion is monitored now by a laser beam, which is reflected onto a split diode from the cantilever holding the sensor tip.
We could obtain the same experimental results at the field-emission diode using the explosive-drive flux compression device.
This quantity is conserved on the path of fluid element 1 on its way through the diode, and is therefore a 'stream function'.
The zero electric field regulates injection of electrons abundantly available at the cathode surface, essentially controlling the diode current.
The electron beam was produced by discharge of the secondary capacitor on a fieldemission diode.
