HEDS Research Area

Laser-Plasma Interactions

The interaction of high-power lasers with plasmas leads to an extremely broad range of physics processes. Light propagation and energy deposition in plasmas is at the center of most HED and inertial confinement fusion concepts. At LLNL, our research encompasses all aspects of these interactions, from laser-energy deposition, to the development and control of laser–plasma instabilities. Controlled laser–plasma interactions have enabled transformative new concepts of light manipulation using plasma (known as plasma photonics); particle acceleration and secondary light sources; and pair production—paving the way to a new generation of plasma-based light and particle sources for HED applications.

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Laser-Wakefield Acceleration

Depiction of laser‒wakefield acceleration, showing the laser pulse, formation of an electron plasma wave, and the trapped electrons that get accelerated and emit betatron x-ray radiation.

A plasma is an ionized medium that can sustain electrical fields many orders of magnitude higher than those found in conventional radiofrequency accelerator structures. When short, intense laser pulses are focused into a gas, it produces electron plasma waves in which electrons can be trapped and accelerated to gigaelectronvolt (GeV) energies. This process, known as laser‒wakefield acceleration (LWFA), first proposed in 1979, is analogous to a surfer being propelled by an ocean wave. Since the advent of chirped-pulse amplification in the early 1980s and high-intensity lasers producing relativistic intensities on target (>1018 W/cm2), many research groups have been working on this topic. To date, the highest electron energy produced with LWFA is 8 GeV.

At LLNL, scientists are exploring one important application of LWFA—development of secondary light sources for applications. Bright sources of x rays, such as synchrotrons and x-ray free electron lasers (XFELs), are transformational tools for many science fields, including biology, material science, and medicine. Such sources rely on conventional particle accelerators, where electrons are accelerated to GeV energies. The accelerating particles are also wiggled in magnetic structures to emit x-ray radiation that is commonly used for molecular crystallography, fluorescence studies, chemical analysis, medical imaging, and many other applications. One of the drawbacks of synchrotrons and XFELs is their size and cost, because electric field gradients are limited to about a few tens of MeV/M in conventional accelerators. The proposed new x-ray source is produced when relativistic electrons oscillate during the LWFA process. The resulting betatron x-ray radiation has unique properties that are analogous to synchrotron radiation, with a 1000-fold shorter pulse. This source is produced when relativistic electrons oscillate during the LWFA process.

An important use of x rays from laser–plasma accelerators is in HED science research. Large laser and XFEL facilities aim to create in the laboratory the extreme temperatures and pressures that are usually found only in the interiors of stars and planets. To diagnose such extreme states of matter, development of efficient, versatile, and fast (sub-picosecond scale) x-ray probes has become essential. In these experiments, x-ray photons from LWFA can pass through dense material, and absorption of the x-rays can be directly measured, via spectroscopy or imaging, to help scientists study the temperature and density of the targets.

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Long-Pulse LPI and Plasma Photonics

Visualization of laser beams propagating through an ICF target, leading to complex laser–plasma phenomena.

Laser–plasma interactions (LPIs) are a central focus of research regarding inertial confinement fusion (ICF) and HED science in general. LPI research deals with the nonlinear propagation of intense lasers through plasmas, their energy deposition, and all the possible instabilities that can arise due to the nonlinear coupling of light waves and plasma waves.

Significant progress has been made over the past decade due to experiments on the National Ignition Facility (NIF) at LLNL. Our efforts involve developing and implementing new mitigation strategies to keep LPI processes under control in ICF experiments. This research requires advancing our understanding of fundamental LPI processes via focused science experiments in collaboration with our partners in academia and at other national laboratories. Ultimately, these experiments inform and guide us in the development of new LPI models that can be directly incorporated into macroscopic radiative-hydrodynamics simulation codes, enabling us to describe the results from the complex mutual interactions between LPI and hydrodynamics in ICF and HED experiments.

