B. Zielbauer
University of Paris-Sud
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by B. Zielbauer.
Plasma Physics and Controlled Fusion | 2011
M. N. Quinn; Xiaohui Yuan; X. X. Lin; D. C. Carroll; O. Tresca; Robert Gray; M. Coury; Changzheng Li; Y. T. Li; C.M. Brenner; A. P. L. Robinson; D. Neely; B. Zielbauer; B. Aurand; J. Fils; T. Kuehl; P. McKenna
The propagation of fast electrons produced in the interaction of relativistically intense, picosecond laser pulses with solid targets is experimentally investigated using K-alpha emission as a diagnostic. The role of fast electron refluxing within the target, which occurs when the electrons are reflected by the sheath potentials formed at the front and rear surfaces, is elucidated. The targets consist of a Cu fluorescence layer of fixed thickness at the front surface backed with a propagation layer of CH, the thickness of which is varied to control the number of times the refluxing fast electron population transits the Cu fluorescence layer. Enhancements in the K-alpha yield and source size are measured as the thickness of the CH layer is decreased. Comparison with analytical and numerical modelling confirms that significant refluxing occurs and highlights the importance of considering this phenomenon when deriving information on fast electron transport from laser-solid interaction experiments involving relatively thin targets.
Optics Letters | 2007
K. Cassou; S. Kazamias; D. Ros; F. Ple; G. Jamelot; A. Klisnick; Olle Lundh; Filip Lindau; Anders Persson; Claes-Göran Wahlström; S. de Rossi; D. Joyeux; B. Zielbauer; D. Ursescu; Thomas Kuehl
We report the near-field imaging characterization of a 10 Hz Ni-like 18.9 nm molybdenum soft-x-ray laser pumped in a grazing incidence pumping (GRIP) geometry with a table-top laser driver. We investigate the effect of varying the GRIP angle on the spatial behavior of the soft-x-ray laser source. After multiparameter optimization, we were able to find conditions to generate routinely a high-repetition-rate soft-x-ray laser with an energy level of up to 3 microJ/pulse and to 6x10(17) photons/s/mm2/mrad2/(0.1% bandwidth) average brightness and 1x10(28) photons/s/mm2/mrad2/(0.1% bandwidth) peak brightness.
Laser and Particle Beams | 2007
Th. Kuehl; D. Ursescu; V. Bagnoud; Dasa Javorkova; O. Rosmej; K. Cassou; S. Kazamias; A. Klisnick; D. Ros; P. V. Nickles; B. Zielbauer; James Dunn; P. Neumayer; G.J. Pert
Intense and stable laser operation with Ni-like Zr and Ag was demonstrated at pump energies between 2 J and 5 J energy from the PHELIX pre-amplifier section. A novel single mirror focusing scheme for the TCE x-ray laser ~XRL! has been successfully implemented by the LIXAM0MBI0GSI collaboration under different pump geometries. This shows potential for an extension to shorter XRL wavelength. Generation of high quality XRL beams for XRL spectroscopy of highly charged ions is an important issue within the scientific program of PHELIX. Long range perspective is the study of nuclear properties of radioactive isotopes within the FAIR project.
Optics Letters | 2010
Daniel Zimmer; B. Zielbauer; M. Pittman; O. Guilbaud; J. Habib; S. Kazamias; David Ros; V. Bagnoud; Thomas Kuehl
This Letter reports on the optimization of a tabletop nickel-like molybdenum transient collisionally excited soft x-ray laser (SXRL) at 18.9 nm performed by a double-pulse single-beam grazing incidence pumping (DGRIP). This scheme allows for the first time, to our knowledge, the full control of the pump laser parameters including the pre-pulse duration optimally generating the SXRL amplifier under a grazing incidence. The single-beam geometry of the collinear double-pulse propagation guarantees the ideal overlap of the pre-pulse and main pulse from shot to shot resulting in a more efficient and highly stable SXRL output. SXRL energies up to 2.2 microJ are obtained with a total pump energy less than 1 J for several hours at a 10 Hz repetition rate without realignment under once optimized double pumping pulse parameters including energy ratio, time delay, pre-pulse and main pulse durations, and line focus width.
Applied Physics Letters | 2011
Robert Gray; Xiaohui Yuan; D. C. Carroll; C. M. Brenner; M. Coury; M. N. Quinn; O. Tresca; B. Zielbauer; B. Aurand; V. Bagnoud; J. Fils; T. Kühl; Xian Lin; Cuncheng Li; Y. T. Li; Markus Roth; D. Neely; P. McKenna
The angular distribution of energetic electrons emitted from thin foil targets irradiated by intense, picosecond laser pulses is measured as a function of laser incidence angle, intensity, and polarization. Although the escaping fast electron population is found to be predominantly transported along the target surface for incidence angles ≥65°, in agreement with earlier work at lower intensities, rear-surface proton acceleration measurements reveal that a significant electron current is also transported longitudinally within the target, irrespective of incident angle. These findings are of interest to many applications of laser-solid interactions, including advanced schemes for inertial fusion energy.
