S. Cipiccia
University of Strathclyde
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Featured researches published by S. Cipiccia.
Scientific Reports | 2017
G. Vieux; S. Cipiccia; D. W. Grant; Nuno Lemos; P. Grant; C. Ciocarlan; B. Ersfeld; Min Sup Hur; P. Lepipas; G. G. Manahan; G. Raj; D. Reboredo Gil; Anna Subiel; G. H. Welsh; S. M. Wiggins; S. R. Yoffe; J. Farmer; Constantin Aniculaesei; E. Brunetti; X. Yang; R. Heathcote; G. Nersisyan; Ciaran Lewis; A. Pukhov; João Dias; D. A. Jaroszynski
Raman amplification arising from the excitation of a density echelon in plasma could lead to amplifiers that significantly exceed current power limits of conventional laser media. Here we show that 1–100 J pump pulses can amplify picojoule seed pulses to nearly joule level. The extremely high gain also leads to significant amplification of backscattered radiation from “noise”, arising from stochastic plasma fluctuations that competes with externally injected seed pulses, which are amplified to similar levels at the highest pump energies. The pump energy is scattered into the seed at an oblique angle with 14 J sr−1, and net gains of more than eight orders of magnitude. The maximum gain coefficient, of 180 cm−1, exceeds high-power solid-state amplifying media by orders of magnitude. The observation of a minimum of 640 J sr−1 directly backscattered from noise, corresponding to ≈10% of the pump energy in the observation solid angle, implies potential overall efficiencies greater than 10%.
Plasma Physics and Controlled Fusion | 2014
R. Assmann; R. Bingham; T. Bohl; C. Bracco; B. Buttenschön; A. Butterworth; A. Caldwell; S. Chattopadhyay; S. Cipiccia; Eduard Feldbaumer; Ricardo Fonseca; B. Goddard; M. Gross; O. Grulke; E. Gschwendtner; J. Holloway; C. Huang; D. A. Jaroszynski; S. Jolly; P. Kempkes; Nelson Lopes; K. V. Lotov; J. Machacek; S. Mandry; J. W. McKenzie; M. Meddahi; B. L. Militsyn; N. Moschuering; P. Muggli; Z. Najmudin
New acceleration technology is mandatory for the future elucidation of fundamental particles and their interactions. A promising approach is to exploit the properties of plasmas. Past research has focused on creating large-amplitude plasma waves by injecting an intense laser pulse or an electron bunch into the plasma. However, the maximum energy gain of electrons accelerated in a single plasma stage is limited by the energy of the driver. Proton bunches are the most promising drivers of wakefields to accelerate electrons to the TeV energy scale in a single stage. An experimental program at CERN—the AWAKE experiment—has been launched to study in detail the important physical processes and to demonstrate the power of proton-driven plasma wakefield acceleration. Here we review the physical principles and some experimental considerations for a future proton-driven plasma wakefield accelerator.
conference on lasers and electro optics | 2010
S. M. Wiggins; Richard P. Shanks; R. C. Issac; G. H. Welsh; M. P. Anania; E. Brunetti; G. Vieux; S. Cipiccia; B. Ersfeld; M. R. Islam; R. T. L. Burgess; G. G. Manahan; Constantin Aniculaesei; W. A. Gillespie; A. M. MacLeod; D. A. Jaroszynski
Very stable, high quality electron beams (current ∼ 10 kA, energy spread < 1%, emittance ∼ 1π mm mrad) have been generated in a laser-plasma accelerator driven by 25 TW femtosecond laser pulses.
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.
Journal of Applied Physics | 2012
S. Cipiccia; S. M. Wiggins; Richard P. Shanks; M. R. Islam; G. Vieux; R. C. Issac; E. Brunetti; B. Ersfeld; G. H. Welsh; M. P. Anania; D. Maneuski; Nuno Lemos; R. A. Bendoyro; Pattathil Rajeev; P. S. Foster; N. Bourgeois; T. Ibbotson; P. A. Walker; V. O’Shea; João Dias; D. A. Jaroszynski
The laser driven plasma wakefield accelerator is a very compact source of high energy electrons. When the quasi-monoenergetic beam from these accelerators passes through dense material, high energy bremsstrahlung photons are emitted in a collimated beam with high flux. We show how a source based on this emission process can produce more than 109 photons per pulse with a mean energy of 10 MeV. We present experimental results that show the feasibility of this method of producing high energy photons and compare the experimental results with GEANT4 Montecarlo simulations, which also give the scaling required to evaluate its suitability as method to produce radioisotopes via photo-nuclear reactions or for imaging applications.
