Our design includes the world's largest laser, which will enable the potential to generate energy as demonstrated at the National Ignition Facility in 2022.
We are building on decades of investments in excimer gas laser systems for semiconductor lithography and defense, combined with fuel capsule and containment chamber concepts that have been waiting for a laser system to enable them.
By using a gas laser architecture, we can reduce laser cost per joule by a factor of over 30x compared to the NIF.
Lower cost enables a much higher-energy laser with under 1 square meter of final optical area.
Higher laser energy enables igniting larger capsules, which are easier to produce, more robust and produce higher gains.
Higher capsule gain enables lower repetition rates (< 1 Hz), simplifying engineering and reducing capsule fabrication costs.
Flowing liquid lithium salt protects the structural wall of the chamber from fusion neutrons, reducing maintenance and waste production.
These advantages together simplify the development roadmap and cost of a power plant, yielding the lowest-risk path with the best economics.
Fusion approaches can be generally classified by how long the fusion plasma is confined, and the method by which the fusion plasma is confined. Across approaches, confinement times range from 10s of picoseconds to several seconds, with plasma densities inversely correlated, ranging from 100s of grams per cc to billionths of a gram per cc. For the long confinement times and low densities, magnetic fields are used for plasma confinement, with the prototypical example being a tokamak. For the short confinement times and high densities, inertial confinement is used, with the prototypical example a laser to implode fuel capsules like on the NIF. There are several approaches in between at moderate confinement time and density, including using pulsed power to drive hybrid magnetic-inertial systems. At this time, the private sector is pursuing all of these differing approaches.
To date, only the laser inertial approach with DT fuel has achieved fusion ignition and scientific breakeven. There are also other advantages unique to Xcimer’s laser inertial approach, aside from having the most-proven science. First, the major elements of the system are maximally decoupled, with the laser able to stand off up to 50 meters away from the low-mass fuel capsule and enter the reactor chamber through only two very small openings. The fusion takes place in about a cubic centimeter in the center of the target chamber and is far removed from the “plasma facing first wall” of the chamber with no physical connection. This also enables the use of molten salt coolant flow to protect the chamber first structural wall from the fusion output. Second, inertial fusion at short confinement time and high density undergoes “burn propagation”, where ignition of only a small amount of fusion fuel in a target can release enough energy to ignite the rest of the fuel, like a match lighting a fire. This leads to high facility “wall-plug” gains even with a 5%-10% efficient laser.
These advantages among others give laser inertial fusion superior long-term economic prospects for fusion power production.
The Xcimer laser combines nonlinear "gas" optics with excimer laser amplifiers to produce very high beam energies at low cost. Excimer lasers have seen wide commercial application in semiconductor lithography, medical and industrial applications.
Like NIF, our fuel capsules are consumables containing hydrogen (DT) fuel that are ignited by the laser, but at much larger size and mass, resulting in higher performance, easier manufacturing, and more robust operation. The higher performance means a power plant can operate at lower repetition rates (< 1 Hz) than conventional IFE concepts.
Pioneered at Livermore National Lab and UC Berkeley over several decades, the chamber uses a self contained liquid flow of lithium salt, or FLiBe to absorb fusion output and completely protect the first structural wall.
The timeline presents pivotal milestones, tracing the journey of fusion energy from the early 20th century’s experiments and foundations, to the 2022 landmark of net energy gain at NIF. They mark key innovations, advancements and partnerships that led to the development of XCIMER’s IFE system.
In 1926 Arthur Eddington proposed that stars
produce energy from hydrogen fusion.
For over a century it was not known how the sun could maintain its temperature and energy output for the billions of years that geologists knew the earth had been in existence. In 1939, Hanz Bethe finally discovered the nuclear fusion cycle that powers the sun, which involves proton-proton fusion.
Los Alamos Laboratory
The idea of using fusion in a weapon dates back as early as the Manhattan project, and was developed primarily by Edward Teller and Stanislaw Ulam. Their concept was to use the x-ray energy produced by an atomic fission device to flow over to a physically separate fusion component and implode and ignite this separate component. This worked on the very first try in the Ivy Mike test of 1952, which yielded 10 megatons of energy. The fusion plasma was inertially confined and produced enormous fusion gain. The physical principle of high-gain inertial confinement fusion was conclusively demonstrated here.
Kurchatov Institute in Moscow
Experimental results from the first Tokamak, the T1, were submitted to the second Atoms for Peace conference in Geneva in 1958. A Tokamak confines a plasma in a toroidal geometry, and, along with the Stellarator, is the most-studied magnetic fusion concept to date.
Hughes Research Laboratory
Theodore Maiman operated the first laser on May 16th 1960 at Hughes Research Laboratory using flashlamps and a ruby rod. The initial paper was rejected by Physical Review Letters, but was subsequently published in Nature.
