An. Tauschwitz
Goethe University Frankfurt
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Featured researches published by An. Tauschwitz.
Physics of Plasmas | 2010
K. Harres; I. Alber; An. Tauschwitz; V. Bagnoud; Hiroyuki Daido; M. Günther; F. Nürnberg; A. Otten; M. Schollmeier; J. Schütrumpf; M. Tampo; Markus Roth
This article reports about controlling laser-accelerated proton beams with respect to beam divergence and energy. The particles are captured by a pulsed high field solenoid with a magnetic field strength of 8.6 T directly behind a flat target foil that is irradiated by a high intensity laser pulse. Proton beams with energies around 2.3 MeV and particle numbers of 1012 could be collimated and transported over a distance of more than 300 mm. In contrast to the protons the comoving electrons are strongly deflected by the solenoid field. They propagate at a submillimeter gyroradius around the solenoid’s axis which could be experimentally verified. The originated high flux electron beam produces a high space charge resulting in a stronger focusing of the proton beam than expected by tracking results. Leadoff particle-in-cell simulations show qualitatively that this effect is caused by space charge attraction due to the comoving electrons. The collimation and transport of laser-accelerated protons is the first ...
Physics of Plasmas | 2010
P. Neumayer; B. Aurand; M. Basko; B. Ecker; P. Gibbon; D. C. Hochhaus; A. Karmakar; E. D. Kazakov; T. Kühl; C. Labaune; O. Rosmej; An. Tauschwitz; B. Zielbauer; D. Zimmer
A study of the contribution of refluxing electrons in the production of K-alpha radiation from high-intensity laser irradiated thin targets has been performed. Thin copper foils both freestanding, and backed by a thick substrate were irradiated with laser pulses of energies around 100 J at intensities ranging from below 1017 to above 1019 W/cm2. At high laser intensities we find a strong reduction in the K-alpha yield from targets backed by the substrate. The observed yield reduction is in good agreement with a simple model using hot electron spectra from particle-in-cell simulations or directly inferred from the measured bremsstrahlung emission and can therefore be interpreted as due to the suppression of hot electron refluxing. The study shows that refluxing electrons play a dominant role in high-intensity laser driven K- alpha generation and have to be taken into account in designing targets for laser driven high-flux K-alpha sources.
Journal of Computational Physics | 2009
M. Basko; J. A. Maruhn; An. Tauschwitz
A new algorithm for solution of diffusion equations in two dimensions on structured quadrilateral grids is proposed. The algorithm is based on a semi-implicit method for the time discretization and has a nine-point local stencil in space. Our scheme is fast, quite accurate and demonstrates good spatial convergence. The presented numerical tests show that it is well suited for hydrocodes with cell-centered principal variables.
Plasma Physics and Controlled Fusion | 2009
Markus Roth; I. Alber; V. Bagnoud; Colin Brown; R. J. Clarke; H. Daido; Juan C. Fernandez; K. A. Flippo; S. A. Gaillard; C. Gauthier; Matthias Geissel; S. H. Glenzer; G. Gregori; M. M. Günther; K. Harres; R. Heathcote; A. L. Kritcher; N. L. Kugland; S. LePape; Bin Li; M. Makita; J. Mithen; C. Niemann; F. Nürnberg; Dustin Offermann; A. Otten; A. Pelka; David Riley; G. Schaumann; M. Schollmeier
The acceleration of intense proton and ion beams by ultra-intense lasers has matured to a point where applications in basic research and technology are being developed. Crucial for harvesting the unmatched beam parameters driven by the relativistic electron sheath is the precise control of the beam. In this paper we report on recent experiments using the PHELIX laser at GSI, the VULCAN laser at RAL and the TRIDENT laser at LANL to control and use laser accelerated proton beams for applications in high energy density research. We demonstrate efficient collimation of the proton beam using high field pulsed solenoid magnets, a prerequisite to capture and transport the beam for applications. Furthermore, we report on two campaigns to use intense, short proton bunches to isochorically heat solid targets up to the warm dense matter state. The temporal profile of the proton beam allows for rapid heating of the target, much faster than the hydrodynamic response time thereby creating a strongly coupled plasma at solid density. The target parameters are then probed by x-ray Thomson scattering to reveal the density and temperature of the heated volume. This combination of two powerful techniques developed during the past few years allows for the generation and investigation of macroscopic samples of matter in states present in giant planets or the interior of the earth.
