Influence of Ionization and Beam Quality on Interaction of TW-Peak CO 2 Laser With Hydrogen Plasma (original) (raw)

Self-modulated laser-plasma acceleration in a H2 gas target, simulated in a spectral particle-in-cell algorithm: wakefield and electron bunch properties

2019 SBFoton International Optics and Photonics Conference (SBFoton IOPC), 2019

We evaluate the results of self-modulated, laser wakefield acceleration of electrons in homogeneous, 150-μm-thick hydrogen gas target, simulated using the spectral particle-in-cell algorithm FBPIC. Considering a single 2-TW laser pulse at 800-nm, which generates ionization and plasma displacement at relativistic intensities, we discuss the resultant wakefield phases, wave-breaking, and the ejected electron bunch properties: charge, length, divergence and energy, also comparing with experimental results.

Particle-in-cell Simulations on Laser-Plasma Interactions in Shock Ignition

Bulletin of the American Physical Society, 2012

We present a series of 1D and 2D particle-in-cell (PIC) simulations using the full PIC code\ textit {OSIRIS} for the shock ignition experiments carried out on the OMEGA facility. The laser intensity is $ I= 2\ times 10^{15} /cm/cm /cm^ 2$. The density profile used in PIC simulations is provided by the hydro simulation and has the scale length $ L= 17\ mu $ m at the quarter-critical-density surface. Physical electron-ion collisions are included in our simulations with a benchmarked collision package in\ textit {OSIRIS}. The 1D simulation covering a larger ...

Efficient modeling of laser–plasma interactions in high energy density scenarios

Plasma Physics and Controlled Fusion, 2011

We describe how a new framework for coupling a full-particle-in-cell (PIC) algorithm with a reduced PIC algorithm has been implemented into the OSIRIS code. We show that OSIRIS, with this new hybrid-PIC algorithm, can efficiently and accurately model high energy density scenarios such as ion acceleration in laser-solid interactions and fast ignition of fusion targets. We model, for the first time, the full-density range of a fast ignition target in a fully selfconsistent hybrid-PIC simulation, illustrating the possibility of stopping the laser generated electron flux at the core region with relatively high efficiencies. Computational speedups greater than 1000 times are demonstrated, opening the way for full-scale multi-dimensional modeling of high energy density scenarios and the guiding of future experiments.

CO2 Laser acceleration of forward directed MeV proton beams in a gas target at critical plasma density

Journal of Plasma Physics, 2012

The generation of 1-5 MeV protons from the interaction of a 3 ps TW CO 2 laser pulse with a gas target with a peak density around the critical plasma density has been studied by 2D particle-in-cell simulations. The proton acceleration in the preformed plasma with a symmetric, linearly ramped density distribution occurs via formation of sheath of the hot electrons on the back surface of the target. The maximum energy of the hot electrons and, hence, net acceleration of protons is mainly defined by Forward Raman scattering instability in the underdense part of the plasma. Forward directed ion beams from a debris free gaseous target can find an application as a high-brightness ion source-injector to a conventional accelerator operating up to kHz pulse repetition frequency.

Computer simulation of radiation acceleration mode in laser-plasma interaction

We present numerical studies on the ion acceleration from thin foils irradiated by ultra-high contrast laser pulses. Two-dimensional particle-in-cell (PIC) simulations reveal that ions are for a certain time accelerated in a phase-stable way by the laser radiation pressure. The development of the Rayleigh-Taylor instability leads to destroy foils and to decelerate the ion acceleration rate.

Three-dimensional simulation of laser–plasma-based electron acceleration

Pramana, 2012

A sequential three-dimensional (3D) particle-in-cell simulation code PICPSI-3D with a user friendly graphical user interface (GUI) has been developed and used to study the interaction of plasma with ultrahigh intensity laser radiation. A case study of laser-plasma-based electron acceleration has been carried out to assess the performance of this code. Simulations have been performed for a Gaussian laser beam of peak intensity 5 × 10 19 W/cm 2 propagating through an underdense plasma of uniform density 1 × 10 19 cm −3 , and for a Gaussian laser beam of peak intensity 1.5 × 10 19 W/cm 2 propagating through an underdense plasma of uniform density 3.5 × 10 19 cm −3. The electron energy spectrum has been evaluated at different time-steps during the propagation of the laser beam. When the plasma density is 1 × 10 19 cm −3 , simulations show that the electron energy spectrum forms a monoenergetic peak at ∼14 MeV, with an energy spread of ±7 MeV. On the other hand, when the plasma density is 3.5 × 10 19 cm −3 , simulations show that the electron energy spectrum forms a monoenergetic peak at ∼23 MeV, with an energy spread of ±7.5 MeV.

