“…Historically, the efforts aimed at improving the efficiency of vacuum neutron tubes with arc ion sources (increasing neutron yield, enhancing stability, and lengthening lifetime) were mainly focused on optimizing the source design and electrical circuit and on increasing the efficiency of hydrogen isotope extraction from the arc plasma (see, e.g. [6][7][8][9] and other publications). At the same time, the processes occurring directly in a vacuum-arc ion source remained poorly understood.…”
A model is proposed to describe the desorption of deuterium from a deuterated cathode during the operation of the vacuum arc cathode spot. The model treats a cathode spot as consisting of individual cells and involves a numerical simulation of the temperature fields that arise during the hydrodynamic processes responsible for the formation of microcraters on the cathode surface. Using a deuterated ZrD 0.67 cathode as an example, it is shown that the amount of deuterium desorbed immediately from the crater formed during the operation of the cathode spot cells is several times smaller than the total amount of desorbed deuterium. The main portion of deuterium is desorbed from the hot cathode region adjacent to the crater and from the crater at the stage of its cooling. For a deuterated ZrD 0.67 cathode, the percentage of desorbed deuterium can reach 80% of the total number of evaporated atoms, and it can be even greater if the cathode spot cells operate in the immediate vicinity of each other.
“…Historically, the efforts aimed at improving the efficiency of vacuum neutron tubes with arc ion sources (increasing neutron yield, enhancing stability, and lengthening lifetime) were mainly focused on optimizing the source design and electrical circuit and on increasing the efficiency of hydrogen isotope extraction from the arc plasma (see, e.g. [6][7][8][9] and other publications). At the same time, the processes occurring directly in a vacuum-arc ion source remained poorly understood.…”
A model is proposed to describe the desorption of deuterium from a deuterated cathode during the operation of the vacuum arc cathode spot. The model treats a cathode spot as consisting of individual cells and involves a numerical simulation of the temperature fields that arise during the hydrodynamic processes responsible for the formation of microcraters on the cathode surface. Using a deuterated ZrD 0.67 cathode as an example, it is shown that the amount of deuterium desorbed immediately from the crater formed during the operation of the cathode spot cells is several times smaller than the total amount of desorbed deuterium. The main portion of deuterium is desorbed from the hot cathode region adjacent to the crater and from the crater at the stage of its cooling. For a deuterated ZrD 0.67 cathode, the percentage of desorbed deuterium can reach 80% of the total number of evaporated atoms, and it can be even greater if the cathode spot cells operate in the immediate vicinity of each other.
“…These reactions are exothermic and can occur at arbitrarily low deuteron energies. In comparison with the generation of neutron pulses with a duration of 1 − 100 ns [6] using small-sized vacuum accelerator tubes, where it is possible at (D-T reaction, 300 kV) the neutron yield is 2 · 10 7 n/imp, the synthesis generator creates accelerated beams of lithium, deuterium and tritium ions, and then the formation of a dense ion or plasma target and a dense incoming flow allows the formation of neutron pulses from units of seconds to milliseconds from 2 · 10 10 to 2 · 10 14 n/imp. The generation of the dense flow of protons, deuterium or tritium atoms for the neutrons synthesis on the ion-plasma target of deuterium, tritium or lithium occurs as the result of primary flow compaction and discretization by software-defined concentration and average energy of the flow.…”
We develop the description of a neutron generator construction for the synthesis of light nuclei. The design of the neutron generator with plasma target is given together with a description of the types of nuclear reactions that are implemented in it. The brief theoretical description of the ion multiphase flow in the synthesis generator is considered.
“…A partial diode locking by a space charge already occurs at the current of ~10 А and a pulse duration of tens of nanoseconds. Besides, the neutron yield and neutron pulse duration are considerably reduced with the growth of emission current from the cathode [6].…”
Section: Experimental Determination Of the Optimal Parameters Of Lasementioning
The current density of 20 A/cm 2 is reached in pulses with duration of less than 0.5 µs at a repetition rate of 1 Hz. The accelerator applies the magnetic electron insulation technique in the accelerating gap. In addition, an intense laser-plasma ion source is used. The diode features and operation modes are considered using the conical geometry of a spiral line forming the magnetic field.
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