Review of Scientific Instruments | 2012
M. Börner; J. Fils; A. Frank; A. Blažević; T. Hessling; A. Pelka; G. Schaumann; A. Schökel; D. Schumacher; M. Basko; J. A. Maruhn; An. Tauschwitz; Markus Roth
This article reports on the development and set-up of a Nomarski-type multi-frame interferometer as a time and space resolving diagnostics of the free electron density in laser-generated plasma. The interferometer allows the recording of a series of 4 images within 6 ns of a single laser-plasma interaction. For the setup presented here, the minimal accessible free electron density is 5 × 10(18) cm(-3), the maximal one is 2 × 10(20) cm(-3). Furthermore, it provides a resolution of the electron density in space of 50 μm and in time of 0.5 ns for one image with a customizable magnification in space for each of the 4 images. The electron density was evaluated from the interferograms using an Abel inversion algorithm. The functionality of the system was proven during first experiments and the experimental results are presented and discussed. A ray tracing procedure was realized to verify the interferometry pictures taken. In particular, the experimental results are compared to simulations and show excellent agreement, providing a conclusive picture of the evolution of the electron density distribution.
The PhysicsofElectronBeamIonTrapsandAdvancedResearchLightSources2005 | 2007
Frank B. Rosmej; R.W. Lee; David Riley; J Meyer-ter-Vehn; A Krenz; T. Tschentscher; An. Tauschwitz; A. Tauschwitz; V. S. Lisitsa; A Ya Faenov
High density plasma physics, radiation emission/scattering and related atomic physics, spectroscopy and diagnostics are going to make large steps forward due to new experimental facilities providing beams of intense heavy ions and X/XUV free electron laser radiation. These facilities are currently being established at GSI-Darmstadt and DESY-Hamburg in Germany to access new and complementary parameter regimes for basic research which have never been obtained in laboratories so far: homogenous benchmark samples near solid density and temperatures from eV up to keV. This will provide important impact to many disciplines like astrophysics, atomic physics in dense environments, dense and strongly coupled plasma effects, radiation emission, equation of state. The spectroscopic analysis of the radiation emission plays a key role in this research to investigate the dynamics of electric fields in multi-particle coupled Coulomb systems and the modification of plasma statistics.
Nature Communications | 2017
W. Cayzac; A. Frank; A. Ortner; V. Bagnoud; M. Basko; S. Bedacht; C. Bläser; A. Blažević; S. Busold; O. Deppert; J. Ding; M. Ehret; P. Fiala; Simon Frydrych; Dirk O. Gericke; L. Hallo; J. Helfrich; D. Jahn; E. Kjartansson; A. Knetsch; D. Kraus; G. Malka; Nico W. Neumann; K. Pépitone; D. Pepler; S. Sander; G. Schaumann; T. Schlegel; N. Schroeter; D. Schumacher
The energy deposition of ions in dense plasmas is a key process in inertial confinement fusion that determines the α-particle heating expected to trigger a burn wave in the hydrogen pellet and resulting in high thermonuclear gain. However, measurements of ion stopping in plasmas are scarce and mostly restricted to high ion velocities where theory agrees with the data. Here, we report experimental data at low projectile velocities near the Bragg peak, where the stopping force reaches its maximum. This parameter range features the largest theoretical uncertainties and conclusive data are missing until today. The precision of our measurements, combined with a reliable knowledge of the plasma parameters, allows to disprove several standard models for the stopping power for beam velocities typically encountered in inertial fusion. On the other hand, our data support theories that include a detailed treatment of strong ion-electron collisions.