Off-harmonic optical probing of high intensity laser plasma expansion dynamics in solid density hydrogen jets

Scientific Reports, 2022

Due to the non-linear nature of relativistic laser induced plasma processes, the development of laser-plasma accelerators requires precise numerical modeling. Especially high intensity laser-solid interactions are sensitive to the temporal laser rising edge and the predictive capability of simulations suffers from incomplete information on the plasma state at the onset of the relativistic interaction. Experimental diagnostics utilizing ultra-fast optical backlighters can help to ease this challenge by providing temporally resolved inside into the plasma density evolution. We present the successful implementation of an off-harmonic optical probe laser setup to investigate the interaction of a high-intensity laser at 5.4 × 10 21 W/cm 2 peak intensity with a solid-density cylindrical cryogenic hydrogen jet target of 5 µm diameter as a target test bed. The temporal synchronization of pump and probe laser, spectral filtering and spectrally resolved data of the parasitic plasma self-emission are discussed. The probing technique mitigates detector saturation by self-emission and allowed to record a temporal scan of shadowgraphy data revealing details of the target ionization and expansion dynamics that were so far not accessible for the given laser intensity. Plasma expansion speeds of up to (2.3 ± 0.4) × 10 7 m/s followed by full target transparency at 1.4 ps after the high intensity laser peak are observed. A three dimensional particle-in-cell simulation initiated with the diagnosed target pre-expansion at −0.2 ps and post processed by ray tracing simulations supports the experimental observations and demonstrates the capability of time resolved optical diagnostics to provide quantitative input and feedback to the numerical treatment within the time frame of the relativistic laser-plasma interaction. Full control of high-intensity laser-matter interaction is key to enable applications like fast ignition for inertial confinement fusion 1,2 or laser-plasma driven particle sources 3 for warm dense matter research 4 , time-resolved studies of transient fields 5 and translational research for radiation oncology 6. It requires predictive power of simulation tools in quantitative agreement with experimental results and it is still challenging to achieve for laser-solid interactions 3. One important reason is the large range of interaction physics at different time scales and laser intensities impacting the solid prior to the arrival of the laser peak 7 and connected to that the difficulty of capturing the dynamics by a single simulation tool. Although the relativistic laser-plasma interaction can be mapped by particle-in-cell simulations 8 , the computable time window is limited and the captured physics must be

Laser acceleration of protons using multi-ion plasma gaseous targets

New Journal of Physics

We present a theoretical and numerical study of a novel acceleration scheme by applying a combination of laser radiation pressure and shielded Coulomb repulsion in laser acceleration of protons in multi-species gaseous targets. By using a circularly polarized CO2 laser pulse with a wavelength of 10 μm—much greater than that of a Ti: Sapphire laser—the critical density is significantly reduced, and a high-pressure gaseous target can be used to achieve an overdense plasma. This gives us a larger degree of freedom in selecting the target compounds or mixtures, as well as their density and thickness profiles. By impinging such a laser beam on a carbon-hydrogen target, the gaseous target is first compressed and accelerated by radiation pressure until the electron layer disrupts, after which the protons are further accelerated by the electron-shielded carbon ion layer. An 80 MeV quasi-monoenergetic proton beam can be generated using a half-sine shaped laser beam with a peak power of 70 TW...

Ion Acceleration by Collisionless Shocks in High-Intensity-Laser–Underdense-Plasma Interaction

Physical Review Letters, 2004

Ion acceleration by the interaction of an ultraintense short-pulse laser with an underdense-plasma has been studied at intensities up to 3 10 20 W=cm 2 . Helium ions having a maximum energy of 13:2 1:0 MeV were measured at an angle of 100 from the laser propagation direction. The maximum ion energy scaled with plasma density as n 0:700:05 e . Two-dimensional particle-in-cell simulations suggest that multiple collisionless shocks are formed at high density. The interaction of shocks is responsible for the observed plateau structure in the ion spectrum and leads to an enhanced ion acceleration beyond that possible by the ponderomotive potential of the laser alone.

Plasma physics with intense laser and ion beams

Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 2000

The unique combination of an intense heavy ion beam and a high-energy Nd:glass laser system at Gesellschaft f ur Schwerionenforschung (GSI-Darmstadt) facilitates pioneering beam-plasma interaction experiments and thus allows to address basic physics issues associated with heavy ion-driven inertial fusion. The deposition power of the intense heavy ion beam from the synchrotron has recently been increased to 1 kJ/g. The hydrodynamic response of solid targets was measured. A comparison with detailed numerical simulations attributes the target response to a pressure pulse of 3 GPa at a maximum temperature of 2500 K. Beam plasma interaction experiments to measure the stopping power of laser plasmas for heavy ion beams have been performed and show an increased energy loss for Ni ions in a 60 eV dense carbon plasma. Subsequently performed time-resolved charge-state measurements indicate that the increased stopping power can partially be attributed to a high charge state of the beam ions traversing the plasma. Improved plasma diagnostic by high-resolution spectroscopy revealed the unexpected existence of He-like resonance and intercombination lines (He a 1s2p 3 P 1 ±1s 2 and Y a 1s2p 3 P 1 ±1s 2 ) of¯uorine even for a modest laser intensity of 5´10 11 W/cm 2 . Ó