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Dive into the research topics where D. C. Carroll is active.

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Featured researches published by D. C. Carroll.


Laser and Particle Beams | 2008

Effects of front surface plasma expansion on proton acceleration in ultraintense laser irradiation of foil targets

P. McKenna; D. C. Carroll; Olle Lundh; F. Nürnberg; K. Markey; S. Bandyopadhyay; D. Batani; R. G. Evans; R. Jafer; S. Kar; D. Neely; D. Pepler; M. N. Quinn; R. Redaelli; Markus Roth; C.-G. Wahlstrom; Xiaohui Yuan; Matthew Zepf

The properties of beams of high energy protons accelerated during ultraintense, picosecond laser-irradiation of thin foil targets are investigated as a function of preplasma expansion at the target front surface. Significant enhancement in the maximum proton energy and laser-to-proton energy conversion efficiency is observed at optimum preplasma density gradients, due to self-focusing of the incident laser pulse. For very long preplasma expansion, the propagating laser pulse is observed to filament, resulting in highly uniform proton beams, but with reduced flux and maximum energy.


Physical Review Letters | 2008

Dynamic Control of Laser-Produced Proton Beams

S. Kar; K. Markey; P.T. Simpson; C. Bellei; J. S. Green; S. R. Nagel; S. Kneip; D. C. Carroll; B. Dromey; L. Willingale; E. L. Clark; P. McKenna; Z. Najmudin; K. Krushelnick; P. A. Norreys; R. J. Clarke; D. Neely; M. Borghesi; M. Zepf

The emission characteristics of intense laser driven protons are controlled using ultrastrong (of the order of 10(9) V/m) electrostatic fields varying on a few ps time scale. The field structures are achieved by exploiting the high potential of the target (reaching multi-MV during the laser interaction). Suitably shaped targets result in a reduction in the proton beam divergence, and hence an increase in proton flux while preserving the high beam quality. The peak focusing power and its temporal variation are shown to depend on the target characteristics, allowing for the collimation of the inherently highly divergent beam and the design of achromatic electrostatic lenses.


Plasma Physics and Controlled Fusion | 2011

Refluxing of fast electrons in solid targets irradiated by intense, picosecond laser pulses

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

High efficiency proton beam generation through target thickness control in femtosecond laser-plasma interactions

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.


Applied Physics Letters | 2009

Diagnostic of laser contrast using target reflectivity

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.


Plasma Physics and Controlled Fusion | 2007

Low- and medium-mass ion acceleration driven by petawatt laser plasma interactions

P. McKenna; Filip Lindau; Olle Lundh; D. C. Carroll; Rosemary Clarke; Kwd Ledingham; T. McCanny; D. Neely; A. P. L. Robinson; L. Robson; P.T. Simpson; Claes-Göran Wahlström; M. Zepf

An experimental investigation of low- and medium-mass ion acceleration from resistively heated thin foil targets, irradiated by picosecond laser pulses at intensities up to 5 × 1020 W cm−2, is reported. It is found that the spectral distributions of ions, up to multi-MeV/nucleon energies, accelerated from the rear surface of the target are broadly consistent with previously reported measurements made at intensities up to 5 × 1019 W cm−2. Properties of the backward-directed beams of ions accelerated from the target front surface are also measured, and it is found that, compared with the rear surface, higher ion numbers and charges, and similar ion energies are produced. Additionally, the scaling of the maximum ion energy as a function of ion charge and laser intensity are measured and compared with the predictions of a numerical model.


New Journal of Physics | 2015

Proton acceleration enhanced by a plasma jet in expanding foils undergoing relativistic transparency

Haydn Powell; M. King; Robert Gray; D. A. MacLellan; Bruno Gonzalez-Izquierdo; Luca C. Stockhausen; George Hicks; Nicholas Dover; Dean Rusby; D. C. Carroll; H. Padda; R. Torres; S. Kar; R. J. Clarke; I. O. Musgrave; Z. Najmudin; M. Borghesi; D. Neely; P. McKenna

Ion acceleration driven by the interaction of an ultraintense (2x10^20 Wcm^-2) laser pulse with an ultrathin (40nm) foil target is experimentally and numerically investigated. Protons accelerated by sheath fields and via laser radiation pressure are angularly separated and identified based on their directionality and signature features (e.g. transverse instabilities) in the measured spatial-intensity distribution. A low divergence, high energy proton component is also detected when the heated target electrons expand and the target becomes relativistically transparent during the interaction. 2D and 3D particle-in-cell (PIC) simulations indicate that under these conditions a plasma jet is formed at the target rear, supported by a self-generated azimuthal magnetic field, which extends into the expanded layer of sheath-accelerated protons. Electrons trapped within this jet are directly accelerated to super-thermal energies by the portion of the laser pulse transmitted through the target. The resulting streaming of the electrons into the ion layers enhances the energy of protons in the vicinity of the jet. Through the addition of a controlled prepulse, the maximum energy of these protons is demonstrated experimentally and numerically to be sensitive to the picosecond rising edge prole of the laser pulse.


