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23587 documents, page 1 of 2359

FLASH.

Feldhaus, J.; Schreiber, S.; Faatz, B.; Honkavaara, K.; Vogt, M.; Kammering, R.; Klose, K.; Hopf, P.; Grün, C.; Brinkmann, A.; Treusch, R.; Düsterer, S.; Tiedtke, K.; Toleikis, S.; Brenner, G.;... (2012)

Research Opportunities at European XFEL

Bressler, Christian (2015)

Gamma-Ray Blazars within the First 2 Billion Years

Ackermann, Markus; Ajello, M.; Bloom, E. D.; Rando, R.; Rani, B.; Razzano, M.; Razzaque, S.; Reimer, A.; Reimer, O.; Romani, R. W.; Sgrò, C.; Simone, D.; Siskind, E. J.; Bonino, R.; Spada, F.;... (2017)
The detection of high-redshift ($z\,\gt 3$) blazars enables the study of the evolution of the most luminous relativistic jets over cosmic time. More importantly, high-redshift blazars tend to host massive black holes and can be used to constrain the space density of heavy black holes in the early universe. Here, we report the first detection with the Fermi-Large Area Telescope of five γ-ray-emitting blazars beyond z = 3.1, more distant than any blazars previously detected in γ-rays. Among the...

Searches for direct pair production of third generation squarks with the ATLAS detector

Usai, Giulio; ATLAS Collaboration (2014)
Naturalness arguments for weak-scale supersymmetry favour supersymmetric partners of the third generation quarks with masses not too far from those of their Standard Model counterparts. Top or bottom squarks with masses less than a few hundred GeV can also give rise to direct pair production rates at the LHC that can be observed in the data sample recorded by the ATLAS detector. This note presents recent ATLAS results from searches for direct stop and sbottom pair production.

Investigating the Key Parameters of a Staged Laser- and Particle Driven Plasma Wakefield Accelerator Experiment

Heinemann, Thomas; Aßmann, Ralph; Schramm, Ulrich; Zarini, Omid; Couperus, Jurjen; Hidding, Bernhard; Irman, Arie; Knetsch, Alexander; Köhler, Alexander; Kononenko, Olena; Kurz, Thomas; Martinez de la Ossa, Alberto (2017)
Plasma wakefield accelerators can be driven by either a powerful laser pulse (LWFA) or a high-current charged particle beam (PWFA). A plasma accelerator combining both schemes consists of a LWFA providing an electron beam which subsequently drives a PWFA in the highly nonlinear regime. This scenario explicitly makes use of the advantages unique to each method, particularly exploiting the capabilities of PWFA schemes to provide high-brightness beams, while the LWFA stage inherently fulfils the...