4 results on '"Lars Goldberg"'
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2. FLASHForward: Plasma-wakefield accelerator science for high-average-power applications
- Author
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Lucas Schaper, Bernhard Schmidt, Timon Mehrling, F. Marutzky, M. Meisel, Martin Quast, Alexander Knetsch, Ming Zeng, P. Kuang, Lars Goldberg, Matthew Wing, J.-H. Röckemann, Vladyslav Libov, S. Diederichs, B. Foster, S. Schröder, Gabriele Tauscher, B. Sheeran, Jens Osterhoff, M. J. Garland, S. Karstensen, J. Chappell, S. Bohlen, Paul Winkler, A. Aschikhin, P. Pourmoussavi, R. D'Arcy, P. Gonzalez, Kristjan Poder, Gregory J. Boyle, K. Ludwig, S. Wesch, A. Martinez de la Ossa, T. Brümmer, Jan-Patrick Schwinkendorf, and P. Niknejadi
- Subjects
Physics ,Orders of magnitude (power) ,Accelerator Physics (physics.acc-ph) ,RF front end ,General Mathematics ,Nuclear engineering ,General Engineering ,General Physics and Astronomy ,FOS: Physical sciences ,Plasma ,Electron ,Articles ,Plasma acceleration ,Laser ,Linear particle accelerator ,Physics - Plasma Physics ,law.invention ,Plasma Physics (physics.plasm-ph) ,Flash (photography) ,law ,Physics - Accelerator Physics ,ddc:510 - Abstract
Philosophical transactions of the Royal Society of London / A Mathematical, physical and engineering sciences Series A 377(2151), 20180392 - (2019). doi:10.1098/rsta.2018.0392, The FLASHForward experimental facility is a high-performance test-bed for precision plasma wakefield research, aiming to accelerate high-quality electron beams to GeV-levels in a few centimetres of ionized gas. The plasma is created by ionizing gas in a gas cell either by a high-voltage discharge or a high-intensity laser pulse. The electrons to be accelerated will either be injected internally from the plasma background or externally from the FLASH superconducting RF front end. In both cases, the wakefield will be driven by electron beams provided by the FLASH gun and linac modules operating with a 10 Hz macro-pulse structure, generating 1.25 GeV, 1 nC electron bunches at up to 3 MHz micro-pulse repetition rates. At full capacity, this FLASH bunch-train structure corresponds to 30 kW of average power, orders of magnitude higher than drivers available to other state-of-the-art LWFA and PWFA experiments. This high-power functionality means FLASHForward is the only plasma wakefield facility in the world with the immediate capability to develop, explore and benchmark high-average-power plasma wakefield research essential for next-generation facilities. The operational parameters and technical highlights of the experiment are discussed, as well as the scientific goals and high-average-power outlook., Published by Soc., London
- Published
- 2019
- Full Text
- View/download PDF
3. A tunable plasma-based energy dechirper
- Author
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Lars Goldberg, A. Martinez de la Ossa, M. J. Garland, C. Behrens, Timon Mehrling, Lucas Schaper, Alexander Knetsch, S. Bohlen, Kristjan Poder, P. Niknejadi, V. Wacker, Boris Schmidt, S. Wesch, A. Aschikhin, P. Gonzalez, R. D'Arcy, Jens Osterhoff, J.-H. Röckemann, Jan-Patrick Schwinkendorf, Gabriele Tauscher, B. Sheeran, Vladyslav Libov, Charlotte Palmer, S. Schröder, M. J. V. Streeter, and M. Meisel
- Subjects
Accelerator Physics (physics.acc-ph) ,General Physics ,FOS: Physical sciences ,General Physics and Astronomy ,Electron ,01 natural sciences ,Stability (probability) ,Mathematical Sciences ,law.invention ,Engineering ,Affordable and Clean Energy ,law ,Physics::Plasma Physics ,physics.plasm-ph ,0103 physical sciences ,ddc:530 ,010306 general physics ,physics.acc-ph ,Physics ,Plasma ,Laser ,Physics - Plasma Physics ,Plasma Physics (physics.plasm-ph) ,Full width at half maximum ,Excited state ,Physical Sciences ,Physics::Accelerator Physics ,Physics - Accelerator Physics ,Atomic physics ,Energy (signal processing) ,Beam (structure) - Abstract
Physical review letters 122(3), 034801 (2019). doi:10.1103/PhysRevLett.122.034801, A tunable plasma-based energy dechirper has been developed at FLASHForward to remove thecorrelated energy spread of a 681 MeV electron bunch. Through the interaction of the bunch withwakefields excited in plasma the projected energy spread was reduced from a FWHM of 1.31% to 0.33%without reducing the stability of the incoming beam. The experimental results for variable plasma densityare in good agreement with analytic predictions and three-dimensional simulations. The proof-of-principledechirping strength of $1.8$ $ GeV/mm/m$ significantly exceeds those demonstrated for competing state-of-the-art techniques and may be key to future plasma wakefield-based free-electron lasers and high energyphysics facilities, where large intrinsic chirps need to be removed, Published by APS, College Park, Md.
- Published
- 2018
- Full Text
- View/download PDF
4. Longitudinal gas-density profilometry for plasma-wakefield acceleration targets
- Author
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Jan-Patrick Schwinkendorf, Jens Osterhoff, Tobias Kleinwächter, Lars Goldberg, and Lucas Schaper
- Subjects
Physics ,Nuclear and High Energy Physics ,Jet (fluid) ,Photon ,Fabrication ,business.industry ,Solid angle ,Plasma ,Plasma acceleration ,symbols.namesake ,Optics ,symbols ,Profilometer ,business ,Instrumentation ,Raman scattering - Abstract
Precise tailoring of plasma-density profiles has been identified as one of the critical points in achieving stable and reproducible conditions in plasma wakefield accelerators. Here, the strict requirements of next generation plasma-wakefield concepts, such as hybrid-accelerators, with densities around 10 17 cm −3 pose challenges to target fabrication as well as to their reliable diagnosis. To mitigate these issues we combine target simulation with fabrication and characterization. The resulting density profiles in capillaries with gas jet and multiple in- and outlets are simulated with the fluid code OpenFOAM. Satisfactory simulation results then are followed by fabrication of the desired target shapes with structures down to the 10 µm level. The detection of Raman scattered photons using lenses with large collection solid angle allows to measure the corresponding longitudinal density profiles at different number densities and allows a detection sensitivity down to the low 10 17 cm −3 density range at high spatial resolution. This offers the possibility to gain insight into steep density gradients as for example in gas jets and at the plasma-to-vacuum transition.
- Published
- 2014
- Full Text
- View/download PDF
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