New Journal of Physics | 2010

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

D. C. Carroll; O. Tresca; R. Prasad; L. Romagnani; P.S. Foster; P. Gallegos; S. Ter-Avetisyan; J. S. Green; Matthew Streeter; Nicholas Dover; C. A. J. Palmer; C. M. Brenner; F.H. Cameron; K. Quinn; J. Schreiber; A. P. L. Robinson; T Baeva; M. N. Quinn; Xiaohui Yuan; Z. Najmudin; M. Zepf; D. Neely; M. Borghesi; P. McKenna

In this study, ion acceleration from thin planar target foils irradiated by ultrahigh-contrast (10 10 ), ultrashort (50fs) laser pulses focused to intensities of 7◊10 20 Wcm 2 is investigated experimentally. Target normal sheath acceleration (TNSA) is found to be the dominant ion acceleration mechanism when the target thickness is >50nm and laser pulses are linearly polarized. Under these conditions, irradiation at normal incidence is found to produce higherenergyions thanobliqueincidenceat35 withrespectto thetargetnormal. 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. 5 Author to whom any correspondence should be addressed.


Applied Physics Letters | 2011

Surface transport of energetic electrons in intense picosecond laser-foil interactions

Robert Gray; Xiaohui Yuan; D. C. Carroll; C. M. Brenner; M. Coury; M. N. Quinn; O. Tresca; B. Zielbauer; B. Aurand; V. Bagnoud; J. Fils; T. Kühl; Xian Lin; Cuncheng Li; Y. T. Li; Markus Roth; D. Neely; P. McKenna

The angular distribution of energetic electrons emitted from thin foil targets irradiated by intense, picosecond laser pulses is measured as a function of laser incidence angle, intensity, and polarization. Although the escaping fast electron population is found to be predominantly transported along the target surface for incidence angles ≥65°, in agreement with earlier work at lower intensities, rear-surface proton acceleration measurements reveal that a significant electron current is also transported longitudinally within the target, irrespective of incident angle. These findings are of interest to many applications of laser-solid interactions, including advanced schemes for inertial fusion energy.


Laser and Particle Beams | 2011

Dependence of laser accelerated protons on laser energy following the interaction of defocused, intense laser pulses with ultra-thin targets

C. M. Brenner; J. S. Green; A. P. L. Robinson; D. C. Carroll; B. Dromey; P. S. Foster; S. Kar; Y. T. Li; K. Markey; C. Spindloe; M. Streeter; M. Tolley; Claes-Göran Wahlström; M.H. Xu; Matthew Zepf; P. McKenna; D. Neely

The scaling of the flux and maximum energy of laser-driven sheath-accelerated protons has been investigated as a function of laser pulse energy in the range of 15-380 mJ at intensities of 10(16)-10(18) W/cm(2). The pulse duration and target thickness were fixed at 40 fs and 25 nm, respectively, while the laser focal spot size and drive energy were varied. Our results indicate that while the maximum proton energy is dependent on the laser energy and laser spot diameter, the proton flux is primarily related to the laser pulse energy under the conditions studied here. Our measurements show that increasing the laser energy by an order of magnitude results in a more than 500-fold increase in the observed proton flux. Whereas, an order of magnitude increase in the laser intensity generated by decreasing the laser focal spot size, at constant laser energy, gives rise to less than a tenfold increase in observed proton flux.

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P. McKenna

University of Strathclyde

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D. Neely

Rutherford Appleton Laboratory

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M. Borghesi

Queen's University Belfast

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S. Kar

Queen's University Belfast

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A. P. L. Robinson

Rutherford Appleton Laboratory

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Xiaohui Yuan

Shanghai Jiao Tong University

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Matthew Zepf

Helmholtz Institute Jena

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J. S. Green

Rutherford Appleton Laboratory

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K. Markey

Rutherford Appleton Laboratory

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