Nuclear product ratio for glow discharge in deuterium

Abstract

New results for glow discharge in deuterium calorimetry are presented. In separate experiments a heat output five times exceeding the input electric power was observed. The result for the charged particle spectrum measurement is presented. Charged particles with energies up to 18 MeV and an average energy of 2-4 MeV were seen. Beams of gamma-rays with energies of about 200 keV and a characteristic X-ray radiation were registered. The summed energy of the registered products is three orders short of the values needed to explain the calorimetric results.

Intensification of Low Energy Nuclear Reactions Using Superwave Excitation

“…A review of the different approaches tried for attainment of cold fusion and of the experiments performed can be found in many publications such as references [2,3]. Among the approaches proposed and tried, in addition to electrolytic cells, [1] are glow-discharge cells [4], catalysis cells [5], electrolysis in high-pressure high-temperature cells [6] and ultrasonic excitation cells [7]. The experimental setups of ET have a number of novel features and the use of superwaves is a novel mode of operation.…”

Triple Deuterium Fusion by Three Body Recombination Between Deuteron and the Nuclei of Lattice Trapped Deuterium Molecules

“…Also the often repeated statement that the effect occurs after a long lag, goes through an optimum, and then disappears again 14,15,16 , gets a natural explanation with the hypothesis. The efimov effect has been much discussed in recent years 8,9,10 .…”

“…Also Karabut 16 -Claytor 19 -Romodanov type glow discharge experiments in deuterium gas with suitable electrodes of silicon or refractory metal carbides or nitrides could be done. These experiments should involve efficient detection of tritium and helium-4 and investigation of the electrodes for radioactive isotopes.…”

Solid state modified nuclear processes

“…(b) Fusionable nuclei, e.g. a fraction of deuterons, introduced with electrolysis [3], by an accelerator [2] or from a gas discharge [25] must move quasi-freely (sometimes after some scatterings or deceleration) with kinetic energy E near to the appropriate value E ∼ ω O , i.e. the distribution and change of E should also be under good control.…”