A crucial aspect that emerged from our expanded understanding of LPI is the many ways in which plasmas can modify the fundamental properties of light, including its propagation direction, amplitude, pulse duration, or polarization. As a result, a growing effort in the past decade to explore potential opportunities in light manipulation using plasma has turned into a vibrant new area of research known as plasma photonics. Using plasma in lieu of solids (like glass or crystals) to manipulate light essentially alleviates the concerns of optics damage, which dictates the scale (and cost) of high-power laser facilities and limits the maximum achievable laser intensity with chirped-pulse amplification technology. Work that started with using plasma gratings in NIF experiments to redirect laser light inside ICF targets and fine-tune the implosion symmetry has now been extended to include new concepts of plasma waveplates and polarizers, and beam combiners, as well as the first demonstrations of slow and fast light in plasmas.

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  • Pierre Michel

Relativistic Electron–Positron Pair Creation

In experiments to produce electron–positron pairs, a short-pulse laser fires a tightly focused pulse at a tiny gold disk. The laser transfers energy to electrons in the plasma in front of the target. As these high-energy electrons interact with the gold nuclei, some transfer their energy to high-energy photons, which then interact with the gold nuclei and transform into a lower-energy electron (green) and its mirror, a positron (purple). Image by Federico Fiuza/SLAC National Accelerator Laboratory.

Positrons are the antimatter particles of ordinary-matter electrons. Positrons and electrons have the same mass, but opposite charges, and they annihilate each other when they meet, converting their masses to energy. Particle accelerators are typically used to generate positrons for antimatter research.

At LLNL, we use high-power lasers to generate positrons by “zapping” a thick target made of a high-atomic-number (high-Z) material, such as gold or tantalum. This event produces very high-energy electrons, which are then deflected by the high-Z nucleus, emitting gamma rays that decay into electron-hole pairs.

In these experiments, billions of positrons are made in the laboratory in less than 100 picoseconds per laser shot—providing a new way to make antimatter accessible for exciting research avenues. For example, the interactions of laser-produced, relativistic, dense electron–positron pair plasmas could mimic the physics processes of some of the most energetic events in the universe, such as the gamma-ray bursts near black holes. We are actively working to achieve this capability. For example, we are exploring how to increase the efficiency by converting more laser energy to the electron–positron pairs, as well as by using new target and laser configurations.

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  • Hui Chen

Laser–Particle Acceleration Experiments and Simulations

Illustration depicting a laser-driven particle acceleration experiment.

Short-pulse ion acceleration has been a topic of interest for decades. These energetic particles have a wide range of applications, including diagnosing extreme electromagnetic fields in laser-driven experiments; heating sample materials to extreme conditions of temperature and density; creating heavy ion or neutron sources; and providing cancerous tumor therapy. Compared to traditional particle accelerators, laser-driven acceleration takes place on the micro-meter scale with extremely large electric fields (~teraVolt/meter). The most studied ion acceleration mechanism is known as target-normal sheath acceleration. Over the last two decades, many experiments have studied this process with the aim of developing scaling laws that can be used to predict the beam characteristics from a given laser‒target interaction.

While many of these studies have been fruitful in describing scaling of the properties of these beams, experiments were typically driven by lasers with pulse widths <1 picosecond (or one trillionth of a second). At LLNL, scientists have demonstrated and explained the ability to generate tens of MeV ion beams with multi-picosecond laser interactions on the Advanced Radiographic Capability (ARC) laser at LLNL’s National Ignition Facility, which were counter to the well-established scalings. Continuing research seeks to push this capability and understanding by performing large-scale, particle-in-cell simulations of these laser experiments on LLNL’s supercomputing resources.

In addition to these expensive large-scale simulations, researchers also produce thousands of lower-dimensional (and computationally “cheaper”) simulations. By utilizing advanced machine-learning methods, scientists can now construct realistic maps of large, multi-dimensional parameter spaces to look for laser pulse and target combinations that can produce optimized ion sources. These new machine-learning-based models then serve as the basis for experimental investigations utilizing high-repetition-rate laser facilities, capable of delivering high-intensity laser pulses at multi-Hz rates.

Researchers at LLNL are developing diagnostics that can operate in extremely hostile experimental environments with integrated machine learning for rapid and accurate analysis of data “on the fly.” The simulations and experiments are being integrated through artificial intelligence in order to smartly navigate experimental investigation without human intervention—massively speeding up the process of scientific learning. The goals of this work include controlling and optimizing laser-driven particle sources, while also tailoring secondary-source delivery, including high- and low-energy x-ray sources.

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  • Derek Mariscal
  • Tammy Ma