Plasma Physics and Controlled Fusion | 2011
O. Tresca; D. C. Carroll; Xiaohui Yuan; B. Aurand; V. Bagnoud; C. M. Brenner; M. Coury; J. Fils; Robert Gray; T. Kühl; Cuncheng Li; Y. T. Li; X. X. Lin; M. N. Quinn; R. G. Evans; B. Zielbauer; Markus Roth; D. Neely; P. McKenna
Compared with conventional bulk metallic glasses, Ce-based and Zn-based bulk metallic glasses have received considerable attention because of their possible application as structural and functional materials. Kinetic fragility parameter m in amorphous material presents degree of deviations from the Arrhenius law above the glass transition temperature (T-g) of the material. Kinetic fragility parameter (m) and Kauzmann temperature (T-K) in (Ce0.72Cu0.28)(90-x) Al10Fex (x = 0, 5 or 10) and Zn38Mg12Ca32Yb18 bulk metallic glasses have been determined by differential scanning calorimetry (DSC). Results show that Zn38Mg12Ca32Yb18 presents a higher m than (Ce0.72Cu0.28)(90-x) Al10Fex (x = 0, 5 or 10). The activation energies E-g for glass transition are 1.51 eV (x = 0), 1.59 eV (x = 5) and 1.83 eV (x = 10) in (Ce0.72Cu0.28)(90-x) Al10Fex (x = 0, 5 or 10), and 3.59 eV in Zn38Mg12Ca32Yb18, respectively. The values of E-g increase with increasing the Fe content in (Ce0.72Cu0.28)(90-x) Al10Fex (x = 0, 5 or 10) bulk metallic glasses. Kinetic fragility parameter in of bulk metallic glasses increases with the glass transition temperature T-g of bulk metallic glasses, in agreement with previous investigations
Optics Express | 2014
F. Wagner; S. Bedacht; A. Ortner; Markus Roth; A. Tauschwitz; B. Zielbauer; V. Bagnoud
We used time-resolved shadowgraphy to characterize the pre-plasma formation in solid-target interaction experiments with micrometer-scale accuracy. We performed quantitative measurements of the plasma density for amplified spontaneous emission (ASE) levels ranging from 2 · 10(-7) to 10(-10) backed with 2-dimensional hydrodynamic simulations. We find that ASE levels above 10(-9) are able to create a significant pre-plasma plume that features a plasma canal driving a self-focusing of the laser beam. For ASE levels of 10(-10), no ASE pre-plasma could be detected.
Optics Express | 2008
D. Zimmer; V. Bagnoud; Boris Ecker; Udo Eisenbarth; J. Habib; Daniel Hochhaus; Dasa Javorkova; S. Kazamias; Thomas Kuehl; David Ros; D. Ursescu; B. Zielbauer
An optimized pumping geometry for transient collisionally excited soft X-ray lasers is presented, similar to the geometry proposed by [1]. In contrast to usual approaches, where a nanosecond pre-pulse is assumed to provide the optimal plasma preparation and a picosecond pulse performs the final heating- and excitation process, two pulses of equal duration in the range around 10 picoseconds are applied. Both pulses are produced in the front end of the CPA pump laser. They are focused onto the target with the same spherical mirror under non-normal incidence geometry, optimized for efficient traveling wave excitation for the main-pulse. A first experiment was performed on Ni-like palladium (14.7 nm) at less than 500mJ total pulse energy on the target. This proves that this configuration is at least as favorable as the standard GRIP scheme, providing much simpler and more reliable operation.
New Journal of Physics | 2015
G. G. Scott; V. Bagnoud; C. Brabetz; R. J. Clarke; J. S. Green; R. Heathcote; Haydn Powell; B. Zielbauer; T. D. Arber; P. McKenna; D. Neely
We measure a record 96 ±2.5% specularly reflected energy fraction from an interaction with a plasma mirror (PM) surface preionized by a controlled prepulse and find that the optical quality is dependent on the inter pulse time delay. Simulations show that the main pulse reflected energy is a strong function of plasma density scale length, which increases with the time delay and reaches a peak reflectivity for a scale length of 0.3 μm, which is achieved here for a pulse separation time of 3 ps. It is found that the incident laser quasi near field intensity distribution leads to nonuniformities in this plasma expansion and consequent critical surface position distribution. The PM optical quality is found to be governed by the resultant perturbations in the critical surface position, which become larger with inter pulse time delay.
Applied Physics Letters | 2012
G. G. Scott; J. S. Green; V. Bagnoud; C. Brabetz; C. M. Brenner; D. C. Carroll; D. A. MacLellan; A. P. L. Robinson; Markus Roth; C. Spindloe; F. Wagner; B. Zielbauer; P. McKenna; D. Neely
We report on a plasma half cavity target design for laser driven ion acceleration that enhances the laser to proton energy conversion efficiency and has been found to modify the low energy region of the proton spectrum. The target design utilizes the high fraction of laser energy reflected from an ionized surface and refocuses it such that a double pulse interaction is attained. We report on numerical simulations and experimental results demonstrating that conversion efficiencies can be doubled, compared to planar foil interactions, when the secondary pulse is delivered within picoseconds of the primary pulse.