E.L. Clark
Imperial College London
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Featured researches published by E.L. Clark.
Physics of Plasmas | 1999
P.A. Norreys; M. I. K. Santala; E.L. Clark; Matthew Zepf; I. Watts; F. N. Beg; K. Krushelnick; M. Tatarakis; A. E. Dangor; X. Fang; Paul Graham; T. McCanny; R. P. Singhal; K.W.D. Ledingham; Alan Creswell; D.C.W. Sanderson; Joseph Magill; A. Machacek; J. S. Wark; R. Allott; B. Kennedy; D. Neely
Novel measurements of electromagnetic radiation above 10 MeV are presented for ultra intense laser pulse interactions with solids. A bright, highly directional source of γ rays was observed directly behind the target. The γ rays were produced by bremsstrahlung radiation from energetic electrons generated during the interaction. They were measured using the photoneutron reaction [63Cu(γ,n)62Cu] in copper. The resulting activity was measured by coincidence counting the positron annihilation γ rays which were produced from the decay of 62Cu. New measurements of the bremsstrahlung radiation at 1019 W cm−2 are also presented.
Applied Physics Letters | 2001
M. I. K. Santala; Matthew Zepf; F. N. Beg; E.L. Clark; A. E. Dangor; K. Krushelnick; M. Tatarakis; I. Watts; K.W.D. Ledingham; T. McCanny; I. Spencer; A. Machacek; R. Allott; Robert J. Clarke; P.A. Norreys
Nuclear activation has been observed in materials exposed to the ablated plasma generated from high intensity laser–solid interactions (at focused intensities up to 2×1019 W/cm2) and is produced by protons having energies up to 30 MeV. The energy spectrum of the protons is determined from these activation measurements and is found to be consistent with other ion diagnostics. The possible development of this technique for “table-top” production of radionuclides for medical applications is also discussed.
Physics of Plasmas | 2000
K. Krushelnick; E.L. Clark; Matthew Zepf; J.R. Davies; F. N. Beg; A. Machacek; M. I. K. Santala; M. Tatarakis; I. Watts; P.A. Norreys; A. E. Dangor
Energetic protons up to 30 MeV have been measured from high intensity laser interactions (⩽5×1019 W/cm2) with solid density plasmas. Up to 1012 protons (> 2 MeV) were observed at the rear of thin aluminum foil targets and measurements of their angular deflection were made. Similar energies were measured from ions produced from the front of the foils. Nuclear activation and track detector measurements suggest that the protons measured at the rear originate from the front surface of the target and are bent by large magnetic fields that exist in the plasma interior, which are likely generated by a laser-produced beam of fast electrons.
Physics of Plasmas | 2002
M. Tatarakis; A. Gopal; I. Watts; F. N. Beg; A. E. Dangor; K. Krushelnick; U. Wagner; P.A. Norreys; E.L. Clark; Matthew Zepf; R. G. Evans
Measurements of magnetic fields generated during ultrahigh intensity (>1019 W cm−2), short pulse (0.7–1 ps) laser–solid target interaction experiments are reported. An innovative method is used and the results are compared with particle-in-cell simulations. It is shown that polarization measurements of the self-generated harmonics of the laser can provide a convenient method for diagnosing the magnetic field—and that the experimental measurements indicate the existence of peak fields greater than 340 MG and below 460 MG at such high intensities. In particular, the observation of the X-wave cutoffs and the observed induced ellipticity of the harmonics can provide a reliable method for measuring these fields. These observations are important for evaluating the use of intense lasers in various potential applications and perhaps for understanding the complex physics of exotic astrophysical objects such as neutron stars.
IEEE Transactions on Plasma Science | 2000
K. Krushelnick; E.L. Clark; R. Allott; F. N. Beg; C. Danson; A. Machacek; V. Malka; Z. Najmudin; D. Neely; P.A. Norreys; M.R. Salvati; M. I. K. Santala; M. Tatarakis; I. Watts; Matthew Zepf; A. E. Dangor
The possibility of using high-intensity laser-produced plasmas as a source of energetic ions for heavy ion accelerators is addressed. Experiments have shown that neon ions greater than 6 MeV can be produced from gas jet plasmas, and well-collimated proton beams greater than 20 MeV have been produced from high intensity laser solid interactions. The proton beams from the back of thin targets appear to be more collimated and reproducible than are high-energy ions generated in the ablated plasma at the front of the target and may be more suitable for ion injection applications. Lead ions have been produced at energies up to 430 MeV.
