Abstract: Method and apparatus are disclosed for producing and sustaining a very intense pinch effect in a ralativistic electron beam by applying a continually accelerating strong electric field along the entire length of the beam. A special anode collects electrons that stray from the beam and conducts them along a conducting wall of the anode. The potential drop due to the flow of these electrons in the anode wall produces a strong electric field along the beam. The clusters of heavy ions in the beam impact a target made of lead, for example, and produces various varieties of sub-nuclear products including mesons, neutrons, neutrinos, and hadrons. Electrons liberated from atoms appear adjacent the cathode along with ions also resulting from the liberation. These electrons are accelerated toward the target leaving behind the positive ions which produce a positive potential trough.

Abstract: An intense high current, high voltage pulsed beam comprising bursts of electrons of about 40 nanoseconds duration each, having a beam radius of about 1 mm is projected through an anode consisting of a hollow tube with much smaller diameter than that of the diode tube surrounding the cathode. By appropriate selection of combinations of materials, sizes, shapes, and surface treatments surrounding the beam in its travel through the anode, or by means such as ion beams directed back along the beam, or by laser pulses on selected areas inside the anode or on the cathode tip, or by controlling supply of appropriate gases or vapors through a small diameter tubular cathode, either metallic or dielectric, and separately into the tubular anode near the end farthest from the cathode and nearer the target, the beam is made to pinch down to a radius of about 0.

Abstract: An intense high current, high voltage pulsed beam comprising bursts of electrons of less than 200 nanoseconds duration each, having a beam radius of about 0.5 mm. is projected through an anode consisting of a hollow tube with much smaller diameter than that of the diode tube surrounding the cathode and with diameter diminishing with deeper penetration into the tubular anode. By appropriate selections of combinations of materials, sizes, shapes, and surface treatments surrounding the beam in its travel through the anode, or by means such as ion beams directed back along the beam, or by laser pulses on selected spots inside the anode or on the cathode tip, or by controlled supply of appropriate gases or vapors through a small diameter tubular cathode, either metallic or dielectric, and separately into the tubular anode near the end farthest from the cathode and nearer the target, the beam is made to pinch down to a radius of 0.1 mm.