GeV electron beams from a laser-plasma accelerator
Institute of Electrical and Electronics Engineers (IEEE) (2006) 538-539
Measurement of high- Q 2 deep inelastic scattering cross sections with a longitudinally polarised positron beam at HERA
Physics Letters Section B Nuclear Elementary Particle and High Energy Physics 637:4-5 (2006) 210-222
Abstract:
The cross sections for charged and neutral current deep inelastic scattering in e + p collisions with a longitudinally polarised positron beam have been measured using the ZEUS detector at HERA. The results, based on data corresponding to an integrated luminosity of 23.8 pb -1 at sqrt(s) = 318 GeV, are given for both e + p charged current and neutral current deep inelastic scattering for both positive and negative values of the longitudinal polarisation of the positron beam. Single differential cross sections are presented for the kinematic region Q 2 > 200 GeV 2. The measured cross sections are compared to the predictions of the Standard Model. A fit to the data yields σ CC ( PMeasurement of high-Q2 deep inelastic scattering cross sections with a longitudinally polarised positron beam at HERA
Physics Letters B 637 (2006) 210-222
Inverse free electron lasers and laser wakefield acceleration driven by CO2 lasers
Philosophical Transactions of the Royal Society A Mathematical Physical and Engineering Sciences 364:1840 (2006) 611-622
Abstract:
The staged electron laser acceleration (STELLA) experiment demonstrated staging between two laser-driven devices, high trapping efficiency of microbunches within the accelerating field and narrow energy spread during laser acceleration. These are important for practical laser-driven accelerators. STELLA used inverse free electron lasers, which were chosen primarily for convenience. Nevertheless, the STELLA approach can be applied to other laser acceleration methods, in particular, laser-driven plasma accelerators. STELLA is now conducting experiments on laser wakefield acceleration (LWFA). Two novel LWFA approaches are being investigated. In the first one, called pseudo-resonant LWFA, a laser pulse enters a low-density plasma where nonlinear laser/plasma interactions cause the laser pulse shape to steepen, thereby creating strong wakefields. A witness e-beam pulse probes the wakefields. The second one, called seeded self-modulated LWFA, involves sending a seed e-beam pulse into the plasma to initiate wakefield formation. These wakefields are amplified by a laser pulse following shortly after the seed pulse. A second e-beam pulse (witness) follows the seed pulse to probe the wakefields. These LWFA experiments will also be the first ones driven by a COForward jet production in deep inelastic ep scattering and low-x parton dynamics at HERA
Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics 632:1 (2006) 13-26