deviation d as a fraction of the nominal (reference) value. The “path length” is from the Super-FRS target. FHF1 is 7.5 m from the end of the last quadrupole, FHF1QT32. Matrix element FMF1 FMF2 FMF3 FMF4

mit Energien bis 12 GeV um konventionelle und exotische Hadronen mit einem Protonen- oder nuklearen Target zu erzeuge. GlueX nutzt dabei kohärente Bremsstrahlung um linear polarisierte Photonen zu erzeugen

colleagues in India The Bose Institute; Kolkata, India, is in charge of producing the beam catchers in target area. Most probably, India will also produce the power converters for the Super-FRS magnets. Our

Collider proton beam on a copper target J. Appl. Phys. 97 , 083532 (2005) N. A. Tahir, H. Weick, et.al., D. H. H. Hoffmann Calculations of high-power production target and beamdump design for the GSI future [...] Berdiyorov, U. Kunishev, E. Khalmuratov, M. Toshikohonov, M. Kanapathipillai Investigation of PbMg target characteristics by a laser mass-spectrometer Laser Part. Beams 23 , 521 - 526 (2005) D. T. Khoa, [...] J. Lopez Cela, N. Grandjouan, N. A. Tahir, M. C. Serna Moreno, R. F. Portugues, D. H. H. Hoffmann Target design for the cylindircal compression of matter driven by heavy ion beams Nucl. Instrum. Meth. A

charged particles and neutrons stemming from central collisions of 108,112,124,132 Sn on 112,124 Sn target. Figure 1 shows a particle ID plot from the 1st NeuLAND plane, displaying the time of flight over [...] currently located at RIKEN , Japan, was moved within the SAMURAI Area to 30 degrees with respect to the target, see photo below. At this new position, NeuLAND together with a VETO wall in front will take data [...] experiment, studying central collision in several combinations of Sn isotopes beams and Sn isotope targets. On the left side the NeuLAND demonstrator VETO Wall is visible, NeuLAND is standing right behind

opportunities for new paths in electron-ion collision physics. CRYRING@ESR features an electron cooler/target with an electron beam that is adiabatically expanded in the transverse direction. The temperatures

Europe . Performance of PHELIX PHELIX is available for experiments in the PHELIX hall and at the Z6 target station of the UNILAC heavy-ion accelerator, where pulses of laser beam can be delivered, synchronized

Characteristic X-rays generation under the action of femtosecond laser pulses on nano-structured targets Laser and Particle Beams 29 (2), pp. 249-254 (2011) A.R. Piriz, L. Di Lucchio, G. Rodriguez Prieto [...] B. Zielbauer, B. Aurand, J. Fils, T. Kühl, and P. McKenna Refluxing of fast electrons in solid targets irradiated by intense, picosecond laser pulses, Plasma Phys. Control. Fusion 53 , 025007 (2011) C [...] ultraintense laser-proton sources using transverse refluxing of hot electrons in shaped mass-limited targets, Plasma Phys. Control. Fusion 53 , 105008 (2011) X. H. Yuan, D. C. Carroll, M. Coury, R. J. Gray

deviation d as a fraction of the nominal (reference) value. The “path length” is from the Super-FRS target. FLF2 is 4 m from the end of the last quadrupole, FLF2QT32. 1st-order transfer matrix elements at

measured with high experimental resolution storage-ring electron coolers or merged-beams free-electron targets, in particular at low electron-ion collision energies. DR is a two-step process: X q+ +e− → X (q−1)+