Journal of Physics: Conference Series | 2016
A. Ortner; D. Schumacher; W. Cayzac; A. Frank; M. Basko; S. Bedacht; A. Blazevic; S. Faik; D. Kraus; T. Rienecker; G. Schaumann; An. Tauschwitz; F. Wagner; Markus Roth
We report on a new experimental setup for ion energy loss measurements in dense moderately coupled plasma which has recently been developed and tested at GSI Darmstadt. A partially ionized, moderately coupled carbon plasma (ne ≤ 0.8• 1022 cm-3, Te = 15 eV, z = 2.5, Γ = 0.5) is generated by volumetrical heating of two thin carbon foils with soft X-rays. This plasma is then probed by a bunched heavy ion beam. For that purpose, a special double gold hohlraum target of sub-millimeter size has been developed which efficiently converts intense laser light into thermal radiation and guarantees a gold-free interaction path for the ion beam traversing the carbon plasma. This setup allows to do precise energy loss measurements in non-ideal plasma at the level of 10 percent solid-state density.
6th International Conference on Inertial Fusion Sciences and Applications | 2010
Markus Roth; I. Alber; V. Bagnoud; C R D Brown; R. J. Clarke; H. Daido; Juan C. Fernandez; K. A. Flippo; S. A. Gaillard; C. Gauthier; S. H. Glenzer; G. Gregori; M. M. Günther; K. Harres; R. Heathcote; A. L. Kritcher; N. L. Kugland; S. LePape; Bin Li; M. Makita; J. Mithen; C. Niemann; F. Nürnberg; Dustin Offermann; A. Otten; A. Pelka; David Riley; G. Schaumann; M Schollmeier; J. Schütrumpf
The acceleration of intense proton and ion beams by ultra-intense lasers has matured to a point where applications in basic research and technology are being developed. Crucial for harvesting the unmatched beam parameters driven by the relativistic electron sheath is the precise control of the beam. We report on recent experiments using the PHELIX laser at GSI, the VULCAN laser at RAL and the TRIDENT laser at LANL to control and use laser accelerated proton beams for applications in high energy density research. We demonstrate efficient collimation of the proton beam using high field pulsed solenoid magnets, a prerequisite to capture and transport the beam for applications. Furthermore we report on two campaigns to use intense, short proton bunches to isochorically heat solid targets up to the warm dense matter state. The temporal profile of the proton beam allows for rapid heating of the target, much faster than the hydrodynamic response time thereby creating a strongly coupled plasma at solid density. The target parameters are then probed by X-ray Thomson scattering (XRTS) to reveal the density and temperature of the heated volume. This combination of two powerful techniques developed during the past few years allows for the generation and investigation of macroscopic samples of matter in states present in giant planets or the interior of the earth.
Journal of Physics: Conference Series | 2016
W. Cayzac; A. Frank; A. Ortner; V. Bagnoud; M. Basko; S. Bedacht; A. Blažević; O. Deppert; D.O. Gericke; L. Hallo; A. Knetsch; D. Kraus; G. Malka; K. Pépitone; G. Schaumann; T. Schlegel; D. Schumacher; An. Tauschwitz; Jan Vorberger; F. Wagner; Markus Roth
Simulations have been performed to study the energy loss of carbon ions in a hot, laser-generated plasma in the velocity region of the stopping-power maximum. In this parameter range, discrepancies of up to 30% exist between the various stopping theories and hardly any experimental data are available. The considered plasma, created by irradiating a thin carbon foil with two high-energy laser beams, is fully-ionized with a temperature of nearly 200 eV. To study the interaction at the maximum stopping power, Monte-Carlo calculations of the ion charge state in the plasma are carried out at a projectile energy of 0.5 MeV per nucleon. The predictions of various stopping-power theories are compared and experimental campaigns are planned for a first-time theory benchmarking in this low-velocity range.