Entity

Time filter

Source Type

Eindhoven, Netherlands

Poplau G.,University of Rostock | Van Rienen U.,University of Rostock | Van Der Geer S.B.,Pulsar Physics | De Loos M.J.,TU Eindhoven
IPAC 2011 - 2nd International Particle Accelerator Conference | Year: 2011

Efficient and accurate space-charge computations are essential for the design of high-brightness charged particle sources. Recently a new adaptive meshing strategy based on multigrid was implemented in GPT and the capabilities were demonstrated. This new meshing scheme uses the solution of an intermediate step in the multigrid algorithm itself to define optimal mesh line positions. In this paper we discuss further developments of this adaptive meshing strategy. We compare the new algorithm with the meshing scheme of GPT where the mesh line positions are based upon the projected charge density. Copyright © 2011 by IPAC'11/EPS-AG. Source


D'Arcy R.T.P.,University College London | Jolly S.,University College London | Muratori B.D.,Daresbury Laboratory | Jones J.K.,Daresbury Laboratory | Van Der Geer B.,Pulsar Physics
IPAC 2012 - International Particle Accelerator Conference 2012 | Year: 2012

EMMA (Electron Machine with Many Applications) is a prototype non-scaling Fixed-Field Alternating Gradient (ns-FFAG) accelerator whose construction at Daresbury Laboratory, UK, was completed in the autumn of 2010. The energy recovery linac ALICE [1] will serve as an injector for EMMA, within an energy range of 10 to 20 MeV. The injection line consists of a symmetric 30o dogleg to extract the beam from ALICE, a matching section and a tomography section for transverse emittance measurements. This is followed by a transport section to the injection point of the EMMA ring. The ring is composed of 42 cells, each containing one focusing and one defocusing quadrupole. Commissioning of the EMMA ring started in late 2010. A number of different injection energy and bunch charge configurations are planned; for some the effects of spacecharge may be significant. It is therefore necessary to model the electron beam transport in the injection line and ring using a code capable of both calculating the effect of and compensating for space-charge. Therefore the General Particle Tracer (GPT) code [2] has been used. A range of injection beam parameters have been modelled for comparison with experimental results. Copyright © 2012 by IEEE. Source


Anania M.P.,University of Strathclyde | Brunetti E.,University of Strathclyde | Cipiccia S.,University of Strathclyde | Clark D.,University of Strathclyde | And 13 more authors.
IPAC 2010 - 1st International Particle Accelerator Conference | Year: 2010

Recent progress in developing laser-plasma accelerators is raising the possibility of a compact coherent radiation source that could be housed in a medium sized university department. Furthermore, since the duration of electron bunches from laser-plasma wakefield accelerators (LWFAs) is determined by the relativistic plasma wavelength, radiation sources based on these accelerators can produce pulses with femtosecond durations. Beam properties from laser-plasma accelerators have been traditionally thought of as not being of sufficient quality to produce amplification. However, our work shows this not to be the case. Here, we present a study of the beam characteristics of a laser-plasma accelerator and the compact ALPHA-X (Advanced Laser Plasma High-energy Accelerators towards X-rays) FEL. We discuss the implementation of a focussing system consisting of a triplet of permanent magnet quadrupoles and a triplet of electromagnetic quadrupoles [1, 2]. The design of these devices has been carried out using the GPT (General Particle Tracer) code [3, 4], which considers space charge effects and allows a realistic estimate of electron beam properties along the beam line. We will present a study of the influence of beam transport on FEL action in the undulator, paying particular attention to bunch dispersion in the undulator. This is an important step for developing a compact synchrotron source or a SASE free-electron laser [5, 6]. Source


Anania M.P.,University of Strathclyde | Anania M.P.,National Institute of Nuclear Physics, Italy | Brunetti E.,University of Strathclyde | Wiggins S.M.,University of Strathclyde | And 15 more authors.
Applied Physics Letters | Year: 2014

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. © 2014 Author(s). Source


Mancini G.F.,Ecole Polytechnique Federale de Lausanne | Mansart B.,Ecole Polytechnique Federale de Lausanne | Pagano S.,Ecole Polytechnique Federale de Lausanne | Van Der Geer B.,Pulsar Physics | And 2 more authors.
Optics InfoBase Conference Papers | Year: 2014

We report the design and implementation of a table-top apparatus for Ultrafast Electron Diffraction capable of experiments in both transmission and reflection geometry with electron packets of 30 keV. The electron pulse properties in terms of charge per pulse, transverse spot-size and temporal duration on the sample can be controlled with the use of radiofrequency technology combined with a set of electron optics. The characterization of the beam is performed via a lightelectrons cross-correlation experiment and we demonstrate an overall temporal resolution around 300 fs for bunches containing up to 105 electrons at 20 kHz repetition rate. © 2014 OSA. Source

Discover hidden collaborations