Abstract: A system and method of enhancing implosion characteristics of an Inertial Confinement Fusion (ICF) target by tailoring the shell such that at the appropriate temperature, the shell allows the energy in the central region to escape. These ICF targets are more efficient than conventional targets in that they utilize the high-Z shell to contain radiation losses from the fusion fuel core. In some embodiments, the shell is designed such that at the appropriate temperature, the shell allows the core radiation to escape. As a result, there is less energy lost. Therefore, the temperature rise in the core is enhanced which aides in the ignition and burn efficiency of the fusion fuel. Further, the ICF targets as described have substantially reduced computational requirements for design and analysis making them more desirable than conventional ICF targets.

Abstract: Inertial Confinement Fusion (ICF) reactor chambers can be designed to contain an ICF target being imploded and capture the resulting energy output from the reaction. The exact amount of energy required to facilitate this implosion depends on the specific target design in use. An ICF target design and implosion mechanism which is more robust against non-uniformities, simpler to analyze and simpler to utilize would be advantageous in achieving practical energy generation. Ideally, the ICF target will be configured to achieve a uniform temperature and density profile when imploding with a variety of parameters not limited to the following: a central region having an areal density (?r) less than 1 g/cm2 at ignition and approximately 1% of the entire mass to be a material having a Z between 6 and 47 inclusive.

Abstract: A confinement chamber for Inertial Confinement Fusion (ICF) may include a closed hohlraum and ICF target wherein the ICF target may comprise a central spherical fuel region, inner shell, outer fuel region, outer shell, and propellant region. A multitude of cylindrical beam channels may penetrate the entire thickness of the hohlraum. At the end of each cylindrical beam channel, where they exit the hohlraum, is a hemispherical cavity. Centered in the curvature of each cavity, and coaxial with each beam channel is a gold foam radiator. By layering materials or grading the density of a material in the propellant region of the closed hohlraum ICF target, the pressure profile on the outer shell may be tailored.

Abstract: A compact, simpler, more economical ICF target chamber and reactor design that maintains a low internal pressure, sub-atmospheric, and very small neutron flux on any pressure bearing vessel or steam generating mechanism. The present invention reduces radiant target emission towards the nearest wall of the hohlraum wall and/or sleeve material so that the radiation from target burn exits the end of the hohlraum through a wall material sufficiently thick to contain the target drive radiation, but becomes transparent to the target emitted radiation. The compact converter contains the energy released by the ICF target and converts it into usable heat to create steam. It also converts the excess neutrons, from the ICF target, into tritium. This is then collected with the unburnt fuel tritium.

Abstract: A compact, simpler, more economical ICF target chamber and reactor design that maintains a low internal pressure, sub-atmospheric, and very small neutron flux on any pressure bearing vessel or steam generating mechanism. The present invention reduces radiant target emission towards the nearest wall of the hohlraum wall and/or sleeve material so that the radiation from target burn exits the end of the hohlraum through a wall material sufficiently thick to contain the target drive radiation, but becomes transparent to the target emitted radiation. The compact converter contains the energy released by the ICF target and converts it into usable heat to create steam. It also converts the excess neutrons, from the ICF target, into tritium. This is then collected with the unburnt fuel tritium.

Abstract: A confinement chamber for Inertial Confinement Fusion (ICF) may include a closed hohlraum and ICF target wherein the ICF target may comprise a central spherical fuel region, inner shell, outer fuel region, outer shell, and propellant region. A multitude of cylindrical beam channels may penetrate the entire thickness of the hohlraum. At the end of each cylindrical beam channel, where they exit the hohlraum, is a hemispherical cavity. Centered in the curvature of each cavity, and coaxial with each beam channel is a gold foam radiator. By layering materials or grading the density of a material in the propellant region of the closed hohlraum ICF target, the pressure profile on the outer shell may be tailored.

Abstract: A set of optical elements for optical extraction composed of packed expanding optical cross sections to efficiently extract from a large gain region. The elements are rectangular shaped concave small expansion lenses matched to rectangular convex collimating lenses. Absorbing sheets divide an overall large volume up into smaller volumes to minimize losses due to amplified spontaneous emission. This arrangement has various applications, particularly in inertial confinement technology, where it may be used to extract energy from KrF laser media energized by electron beams. For certain applications, this regime of the gain medium may have zones at the absorbing sheets where this is no gain.

Abstract: Various configurations for ICF targets and techniques for their utilization are disclosed which may be simpler and more robust than conventional targets. In some embodiments, these targets may operate at a large areal density (?r), and/or may be imploded primarily by a single strong shock. In some embodiments, the entire volume of a region of fuel may be heated to a desired temperature at once, such that all the fuel mass may participate in the physical processes that may lead to fusion ignition. Targets of this type may be less sensitive to drive non-uniformity and to the temporal profile of driver energy delivery than conventional ICF targets.

Abstract: A system and method for integrating a direct compressor with a primary laser source and fast compressor while also reducing the number of mechanical elements and gas interfaces. A nonlinear scattering aperture combiner does not need to be optically multiplexed in order to drive a direct compressor stage, but by producing a large temporal compression ratio it will then pump the fast compressor. In order to accomplish this, a technique for transversely segmenting by color and/or polarization of the optical extraction beams of the direct compressor is utilized.

