Investigation of accelerated carbon ions with the presence of QED effect by ultra-intense high-power lasers (original) (raw)

Simulations of carbon ion acceleration by 10 PW laser pulses on ELI-NP

Laser and Particle Beams, 2019

We present results of 2D particle-in-cell (PIC) simulations of carbon ion acceleration by 10 petawatt (PW) laser pulses, studying both circular polarized (CP) and linear polarized (LP) pulses. We carry out a thickness scanning of a solid carbon target to investigate the ideal thickness for carbon ion acceleration mechanisms using a 10 PW laser with an irradiance of 5 × 1022 W cm−2. The energy spectra of carbon ions and electrons and their temperature are studied. Additionally, for the carbon ions, their angular divergence is studied. It is shown that the ideal thickness for the carbon acceleration is 120 nm and the cutoff energy for carbon ions is 5 and 3 GeV for CP and LP pulses, respectively. The corresponding carbon ions temperature is ~1 and ~0.75 GeV. On the other hand, the energy cutoff for the electrons is ~500 MeV with LP and ~400 MeV with CP laser pulses. We report that the breakout afterburner mechanism is most likely causing the acceleration of carbon ions to such high en...

Laser-accelerated high-energy ions: state of-the-art and applications

Journal of Physics: Conference Series, 2007

The acceleration of high-energy ion beams (up to several tens of MeV per nucleon) following the interaction of short (t < 1ps) and intense (I 2 > 10 18 W cm -2 μm -2 ) laser pulses with solid targets has been one of the most important results of recent laser-plasma research. The acceleration is driven by relativistic electrons, which acquire energy directly from the laser pulse and set up extremely large (~TV/m) space charge fields at the target interfaces. In view of a number of advantageous properties, laser-driven ion beams can be employed in a number of innovative applications in the scientific, technological and medical areas. Among these, their possible use in hadrontherapy, with potential reduction of facility costs, has been proposed recently. This paper will briefly review the current state-of-the-art in laser-driven proton/ion source development, and will discuss the progress needed in order to implement some of the above applications. Recent results relating to the optimization of beam energy, spectrum and collimation will be presented.

The Radiation Reaction Effect on Electrons at Super-High Laser Intensities with Application to Ion Acceleration

AIP Conference Proceedings, 2009

At super-high laser intensities the radiation back reaction on electrons becomes so significant that its influence on laser-plasma interaction cannot be neglected while simulating these processes with particle-in-cell (PIC) codes. We discuss a way of taking the radiation effect on electrons into account and extracting spatial and frequency distributions of the generated highfrequency radiation. We also examine ponderomotive acceleration of ions in the double layer created by strong laser pulses and we compare an analytical description with PIC simulations as well. We discuss: (1) non-stationary features found in simulations, (2) electron cooling effect due to radiation losses, and (3) the limits of the analytical model.

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

Laser acceleration of electrons to giga-electron-volt energies using highly charged ions

Physical Review E, 2006

The recent proposal to use highly charged ions as sources of electrons for laser acceleration ͓S. X. Hu and A. F. Starace, Phys. Rev. Lett. 88, 245003 ͑2002͔͒ is investigated here in detail by means of three-dimensional, relativistic Monte Carlo simulations for a variety of system parameters, such as laser pulse duration, ionic charge state, and laser focusing spot size. Realistic laser focusing effects-e.g., the existence of longitudinal laser field components-are taken into account. Results of spatial averaging over the laser focus are also presented. These numerical simulations show that the proposed scheme for laser acceleration of electrons from highly charged ions is feasible with current or near-future experimental conditions and that electrons with GeV energies can be obtained in such experiments.

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.

Acceleration of heavy Ions to MeV/nucleon Energies by Ultrahigh-Intensity Lasers

2002

In this thesis the acceleration of heavy ions to multi-MeV energies by means of a laser is demonstrated for the first time. Using an ultrahigh-intensity laser, with focal intensities exceeding 5 x 10^19 W/cm^2, the laser-plasma interaction becomes relativistic and a strong electron current is driven in laser direction. These relativistic electrons penetrate the target foil and set up a quasistatic electric field at the target rear surface. This field is of the order of TV/m and accelerated Fluorine ions to energies of 100 MeV, i.e. about 10 % light speed, within 300 fs. While a normal accelerator needs a distance of roughly 100 m to reach these energies, the laser-driven acceleration achieves this in about 10 microns. Within the scope of this work, a technique was developed to select a specific ion species. The energy spectra and charge state distributions of several different species were measured and used to analyze the acceleration mechanism. The measured results were than compar...

Effect of a nanometer scale plasma on laser-accelerated ion beams

New Journal of Physics, 2009

Energies of laser-accelerated ions from thin foils in the so-called 'ultra-high-contrast' regime have been measured for various preformed plasma sizes on the non-irradiated foil surface. Whereas energies of protons accelerated in the laser counter-propagating direction remain almost constant for plasma scale length up to 300 nm, we found that plasmas as short as a few tens of nanometers reduce the maximum energy of ions accelerated in the laser direction. These experimental measurements are numerically confirmed with two-dimensional particle-in-cell simulations coupled to hydrodynamic calculation. Moreover, our experimental results, supported by simulations, provide evidence for the occurrence of ion wave breaking, and demonstrate its ability to mitigate the ion energy reduction due to the plasma gradient. This wave breaking is observed and characterized for both proton and carbon ion components.

Carbon ion acceleration from thin foil targets irradiated by ultrahigh-contrast, ultraintense laser pulses

New Journal of …, 2010

In this study, ion acceleration from thin planar target foils irradiated by ultrahigh-contrast (10 10 ), ultrashort (50 fs) laser pulses focused to intensities of 7 × 10 20 W cm −2 is investigated experimentally. Target normal sheath acceleration (TNSA) is found to be the dominant ion acceleration mechanism when the target thickness is 50 nm and laser pulses are linearly polarized. Under these conditions, irradiation at normal incidence is found to produce higher energy ions than oblique incidence at 35 • with respect to the target normal. Simulations using one-dimensional (1D) boosted and 2D particle-in-cell codes support the result, showing increased energy coupling efficiency to fast electrons for normal incidence. The effects of target composition and thickness on the acceleration of carbon ions are reported and compared to calculations using analytical models of ion acceleration.

Longitudinal Ion Acceleration From High-Intensity Laser Interactions With Underdense Plasma

Plasma Science, …, 2008

Longitudinal ion acceleration from high-intensity (I ∼ 10 20 Wcm −2 ) laser interactions with helium gas jet targets (n e ≈ 0.04n c ) have been observed. The ion beam has a maximum energy for He 2+ of (40 +3 −8 ) MeV and was directional along the laser propagation path, with the highest energy ions being collimated to a cone of less than 10 • . 2D particle-in-cell simulations have been used to investigate the acceleration mechanism. The time varying magnetic field associated with the fast electron current provides a contribution to the accelerating electric field as well as providing a collimating field for the ions. A strong correlation between the plasma density and the ion acceleration was found. A short plasma scale-length at the vacuum interface was observed to be beneficial for the maximum ion energies, but the collimation appears to be improved with longer scale-lengths due to enhanced magnetic fields in the ramp acceleration region.