Applied Physics Letters | 2002
R.D. Edwards; M.A. Sinclair; T.J. Goldsack; K. Krushelnick; F. N. Beg; E.L. Clark; A. E. Dangor; Z. Najmudin; M. Tatarakis; B. Walton; Matthew Zepf; K.W.D. Ledingham; I. Spencer; P.A. Norreys; R. J. Clarke; R. Kodama; Y. Toyama; M. Tampo
The application of high intensity laser-produced gamma rays is discussed with regard to picosecond resolution deep-penetration radiography. The spectrum and angular distribution of these gamma rays is measured using an array of thermoluminescent detectors for both an underdense (gas) target and an overdense (solid) target. It is found that the use of an underdense target in a laser plasma accelerator configuration produces a much more intense and directional source. The peak dose is also increased significantly. Radiography is demonstrated in these experiments and the source size is also estimated.
Physics of Plasmas | 2001
Matthew Zepf; E.L. Clark; K. Krushelnick; F. N. Beg; C. Escoda; A. E. Dangor; M. I. K. Santala; M. Tatarakis; I. F. Watts; P.A. Norreys; Robert J. Clarke; J. R. Davies; M.A. Sinclair; R.D. Edwards; T.J. Goldsack; I. Spencer; K.W.D. Ledingham
The generation of MeV electron and ion beams using lasers with intensities of up to 1020 W cm−2 is reported. Intense ion beams with high energies (up to 40 MeV and to 3×1012 protons >5 MeV) are observed. The properties of these particle beams were measured in considerable detail and the results are compared to current theoretical explanations for their generation.
Physics of Plasmas | 2004
K. L. Lancaster; Stefan Karsch; H. Habara; F. N. Beg; E.L. Clark; R. R. Freeman; M.H. Key; J.A. King; R. Kodama; K. Krushelnick; K.W.D. Ledingham; P. McKenna; C. D. Murphy; P. A. Norreys; R. Stephens; C. Stoeckl; Y. Toyama; M.S. Wei; Matthew Zepf
Investigations of 7Li(p,n)7Be reactions using Cu and CH primary and LiF secondary targets were performed using the VULCAN laser [C.N. Danson et al., J. Mod. Opt. 45, 1653 (1997)] with intensities up to 3×1019 W cm−2. The neutron yield was measured using CR-39 plastic track detector and the yield was up to 3×108 sr−1 for CH primary targets and up to 2×108 sr−1 for Cu primary targets. The angular distribution of neutrons was measured at various angles and revealed a relatively anisotropic neutron distribution over 180° that was greater than the error of measurement. It may be possible to exploit such reactions on high repetition, table-top lasers for neutron radiography.
Review of Scientific Instruments | 2002
P. McKenna; K.W.D. Ledingham; I. Spencer; T. McCany; R. P. Singhal; C. Ziener; P. S. Foster; E. J. Divall; C. J. Hooker; D. Neely; A. J. Langley; R. J. Clarke; P.A. Norreys; K. Krushelnick; E.L. Clark
A comprehensive characterization of experimental parameters in a study of proton acceleration by short-pulse laser–solid interactions at intensities up to 1019 W cm−2 is reported. Laser pulse and prepulse conditions were measured, with a contrast ratio of the order of 10−6 obtained. The focused laser intensity was experimentally calibrated using a time-of-flight spectrometer to resolve the stages of ionization of a target gas. By comparing the measured ion yields with predictions of an atomic tunneling ionization model a factor of 1.5 uncertainty in the focused intensity was determined. Drive mechanisms for mounting solid targets with thickness in the range of 0.2 to 125 μm have been developed for use with high-repetition rate lasers. A retro-focus imaging system has also been implemented to position the target relative to the laser focus. The techniques have been applied to study proton acceleration as a function of various laser and target parameters. Measurements of the energy distribution of protons a...
Physics of Plasmas | 2003
Z. Najmudin; K. Krushelnick; M. Tatarakis; E.L. Clark; C. Danson; Victor Malka; D. Neely; M. I. K. Santala; A. E. Dangor
Experiments have been performed using high power laser pulses (up to 50 TW) focused into underdense helium plasmas (ne⩽5×1019 cm−3). Using shadowgraphy, it is observed that the laser pulse can produce irregular density channels, which exhibit features such as long wavelength hosing and “sausage-like” self-focusing instabilities. This phenomenon is a high intensity effect and the characteristic period of oscillation of these instabilities is typically found to correspond to the time required for ions to move radially out of the region of highest intensity.