R. Trines
Rutherford Appleton Laboratory
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Featured researches published by R. Trines.
Physics of Plasmas | 2006
C. D. Murphy; R. Trines; Jorge Vieira; Albert Reitsma; R. Bingham; John Collier; E. J. Divall; P. S. Foster; C. J. Hooker; A. J. Langley; P.A. Norreys; Ricardo Fonseca; F. Fiuza; L. O. Silva; J. T. Mendonça; W. B. Mori; J. G. Gallacher; R. Viskup; D. A. Jaroszynski; S. P. D. Mangles; A. G. R. Thomas; K. Krushelnick; Z. Najmudin
Photon acceleration is the phenomenon whereby a light wave changes color when propagating through a medium whose index of refraction changes in time. This concept can be used to describe the spectral changes experienced by electromagnetic waves when they propagate in spatially and temporally varying plasmas. In this paper the detection of a large-amplitude laser-driven wake field is reported for the first time, demonstrating photon acceleration. Several features characteristic of photon acceleration in wake fields, such as splitting of the main spectral peak and asymmetries between the blueshift and redshift for large shifts, have been observed. The experiment is modeled using both a novel photon-kinetic code and a three-dimensional particle-in-cell code. In addition to the wide-ranging applications in the field of compact particle accelerators, the concept of wave kinetics can be applied to understanding phenomena in nonlinear optics, space physics, and fusion energy research.
Physics of Plasmas | 2009
P. A. Norreys; F. N. Beg; Y. Sentoku; L. O. Silva; R. A. Smith; R. Trines
A review is presented here of a number of invited papers presented at the 2008 American Physical Society April meeting [held jointly with High Energy Density Physics/High Energy Density Laboratory Astrophysics (HEDP/HEDLA) Conference] devoted to intense laser-matter interactions. They include new insights gained from wave-kinetic theory into laser-wakefield accelerators and drift wave turbulence interacting with zonal flows in magnetized plasmas; interactions with cluster media for the generation of radiative blast waves; fast electron energy transport in cone-wire targets; numerical investigations into Weibel instability in electron-positron-ion plasmas and the generation of gigabar pressures with thin foil interactions.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016
E. Gschwendtner; E. Adli; L. D. Amorim; Robert Apsimon; R. Assmann; A.M. Bachmann; F. Batsch; J. Bauche; V. K. Berglyd Olsen; M. Bernardini; R. Bingham; B. Biskup; T. Bohl; C. Bracco; Philip Burrows; Graeme Burt; B. Buttenschön; A. Butterworth; A. Caldwell; M. Cascella; Eric Chevallay; S. Cipiccia; H. Damerau; L. Deacon; P. Dirksen; S. Doebert; Ulrich Dorda; J. Farmer; Valentin Fedosseev; Eduard Feldbaumer
The Advanced Proton Driven Plasma Wakefield Acceleration Experiment (AWAKE) aims at studying plasma wakefield generation and electron acceleration driven by proton bunches. It is a proof-of-principle R&D experiment at CERN and the world׳s first proton driven plasma wakefield acceleration experiment. The AWAKE experiment will be installed in the former CNGS facility and uses the 400 GeV/c proton beam bunches from the SPS. The first experiments will focus on the self-modulation instability of the long (rms ~12 cm) proton bunch in the plasma. These experiments are planned for the end of 2016. Later, in 2017/2018, low energy (~15 MeV) electrons will be externally injected into the sample wakefields and be accelerated beyond 1 GeV. The main goals of the experiment will be summarized. A summary of the AWAKE design and construction status will be presented.
Physics of Plasmas | 2006
R. Trines; P.A. Norreys
The propagation of electrostatic plasma waves having relativistic phase speed and amplitude has been studied. The plasma is described as a warm, relativistic, collisionless, nonequilibrium, one-dimensional electron fluid. Wave-breaking limits for the electrostatic field are calculated for nonrelativistic initial plasma temperatures and arbitrary phase velocities, and a correspondence between wave breaking and background particle trapping has been uncovered. Particular care is given to the ultrarelativistic regime (γφ2kBT0∕(mec2)≫1), since conflicting results for this regime have been published in the literature. It is shown here that the ultrarelativistic wave-breaking limit will reach arbitrarily large values for γφ→∞ and fixed initial temperature. Previous results claiming that this limit is bounded even in the limit γφ→∞ are shown to suffer from incorrect application of the relativistic fluid equations and higher, more realistic wave-breaking limits are appropriate.
Physics of Plasmas | 2012
R. H. H. Scott; F. Perez; J. J. Santos; C. P. Ridgers; J. R. Davies; K. L. Lancaster; S. D. Baton; Ph. Nicolaï; R. Trines; A. R. Bell; S. Hulin; Michail Tzoufras; S.J. Rose; P. A. Norreys
A systematic experimental and computational investigation of the effects of three well characterized density scalelengths on fast electron energy transport in ultra-intense laser-solid interactions has been performed. Experimental evidence is presented which shows that, when the density scalelength is sufficiently large, the fast electron beam entering the solid-density plasma is best described by two distinct populations: those accelerated within the coronal plasma (the fast electron pre-beam) and those accelerated near or at the critical density surface (the fast electron main-beam). The former has considerably lower divergence and higher temperature than that of the main-beam with a half-angle of ∼20°. It contains up to 30% of the total fast electron energy absorbed into the target. The number, kinetic energy, and total energy of the fast electrons in the pre-beam are increased by an increase in density scalelength. With larger density scalelengths, the fast electrons heat a smaller cross sectional are...
