A. P. L. Robinson
Rutherford Appleton Laboratory
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by A. P. L. Robinson.
New Journal of Physics | 2008
A. P. L. Robinson; M. Zepf; S. Kar; R. G. Evans; C. Bellei
A new regime is described for radiation pressure acceleration of a thin foil by an intense laser beam of above 1020 W cm−2. Highly monoenergetic proton beams extending to giga-electron-volt energies can be produced with very high efficiency using circularly polarized light. The proton beams have a very small divergence angle (<4°). This new method allows the construction of ultra-compact proton and ion accelerators with ultra-short particle bursts.
Applied Physics Letters | 2006
D. Neely; P. S. Foster; A. P. L. Robinson; Filip Lindau; Olle Lundh; Anders Persson; Claes-Göran Wahlström; P. McKenna
The generation of proton beams from ultrathin targets, down to 20 nm in thickness, driven with ultrahigh contrast laser pulses is explored. the conversion efficiency from laser energy into protons increases as the foil thickness is decreased, with good beam quality and high efficiencies of 1% being achieved, for protons with kinetic energy exceeding 0.9 MeV, for 100 nm thick aluminum foils at intensities of 10(19) W/cm(2) with 33 fs, 0.3 J pulses. To minimize amplified spontaneous emission (ASE) induced effects disrupting the acceleration mechanism, exceptional laser to ASE intensity contrasts of up to 1010 are achieved by introducing a plasma mirror to the high contrast 10 Hz multiterawatt laser at the Lund Laser Centre. It is shown that for a given laser energy on target, regimes of higher laser-to-proton energy conversion efficiency. can be accessed with increasing contrast. The increasing efficiency as the target thickness decreases is closely correlated to an increasing proton temperature. (c) 2006 American Institute of Physics.
Nuclear Fusion | 2014
A. P. L. Robinson; D. J. Strozzi; J.R. Davies; Laurent Gremillet; J.J. Honrubia; Tomoyuki Johzaki; R. J. Kingham; M. Sherlock; A.A. Solodov
Fast ignition (FI) inertial confinement fusion is a variant of inertial fusion in which DT fuel is first compressed to high density and then ignited by a relativistic electron beam generated by a fast (<20?ps) ultra-intense laser pulse, which is usually brought in to the dense plasma via the inclusion of a re-entrant cone. The transport of this beam from the cone apex into the dense fuel is a critical part of this scheme, as it can strongly influence the overall energetics. Here we review progress in the theory and numerical simulation of fast electron transport in the context of FI. Important aspects of the basic plasma physics, descriptions of the numerical methods used, a review of ignition-scale simulations, and a survey of schemes for controlling the propagation of fast electrons are included. Considerable progress has taken place in this area, but the development of a robust, high-gain FI ?point design? is still an ongoing challenge.
New Journal of Physics | 2008
Sebastian M. Pfotenhauer; Oliver Jäckel; A. Sachtleben; Jens Polz; Ziegler W; Hans-Peter Schlenvoigt; K.-U. Amthor; Malte C. Kaluza; K.W.D. Ledingham; R. Sauerbrey; Paul Gibbon; A. P. L. Robinson; Heinrich Schwoerer
The rapid progress in the field of laser particle acceleration has stimulated a debate about the promising perspectives of laser based ion beam sources. For a long time, the beams produced exhibited quasi-thermal spectra. Recent proof-of-principle experiments demonstrated that ion beams with narrow energy distribution can be generated from special target geometries. However, the achieved spectra were strongly limited in terms of monochromacity and reproducibility. We show that microstructured targets can be used to reliably produce protons with monoenergetic spectra above 2 MeV with less than 10% energy spread. Detailed investigations of the effects of laser ablation on the target resulted in a significant improvement of the reproducibility. Based on statistical analysis, we derive a scaling law between proton peak position and laser energy, underlining the suitability of this method for future applications. Both the quality of the spectra and the scaling law are well reproduced by numerical simulations.
Physical Review Letters | 2012
Gianluca Sarri; Andrea Macchi; C. A. Cecchetti; S. Kar; T. V. Liseykina; X. H. Yang; Mark E Dieckmann; J. Fuchs; M. Galimberti; L. A. Gizzi; R. Jung; Ioannis Kourakis; J. Osterholz; Francesco Pegoraro; A. P. L. Robinson; L. Romagnani; O. Willi; M. Borghesi
The dynamics of magnetic fields with an amplitude of several tens of megagauss, generated at both sides of a solid target irradiated with a high-intensity (~10(19) W/cm(2)) picosecond laser pulse, has been spatially and temporally resolved using a proton imaging technique. The amplitude of the magnetic fields is sufficiently large to have a constraining effect on the radial expansion of the plasma sheath at the target surfaces. These results, supported by numerical simulations and simple analytical modeling, may have implications for ion acceleration driven by the plasma sheath at the rear side of the target as well as for the laboratory study of self-collimated high-energy plasma jets.
