Laser-Plasma Electron Acceleration With Dense Plasma Wake Injection

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Solution Overview

Problem

Existing laser-based electron acceleration methods, such as Vacuum Laser Acceleration (VLA) and Laser WakeField Acceleration (LWFA), face challenges in producing high-quality electron beams with sufficient charge and low divergence and energy dispersion, which are crucial for applications like high-energy physics and radiotherapy.

Innovation Solution

A method and system for accelerating electrons using laser-plasma interaction, where an ultrashort laser pulse is directed at oblique incidence and s-polarization onto a dense plasma to generate a laser wake, allowing for the injection and heating of electrons into the wake for acceleration, optimizing electron beam quality.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Device complexity

If Vacuum Laser Acceleration (VLA) method is used to accelerate electrons, then the acceleration mechanism is simple, but the electron beam quality deteriorates with high divergence and strong energy dispersion

Engineering Contradiction:
Improveacceleration mechanism complexityVSAvoidelectron beam quality
Core Design Contradiction:
Device complexityVSManufacturing precision

Solution Approach 1:

The patent introduces a dense plasma as an intermediary medium between the laser field and the gas layer. The laser wake generated in the gas layer is reflected by the dense plasma, which mediates the interaction to improve electron injection efficiency and beam quality while maintaining the simplicity of the laser-based acceleration approach.

Inventive Principle:
Principle #24Intermediary (Mediator)

Solution Approach 2:

The patent changes the physical state and density parameters of the plasma medium. By creating a dense plasma with electron density between 10^19 and 10^21 cm^-3 (much higher than conventional LWFA), the system achieves better electron beam quality with lower divergence and energy dispersion while keeping the acceleration mechanism relatively simple.

Inventive Principle:
Principle #35Parameter changes

2Manufacturing precision

If Laser WakeField Acceleration (LWFA) is used to accelerate electrons, then electron beam quality is improved with low divergence and energy dispersion, but the charge per electron packet remains relatively low

Engineering Contradiction:
Improveelectron beam qualityVSAvoidelectron packet charge
Core Design Contradiction:
Manufacturing precisionVSQuantity of substance

Solution Approach 1:

The patent performs preliminary action by pre-generating a dense plasma layer before the main laser pulse interacts with the gas. This pre-prepared dense plasma serves as an efficient electron source that can be rapidly heated and injected into the laser wake, enabling high charge extraction while maintaining beam quality.

Inventive Principle:
Principle #10Preliminary action

Solution Approach 2:

The patent utilizes the periodic oscillation of the laser field to repeatedly extract electrons from the dense plasma and inject them into the accelerating wake structure. This periodic interaction mechanism enables continuous electron injection and accumulation of high charge in the electron packet while maintaining low divergence and energy dispersion through the structured wake field.

Inventive Principle:
Principle #19Periodic action

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

The method significantly increases the electron packet charge while maintaining low divergence and energy dispersion, producing high-quality electron beams suitable for applications requiring high energy and dose rates.

Implementation Method 1

By focusing pulses delivered by femtosecond lasers ranging from the TW class to the multi-PW class onto focal spots of a few microns to a few tens of micrometers, it is possible to obtain intensities greater than 10^18 W/cm^2. The extreme electric fields ionize the matter almost instantaneously and form an ultra-relativistic plasma

Methodology Applied
Scientific EffectLaser-induced plasma generation: Laser Ablation

Implementation Method 2

After reflection by the dense plasma, generate a laser wake in the gas layer. In the LWFA method, a laser delivers ultrashort pulses that are focused into a gas with a high intensity, typically greater than 10^18 W/cm^2. At the laser focus, the gas is ionized almost instantaneously by the ultra-intense laser field and forms a 'sub-dense' plasma

Methodology Applied
Scientific EffectLaser wakefield generation:

Implementation Method 3

Heat the electrons of said dense plasma to an energy such that a packet of said electrons is injected into said wake to be accelerated. In this method, electrons interact with an intense laser field in a vacuum and can be continuously accelerated, provided they remain in a specific phase of the field until they escape the laser beam. In the VLA method, the laser field itself delivers electric fields of several TV/m, which can, in principle, accelerate electrons to relativistic speeds

Methodology Applied
Scientific EffectLaser heating of plasma electrons: Laser Ablation

Implementation Method 4

LWFA-type devices can already provide high-quality electron beams: ultrashort (a few fs), small (micrometer scale), with low divergence, and low energy dispersion (a few percent). This LWFA mechanism enables the acceleration of electrons up to 8 GeV on the centimeter scale

Methodology Applied
Scientific EffectLaser wakefield electron acceleration:

Data Source

PatentEP4508949B1Method and system for accelerating electrons using laser-plasma interaction
Publication Date: 2026.03.11 COMMISSARIAT A LENERGIE ATOMIQUE ET AUX ENERGIES ALTERNATIVES
  • EP4508949B1 patent drawingFigure 1A~1B
  • EP4508949B1 patent drawingFigure 2~3
  • EP4508949B1 patent drawingFigure 4A~4B

AI summary

The invention relates to a method for accelerating electrons using laser-plasma interaction, wherein at least one laser pulse is directed onto a surface (SS) of a target in the condensed state (CS), the surface being covered with a layer of gas (CG), the intensity of the at least one pulse being enough to: - in a step A, generate, from the target in the condensed state, a dense plasma; - in a step B, after being reflected by the dense plasma, generate a wake in the gas layer; - in a step C, heat the electrons of the dense plasma to an energy such that a packet of the electrons is injected into the wake so as to be accelerated therein, the pulse, or at least the pulse that is intended to be reflected by the dense plasma and heat the electrons thereof, being at an s-polarised oblique incidence relative to the target.