Physics of Plasmas | 2010
Gianluca Sarri; K.L. Lancaster; R. Trines; E.L. Clark; S. Hassan; J. Jiang; N. Kageiwa; Nelson Lopes; R. Ramis; A. Rehman; X. Ribeyre; C. Russo; R. H. H. Scott; T. Tanimoto; M. Temporal; M. Borghesi; J. R. Davies; Z. Najmudin; K.A. Tanaka; M. Tatarakis; P. A. Norreys
The experimental study of the behavior of deuterium plasma with densities between 2×1018 and 2×1020 cm−3, subjected to a 6 TW, 30 ps, 3×1018 W cm−2 laser pulse, is presented. Conclusive experimental proof that a single straight channel is generated when the laser pulse interacts with the lowest densities is provided. This channel shows no small-scale longitudinal density modulations, extends up to 2 mm in length and persists for up to 150 ps after the peak of the interaction. Bifurcation of the channel after 1 mm propagation distance is observed for the first time. For higher density interactions, above the relativistic self-focusing threshold, bubblelike structures are observed to form at late times. These observations have implications for both laser wakefield accelerators and fast ignition inertial fusion studies.
IEEE Transactions on Plasma Science | 2000
A. Reitsma; R. Trines; Vladimir V. Goloviznin
Electron acceleration in a one-dimensional plasma wave has been simulated, with emphasis on minimizing the energy spread of an accelerated electron bunch, while keeping the mean energy gain at a reasonable level. Bunch length, beam loading, and the injection phase are tuned to reach this goal. The simulation results show that, in a wide range of initial bunch lengths and beam loading parameters, an optimum acceleration distance exists, which combines low energy spread and high energy gain. The energy spread at the optimum is found to be weakly dependent on bunch length and beam loading, while it is highly sensitive to deviations in the injection phase.
Physics of Plasmas | 2009
R. Trines; R. Bingham; L. O. Silva; J. T. Mendonça; P. K. Shukla; C. D. Murphy; M. W. Dunlop; J. A. Davies; R. Bamford; Andris Vaivads; P. A. Norreys
Nonlinear wave-driven processes in plasmas are normally described by either a monochromatic pump wave that couples to other monochromatic waves or as a random phase wave coupling to other random phase waves. An alternative approach involves a random or broadband pump coupling to monochromatic and/or coherent structures in the plasma. This approach can be implemented through the wave kinetic model. In this model, the incoming pump wave is described by either a bunch (for coherent waves) or a sea (for random phase waves) of quasiparticles. This approach has been applied to both photon acceleration in laser wakefields and drift wave turbulence in magnetized plasma edge configurations. Numerical simulations have been compared to experiments, varying from photon acceleration to drift mode-zonal flow turbulence, and good qualitative correspondences have been found in all cases.
Plasma Physics and Controlled Fusion | 2007
Simon M. Hooker; E. Brunetti; E. Esarey; J. G. Gallacher; C. G. R. Geddes; A J Gonsalves; D. A. Jaroszynski; Christos Kamperidis; S. Kneip; K. Krushelnick; W. P. Leemans; S. P. D. Mangles; C. D. Murphy; B. Nagler; Z. Najmudin; K Nakamura; P. A. Norreys; D Panasenko; T. P. Rowlands-Rees; C. B. Schroeder; C s Tóth; R. Trines
During the last few years laser-driven plasma accelerators have been shown to generate quasi-monoenergetic electron beams with energies up to several hundred MeV. Extending the output energy of laser-driven plasma accelerators to the GeV range requires operation at plasma densities an order of magnitude lower, i.e. 1018 cm−3, and increasing the distance over which acceleration is maintained from a few millimetres to a few tens of millimetres. One approach for achieving this is to guide the driving laser pulse in the plasma channel formed in a gas-filled capillary discharge waveguide. We present transverse interferometric measurements of the evolution of the plasma channel formed and compare these measurements with models of the capillary discharge. We describe in detail experiments performed at Lawrence Berkeley National Laboratory and at Rutherford Appleton Laboratory in which plasma accelerators were driven within this type of waveguide to generate quasi-monoenergetic electron beams with energies up to 1 GeV.
Physics of Plasmas | 2006
Albert Reitsma; R. Trines; R. Bingham; R. A. Cairns; J. T. Mendonça; D. A. Jaroszynski
This paper discusses photon kinetic theory, which is a description of the electromagnetic field in terms of classical particles in coordinate and wave number phase space. Photon kinetic theory is applied to the interaction of laser pulses with underdense plasma and the transfer of energy and momentum between the laser pulse and the plasma is described in photon kinetic terms. A comparison is made between a one-dimensional full wave and a photon kinetic code for the same laser and plasma parameters. This shows that the photon kinetic simulations accurately reproduce the pulse envelope evolution for photon frequencies down to the plasma frequency.