thin wire targets Phys. Plasmas 20 , 062703 (2013) G. Hoffmeister, C. Bellei, K. Harres, D. Ivanov, D. Kraus, A. Pelka, B. Rethfeld, G. Schaumann, M. Roth Influence of fs-laser desorption on target normal [...] Cohen, J. Kim, P. Neumayer, M. Roth, B. G. Logan Initial experimental evidence of self-collimation of target-normal-sheath-accelerated proton beam in a stack of conducting foils Phys. Plasmas 20 , 083111 (2013) [...] Novikov, A. Grushin, A. Blazevic and J.A. Maruhn 2D radiation-hydrodynamics modeling of laser-plasma targets for ion stopping measurements High Energy Density Physics 9 , pp. 158-166 (2013) L. Tkachenko, I

the final p-process abundance are unstable. Since there is no chance of producing any reasonable targets from unstable nuclei of interest, it is proposed to determine the desired reaction rates in inverse [...] owing to high revolution frequencies in the ring, to the windowless pure internal hydrogen or helium targets, and to nearly unity detection efficiency of reaction products. Furthermore, electron cooling of [...] high-intensity 21 Ne beam will be stored in the ESR and intersected with the internal hydrogen-gas jet target. The state of interest will be identified by measuring the energies and angles of the emitted in

repetition rate, particularly using gaseous targets. Fundamental research into innovative mechanisms for accelerating electrons and ions from gaseous targets must be carried out in order to increase the [...] requires targets with a relatively low electron density in the range of 10 18 - 10 19 cm -3 , but with a large spatial expansion in the range of several millimeters. In order to realize such a target with [...] Positions Research Assistant (all genders) "Multi-MeV laser accelerated particle beams from a gas jet target" At the Institute LP2IB, 19 Chemin du Solarium, F-33170 Gradignan, France a position is open in the

deviation d as a fraction of the nominal (reference) value. The “path length” is from the Super-FRS target. 1st-order transfer matrix elements at the focal planes in the Pre-Separator Matrix element FPF1

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

South tower bottom EH.1.013 1571 South tower top EH.2.013 1849 Z6 control room EH.1.002 1850 or 2286 Target area EH.1.011 1569 Visar EH.2.011 2612 nhelix room EH.1.010 1570 HHT Cave Work station Building/Room

Winters, and N. Winters Evidence for ultra-fast heating in intense-laser irradiated reduced-mass targets Phys. of Plasmas 19 , 122708 (2012) C. Niemann, C. G. Constantin, D. B. Schaeffer, A. Tauschwitz [...] Zielbauer, P. McKenna, and D. Neely Multi-pulse enhanced laser ion acceleration using plasma half cavity targets Appl. Phys. Lett. 101 , 024101 (2012) E. Siminos, M. Grech, S. Skupin, T. Schlegel, and V.T. Tikhonchuk [...] Sancho, A. Shutov, R. Schmidt, and A.R. Piriz Impact of high energy high intensity proton beams on targets: Case studies for Super Proton Synchrotron and Large Hadron Collider Phys. Rev. ST Accel. and Beams

accelerator UNILAC and fired at a target containing plutonium-244, resulting in the formation of a few flerovium atoms per day. The formed flerovium atoms recoiled from the target into the gas-filled separator [...] International and interdisciplinary collaboration as the key to understanding The exotic plutonium target material for the production of the flerovium was provided in part by Lawrence Livermore National

time in fusion reactions of 70 Zn (proton number 30) projectiles with 208 Pb (proton number 82) targets. The formed compound nucleus 278 112 deexcites by emitting a neutron and results in the isotope 277

neutron-rich cadmium nuclei were produced by projectile fission of uranium nuclei on a beryllium target and identified by the BigRIPS separator. The gamma rays emitted following the decay of isomeric states