Lawrence Livermore National Laboratory
Shortly after the laser was invented, scientists realized a laser could be used to provide the temperatures and pressures needed to implode and ignite fusion fuel, without needing an atomic fission bomb. The major difference, however, was that the laser energy available was many orders of magnitude less than what could be provided by a fission bomb, and this led to many challenges.
Kurchatov Institute in Moscow
The Russians announced the achievement of 1 keV electron temperature in the T3 tokamak in 1968. This result was met with intense skepticism, but was confirmed the following year by a team of physicists from the UK who visited the machine and performed their own measurements.
Lawrence Livermore National Laboratory
Nuckolls’ seminal paper in the field of inertial fusion proposed using a laser pulse shaped precisely in time to implode DT fuel and achieve densities 10,000 times solid. It was estimated that if this could be achieved, then ignition could be achieved with only 1 kJ of laser energy. While this turned out to be impossible due to hydrodynamic instabilities and nonlinear laser plasma interaction issues, it began investigation into laser-driven inertial fusion in earnest.
Lawrence Livermore National Laboratory
The High Yield Lithium Injection Fusion Energy (HYLIFE) chamber was the first proposal put forward by Livermore for how to contain sequential fusion bursts and convert the energy into heat to drive a steam cycle. The concept utilized two opposing beams to illuminate a sequence of fusion targets at a repetition rate of once per second inside a waterfall of lithium contained in a steel chamber. The lithium would contain gigajoule fusion bursts and protect the steel chamber from all ions, target debris, and 14 MeV neutrons. Xcimer’s approach is largely based around this original concept.
Lawrence Livermore National Laboratory
The Shiva laser was a 10 kJ system at 1 micron wavelength. It was the largest laser in the world at the time, and was built to better understand the coupling of laser energy to a fusion target as well as target implosions. A major result was the discovery of the need to move to shorter wavelengths due to laser plasma interactions inhibiting effective coupling of laser energy to targets.
The first excimer laser was built at Livermore by Paul Hoff in 1972, and by the late 70s many more excimers had been discovered, including argon fluoride and krypton fluoride. Much of the gas chemistry of these lasers had been worked out by the end of the decade, with several kJ-scale systems built.
Lawrence Livermore National Laboratory
The Nova laser was built after lessons learned on Shiva, and could hit a target with a 45 kJ laser pulse at a much shorter wavelength of 351 nm. Ignition was expected, but it was more difficult to achieve the needed high-compression implosions than originally thought (the lower the laser energy, the higher the compression of the fuel capsule that is needed). Nevertheless, Nova significantly advanced the science of inertial fusion, and paved the way for the NIF.
A series of underground nuclear tests were fielded to lay to rest the viability of imploding and igniting laboratory scale fusion fuel capsules. These capsules were driven by siphoning a very small amount of x-ray energy from adjacent nuclear detonations, and they achieved ignition and high gain. Detailed reports are classified, but these tests conclusively demonstrated inertial fusion energy is possible with a high-enough energy laser.
National Academy of Sciences
The National Academy of Sciences held a review of inertial fusion in 1986, after analysis of all data to date from both laser fusion facilities as well as the Halite Centurion tests. The committee recommended the construction of a 10 MJ laser to ensure robust fusion ignition and high gain.
Lawrence Livermore National Laboratory
The National Ignition Facility was sold to Congress with a laser energy of 2 MJ, significantly short of the 10 MJ level recommended by the NAS. The 2 MJ system was a compromise, as a 10 MJ system with then-proposed technologies would have been far too expensive.
Culham Centre UK
The Joint European Torus set a world record in fusion plasma power gain of 0.67, producing 16 MW of peak fusion power with 24 MW of heat deposited into the plasma during a pulse of a couple seconds. While this gain is measured relative to fusion peak power, a value of 1 is defined as scientific breakeven for a tokamak. Thus the JET experiments have produced the highest performing fusion plasmas to date, after the NIF.
NRL
During the High Average Power Laser (HAPL) program, the Naval Research Laboratory (NRL) significantly advanced excimer laser technology for inertial fusion energy. In particular, the kJ-scale Electra laser operated repetitively at five shots per second for up to a day at a time, demonstrating key technology necessary for enabling an excimer laser to continuously shoot fusion fuel capsules in a power plant.
Lawrence Livermore National Laboratory
In 2022 the NIF achieved scientific breakeven, with the fusion burst from a fusion target exceeding the total laser energy delivered to the target. Since then, the NIF has improved over this result, with 5 MJ of fusion energy produced from a 2 MJ laser pulse. The significance of this result is the production of a fully ignited and burning plasma, with a fuel capsule gain of 20. The data from the NIF fully supports the original 1986 NAS conclusion that a 10 MJ would allow for robust ignition and high gain.