A fusible target is embedded in a high Z liner, ohmically heated and then shock wave heated by implosion of an enveloping high Z liner. The target is adiabatically heated by compression, fusibly ignited and charged-particle heated as it is being ignited. A shock front forms as the liner implodes which shock front detaches from the more slowly moving liner, collides with the outer surface of the target, accelerates inward, rapidly heating the target, adiabatically compressing the target and liner and amplifying the current to converge the liner mass toward a central axis thereby compressing the target to a fusion condition when it begins to ignite and produce charged particles. The charged particles are trapped in a large magnetic field surrounding the target. The energy of the charged particles is deposited into the target to further heat the target to produce an energy gain.

A fusible target is embedded in a high Z liner, ohmically heated and then shock wave heated by implosion of an enveloping high Z liner. The target is adiabatically heated by compression, fusibly ignited and charged-particle heated as it is being ignited. A shock front forms as the liner implodes which shock front detaches from the more slowly moving liner, collides with the outer surface of the target, accelerates inward, rapidly heating the target, adiabatically compressing the target and liner and amplifying the current to converge the liner mass toward a central axis thereby compressing the target to a fusion condition when it begins to ignite and produce charged particles. The charged particles are trapped in a large magnetic field surrounding the target. The energy of the charged particles is deposited into the target to further heat the target to produce an energy gain.

A well logging tool includes a neutron generator to generate and emit energetic neutrons using substantially exclusively a T-T fusion reaction. The well logging tool can include measuring instrumentation for measurement and logging of formation parameters based on elastic scattering in subsurface formations of neutrons emitted by the neutron generator. The neutron generator can have a concentric layout, in which a cylindrical target structure loaded with tritium particles is located co-axially in an elongate cylindrical housing, with mobile tritium ions being accelerated radially inwardly into impact with the target structure. Production of the mobile tritium ions may be by field ionization through operation of a nano-structure field ionization array.

Embodiments that are directed to a target for producing a high epithermal neutron yield for boron-neutron capture therapy (BNCT) treatments are disclosed. The target includes a thin flat film of solid lithium mounted onto a heat-removal support structure that is cooled with a liquid coolant and configured to maintain the turbulent flow regime for a liquid coolant and distribute the flow of coolant directed at the center of the support structure toward a periphery of the support structure via a plurality of channels formed in the support structure. The support structure includes a nozzle located at its center to direct coolant flow outwardly from the center to avoid stagnant water flow at the center of the support structure. Systems, device, and methods utilizing the approaches are also described.

Embodiments that are directed to a target for producing a high epithermal neutron yield for boron-neutron capture therapy (BNCT) treatments are disclosed. The target includes a thin flat film of solid lithium mounted onto a heat-removal support structure that is cooled with a liquid coolant and configured to maintain the turbulent flow regime for a liquid coolant and distribute the flow of coolant directed at the center of the support structure toward a periphery of the support structure via a plurality of channels formed in the support structure. The support structure includes a nozzle located at its center to direct coolant flow outwardly from the center to avoid stagnant water flow at the center of the support structure. Systems, device, and methods utilizing the approaches are also described.

An inertial electrostatic confinement fusion device has a body defining an internal vacuum chamber cavity, the chamber having attached a pump to evacuate atmosphere to vacuum conditions, the chamber further having attached a source to inject a nuclear fusion fuel at a metered rate, the chamber further having within it a plurality of electrodes connected to a high voltage alternating current power supply such that at least one pair of electrodes consistently have electrical charge of opposite polarity and of equal magnitude, the distance between them defining an electrode gap. The assembly acts to control the specific relationship between the electrode gap and the applied power, both frequency and voltage, to excite ions of the nuclear fuel enough to generate fusion but alternate the electrode polarity sufficiently to prevent the ions from completely traversing the electrode gap, preventing electrode bombardment.

An inertial electrostatic confinement fusion device has a body defining an internal vacuum chamber cavity, the chamber having attached a pump to evacuate atmosphere to vacuum conditions, the chamber further having attached a source to inject a nuclear fusion fuel at a metered rate, the chamber further having within it a plurality of electrodes connected to a high voltage alternating current power supply such that at least one pair of electrodes consistently have electrical charge of opposite polarity and of equal magnitude, the distance between them defining an electrode gap. The assembly acts to control the specific relationship between the electrode gap and the applied power, both frequency and voltage, to excite ions of the nuclear fuel enough to generate fusion but alternate the electrode polarity sufficiently to prevent the ions from completely traversing the electrode gap, preventing electrode bombardment.

Provided herein are high energy ion beam generator systems and methods that provide low cost, high performance, robust, consistent, uniform, low gas consumption and high current/high-moderate voltage generation of neutrons and protons. Such systems and methods find use for the commercial-scale generation of neutrons and protons for a wide variety of research, medical, security, and industrial processes.

Provided herein are high energy ion beam generator systems and methods that provide low cost, high performance, robust, consistent, uniform, low gas consumption and high current/high-moderate voltage generation of neutrons and protons. Such systems and methods find use for the commercial-scale generation of neutrons and protons for a wide variety of research, medical, security, and industrial processes.

A continuous, thin layer of neutron source material, for example solid lithium, is formed into a belt. The belt is continuously advanced in front of a proton source to generate neutrons from the lithium target. Additionally, the belt is continuously cooled, as it passes through a gas cooling section. Through the continuous motion and cooling of the lithium target, the belt can provide an effective neutron source without melting the target neutron source material.