Physics in Medicine and Biology | 2014
Anna Subiel; V Moskvin; G. H. Welsh; S. Cipiccia; David Reboredo; Philip M. Evans; Mike Partridge; Colleen DesRosiers; M. P. Anania; A. Cianchi; A. Mostacci; E. Chiadroni; D. Di Giovenale; F. Villa; R. Pompili; M. Ferrario; M. Belleveglia; G. Di Pirro; G. Gatti; C. Vaccarezza; B. Seitz; R. Isaac; E. Brunetti; S. M. Wiggins; B. Ersfeld; M. R. Islam; M S Mendonca; Annette Sorensen; Marie Boyd; D. A. Jaroszynski
Very high energy electrons (VHEE) in the range from 100-250 MeV have the potential of becoming an alternative modality in radiotherapy because of their improved dosimetry properties compared with MV photons from contemporary medical linear accelerators. Due to the need for accurate dosimetry of small field size VHEE beams we have performed dose measurements using EBT2 Gafchromic® film. Calibration of the film has been carried out for beams of two different energy ranges: 20 MeV and 165 MeV from conventional radio frequency linear accelerators. In addition, EBT2 film has been used for dose measurements with 135 MeV electron beams produced by a laser-plasma wakefield accelerator. The dose response measurements and percentage depth dose profiles have been compared with calculations carried out using the general-purpose FLUKA Monte Carlo (MC) radiation transport code. The impact of induced radioactivity on film response for VHEEs has been evaluated using the MC simulations. A neutron yield of the order of 10(-5) neutrons cm(-2) per incident electron has been estimated and induced activity due to radionuclide production is found to have a negligible effect on total dose deposition and film response. Neutron and proton contribution to the equivalent doses are negligible for VHEE. The study demonstrates that EBT2 Gafchromic film is a reliable dosimeter that can be used for dosimetry of VHEE. The results indicate an energy-independent response of the dosimeter for 20 MeV and 165 MeV electron beams and has been found to be suitable for dosimetry of VHEE.
New Journal of Physics | 2015
M. R. Islam; E. Brunetti; Richard P. Shanks; B. Ersfeld; R. C. Issac; S. Cipiccia; M. P. Anania; G. H. Welsh; S. M. Wiggins; Adam Noble; R. A. Cairns; G. Raj; D. A. Jaroszynski
The laser–plasma wakefield accelerator is a compact source of high brightness, ultra-short duration electron bunches. Self-injection occurs when electrons from the background plasma gain sufficient momentum at the back of the bubble-shaped accelerating structure to experience sustained acceleration. The shortest duration and highest brightness electron bunches result from self-injection close to the threshold for injection. Here we show that in this case injection is due to the localized charge density build-up in the sheath crossing region at the rear of the bubble, which has the effect of increasing the accelerating potential to above a critical value. Bunch duration is determined by the dwell time above this critical value, which explains why single or multiple ultra-short electron bunches with little dark current are formed in the first bubble. We confirm experimentally, using coherent optical transition radiation measurements, that single or multiple bunches with femtosecond duration and peak currents of several kiloAmpere, and femtosecond intervals between bunches, emerge from the accelerator.
New Journal of Physics | 2014
G. G. Manahan; E. Brunetti; Constantin Aniculaesei; M. P. Anania; S. Cipiccia; M. R. Islam; D. W. Grant; Anna Subiel; Richard P. Shanks; R. C. Issac; G. H. Welsh; S. M. Wiggins; D. A. Jaroszynski
Electron beams from laser-plasma wakefield accelerators have low transverse emittance, comparable to those from conventional radio frequency accelerators, which highlights their potential for applications, many of which will require the use of quadrupole magnets for optimal electron beam transport. We report on characterizing electron bunches where double bunches are observed under certain conditions. In particular, we present pepper-pot measurements of the transverse emittance of 120–200 MeV laser wakefield electron bunches after propagation through a triplet of permanent quadrupole magnets. It is shown that the normalized emittance at source can be as low as 1 π mm mrad (resolution limited), growing by about five times after propagation through the quadrupoles due to beam energy spread. The inherent energy-dependence of the magnets also enables detection of double electron bunches that could otherwise remain unresolved, providing insight into the self-injection of multiple bunches. The combination of quadrupoles and pepper-pot, in addition, acts as a diagnostic for the alignment of the magnetic triplet.
Applied Physics Letters | 2014
M. P. Anania; E. Brunetti; S. M. Wiggins; D. W. Grant; G. H. Welsh; R. C. Issac; S. Cipiccia; Richard P. Shanks; G. G. Manahan; Constantin Aniculaesei; S.B. van der Geer; M.J. de Loos; M.W. Poole; B. J. A. Shepherd; J.A. Clarke; W. A. Gillespie; A. M. MacLeod; D. A. Jaroszynski
Narrow band undulator radiation tuneable over the wavelength range of 150–260 nm has been produced by short electron bunches from a 2 mm long laser plasma wakefield accelerator based on a 20 TW femtosecond laser system. The number of photons measured is up to 9 × 106 per shot for a 100 period undulator, with a mean peak brilliance of 1 × 1018 photons/s/mrad2/mm2/0.1% bandwidth. Simulations estimate that the driving electron bunch r.m.s. duration is as short as 3 fs when the electron beam has energy of 120–130 MeV with the radiation pulse duration in the range of 50–100 fs.
Optics Express | 2014
S. Cipiccia; Fabio A. Vittoria; Maria Weikum; Alessandro Olivo; D. A. Jaroszynski
Interest in phase contrast imaging methods based on electromagnetic wave coherence has increased significantly recently, particularly at X-ray energies. This is giving rise to a demand for effective simulation methods. Coherent imaging approaches are usually based on wave optics, which require significant computational resources, particularly for producing 2D images. Monte Carlo (MC) methods, used to track individual particles/photons for particle physics, are not considered appropriate for describing coherence effects. Previous preliminary work has evaluated the possibility of incorporating coherence in Monte Carlo codes. However, in this paper, we present the implementation of refraction in a model that is based on time of flight calculations and the Huygens-Fresnel principle, which allow reproducing the formation of phase contrast images in partially and fully coherent experimental conditions. The model is implemented in the FLUKA Monte Carlo code and X-ray phase contrast imaging simulations are compared with experiments and wave optics calculations.