Abstract: An apparatus and process for pumping laser media by an optical pump over a 10 nanosecond period and thereafter time compressing the energy into an extraction pulse and focusing onto a target with a final 1 nanosecond irradiation time are disclosed. The exciting pump pulses are directed into a lookthrough compression arrangement wherein they energize a stimulated scattering process in low pressure (about 1 atmosphere) gaseous media and impinge in an off axis backward geometry. The extraction pulse is formed and directed towards the target with the appropriate information (color, phase, desired irradiance pattern) impressed on it at relatively low energy by manipulation with conventional, solid material optical elements. Once formed, it traverses the gaseous media, is amplified, and proceeds through a vacuum transition section and onto the target.

Abstract: A method of using an ICF chamber may include causing a target in the ICF chamber to emit x-ray radiation; receiving the x-ray radiation through a plurality of holes in a wall of the ICF chamber; and absorbing the x-ray radiation in a gas contained in a plurality of tubes that are coupled to the plurality of holes.

Abstract: In Inertial Confinement Fusion (ICF) targets that ignite a fuel section having a low areal density at ignition, the fuel section tends to have a very non-uniform temperature profile. As the areal density decreases, the temperature profile becomes less uniform. This leads to non-equilibrium ignition and a non-uniform density profile. However, there is an optimal material and content for the fuel region for any given target design. One can smooth both the temperature and density profiles in the fuel of non-equilibrium ignition targets while still allowing runaway burn but preventing margin parameters such as fall-line from being affected greatly.

Abstract: In a system and method for favorably affecting the Rayleigh-Taylor growth on the interface between the fuel and shell regions of an ICF target. One may increase the ratio of the tritium content to the deuterium content of the fuel or decrease the ratio of the density of the shell to the density of the fuel region. By proper configuration of the ratio between the fuel and shell regions, the Rayleigh-Taylor growth may become more stabilized. This invention would make target manufacturing much simpler and less constrictive, which would in turn decrease the cost.

Abstract: A target assembly for Inertial Confinement Fusion (ICF) achieving a high yield energy output. This high gain target has a low Z fuel/shell region which is lined with a thin layer of a high Z material on the inner surface and then surrounds a low density hotspot region. Adding a thin high Z liner to the inside of the low Z fuel shell has many advantages. As the shell region compresses and heats the central low density hotspot region, the radiation will be contained, and unable to leave the core. This will lower the ignition temperature of target considerably (around a factor of 4). A high Z shell liner may also increase the burn fraction of the fuel as well as increase the areal density (?r) of the hotspot.

Abstract: A method of imploding an Inertial Confinement Fusion (ICF) target may include directing laser energy into a hohlraum, where a target is disposed within the hohlraum that includes an ablator layer, a shell disposed within the ablator layer, and a fuel region disposed within the shell. The method may also include ablating the ablator layer in response to the laser energy being directed into the hohlraum, and generating a single shockwave that is driven inward through the ablator layer. The method may further include impulsively accelerating the shell inward when hit by the single shockwave, and compressing the fuel region by the inward acceleration of the shell.

Abstract: A method of imploding an Inertial Confinement Fusion (ICF) target may include directing laser energy into a hohlraum, where a target is disposed within the hohlraum that includes an ablator layer, a shell disposed within the ablator layer, and a fuel region disposed within the shell. The method may also include ablating the ablator layer in response to the laser energy being directed into the hohlraum, and generating a single shockwave that is driven inward through the ablator layer. The method may further include impulsively accelerating the shell inward when hit by the single shockwave, and compressing the fuel region by the inward acceleration of the shell.

Abstract: A set of optical elements for optical extraction composed of packed expanding optical cross sections to efficiently extract from a large gain region. The elements are rectangular shaped concave small expansion lenses matched to rectangular convex collimating lenses. Absorbing sheets divide an overall large volume up into smaller volumes to minimize losses due to amplified spontaneous emission. This arrangement has various applications, particularly in inertial confinement technology, where it may be used to extract energy from KrF laser media energized by electron beams. For certain applications, this regime of the gain medium may have zones at the absorbing sheets where this is no gain.

Abstract: A system and method for driving an ICF target with a thermal wave comprising: a target assembly, located inside a hohlraum, comprising a drive region, shell region and central fuel region; wherein said hohlraum comprises one or more laser entrance apertures; wherein said one or more laser entrance apertures are sized according to the shape of said hohlraum and to prevent energy from escaping said hohlraum; a laser assembly to irradiate a laser pulse through said laser entrance apertures; inner walls of said hohlraum to reradiate said laser pulse as x-ray radiation; wherein said x-ray radiation penetrates the target assembly as a thermal wave before any significant hydrodynamic motion occurs within said target assembly during the time in which the laser assembly is active; wherein said drive region is evenly heated to a sufficient temperature to expand in an inward and outward direction; and wherein said shell region is launched into said fuel region to drive said ICF target.

Abstract: A method of imploding an Inertial Confinement Fusion (ICF) target may include directing laser energy into a hohlraum, where a target is disposed within the hohlraum that includes an ablator layer, a shell disposed within the ablator layer, and a fuel region disposed within the shell. The method may also include ablating the ablator layer in response to the laser energy being directed into the hohlraum, and generating a single shockwave that is driven inward through the ablator layer. The method may further include impulsively accelerating the shell inward when hit by the single shockwave, and compressing the fuel region by the inward acceleration of the shell.

Abstract: In a system and method for utilizing a non-fissile fissionable shell material in a target assembly for Inertial Confinement Fusion (ICF). In one embodiment, the target assembly comprises a central region and a first shell surrounding said central region, wherein said central region receives a fusion fuel mixture and said first shell is a non-fissile fissionable material having a Z greater than 48. By proper configuration of the high-Z shell's fissionable properties, and the timing, the 14 MeV neutrons provide sufficient energy deposition into the shell that it expands at the requisite rate during the implosion, you can get an intrinsically stable implosion.