Plasma Physics and Controlled Fusion | 2007
A. P. L. Robinson; D. Neely; P. McKenna; R. G. Evans
We address the question of whether multiple high intensity (> 10(18) W cm(-2)) laser pulses ( each O( 100 fs)) can produce proton beams with a modified energy spectrum on irradiating a foil target. This has been studied in one dimension with both Vlasov and particle-in-cell codes. A reduction in the maximum proton energy, and the generation of spectral peaks, is observed. This is the first theoretical demonstration of spectral peak generation by purely optical means. The mechanism, which has been termed multiple pulse sheath acceleration, that produces these spectral peaks is described, and the same mechanism occurs in both sets of simulations.
Plasma Physics and Controlled Fusion | 2011
M. N. Quinn; Xiaohui Yuan; X. X. Lin; D. C. Carroll; O. Tresca; Robert Gray; M. Coury; Changzheng Li; Y. T. Li; C.M. Brenner; A. P. L. Robinson; D. Neely; B. Zielbauer; B. Aurand; J. Fils; T. Kuehl; P. McKenna
The propagation of fast electrons produced in the interaction of relativistically intense, picosecond laser pulses with solid targets is experimentally investigated using K-alpha emission as a diagnostic. The role of fast electron refluxing within the target, which occurs when the electrons are reflected by the sheath potentials formed at the front and rear surfaces, is elucidated. The targets consist of a Cu fluorescence layer of fixed thickness at the front surface backed with a propagation layer of CH, the thickness of which is varied to control the number of times the refluxing fast electron population transits the Cu fluorescence layer. Enhancements in the K-alpha yield and source size are measured as the thickness of the CH layer is decreased. Comparison with analytical and numerical modelling confirms that significant refluxing occurs and highlights the importance of considering this phenomenon when deriving information on fast electron transport from laser-solid interaction experiments involving relatively thin targets.
Applied Physics Letters | 2014
J. S. Green; A. P. L. Robinson; N. Booth; D. C. Carroll; R. J. Dance; Robert Gray; D. A. MacLellan; P. McKenna; C. D. Murphy; Dean Rusby; L. Wilson
Bright proton beams with maximum energies of up to 30 MeV have been observed in an experiment investigating ion sheath acceleration driven by a short pulse (<50 fs) laser. The scaling of maximum proton energy and total beam energy content at ultra-high intensities of ∼1021 W cm−2 was investigated, with the interplay between target thickness and laser pre-pulse found to be a key factor. While the maximum proton energies observed were maximised for μm-thick targets, the total proton energy content was seen to peak for thinner, 500 nm, foils. The total proton beam energy reached up to 440 mJ (a conversion efficiency of 4%), marking a significant step forward for many laser-driven ion applications. The experimental results are supported by hydrodynamic and particle-in-cell simulations.
Nature Communications | 2016
S. Kar; H. Ahmed; R. Prasad; M. Cerchez; S. Brauckmann; Bastian Aurand; Giada Cantono; P. Hadjisolomou; Ciaran Lewis; Andrea Macchi; G. Nersisyan; A. P. L. Robinson; Anna Marie Schroer; Marco Swantusch; Matthew Zepf; O. Willi; M. Borghesi
All-optical approaches to particle acceleration are currently attracting a significant research effort internationally. Although characterized by exceptional transverse and longitudinal emittance, laser-driven ion beams currently have limitations in terms of peak ion energy, bandwidth of the energy spectrum and beam divergence. Here we introduce the concept of a versatile, miniature linear accelerating module, which, by employing laser-excited electromagnetic pulses directed along a helical path surrounding the laser-accelerated ion beams, addresses these shortcomings simultaneously. In a proof-of-principle experiment on a university-scale system, we demonstrate post-acceleration of laser-driven protons from a flat foil at a rate of 0.5 GeV m−1, already beyond what can be sustained by conventional accelerator technologies, with dynamic beam collimation and energy selection. These results open up new opportunities for the development of extremely compact and cost-effective ion accelerators for both established and innovative applications.
Applied Physics Letters | 2009
A. S. Pirozhkov; I. W. Choi; J. H. Sung; Soo-Keun Lee; T. J. Yu; T. M. Jeong; I. J. Kim; N. Hafz; C. M. Kim; K. H. Pae; Y.‐C. Noh; D.‐K. Ko; A. P. L. Robinson; P. S. Foster; S. Hawkes; M. Streeter; Ch. Spindloe; P. McKenna; D. C. Carroll; Claes-Göran Wahlström; M. Zepf; D. Adams; B. Dromey; K. Markey; S. Kar; Y. T. Li; M. H. Xu; H. Nagatomo; M. Mori; Akifumi Yogo
Using three different laser systems, we demonstrate a convenient and simple plasma based diagnostic of the contrast of high-power short-pulse lasers. The technique is based on measuring the specular reflectivity from a solid target. The reflectivity remains high even at relativistic intensities above 10(19) W/cm(2) in the case of a high-contrast prepulse-free laser. On the contrary, the specular reflectivity drops with increasing intensities in the case of systems with insufficient contrast due to beam breakup and increased absorption caused by preplasma.