S.M. Lidia
Lawrence Berkeley National Laboratory
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Featured researches published by S.M. Lidia.
Journal of Physics: Conference Series | 2010
F.M. Bieniosek; J.J. Barnard; A. Friedman; E. Henestroza; J.Y. Jung; M. Leitner; S.M. Lidia; B.G. Logan; R.M. More; P. Ni; P.K. Roy; P.A. Seidl; W.L. Waldron
Author(s): Bieniosek, F.M.; Ni, P.; Leitner, M.; Roy, P.; More, R.; Barnard, J.J.; Covo, M. Kireeff; Molvik, A.W.; Yoneda, H.
Physics of Plasmas | 2009
Adam B Sefkow; Ronald C. Davidson; E. P. Gilson; Igor D. Kaganovich; André Anders; J.E. Coleman; M. Leitner; S.M. Lidia; P.K. Roy; P.A. Seidl; W.L. Waldron; S.S. Yu; D.R. Welch
The Heavy Ion Fusion Science Virtual National Laboratory has achieved 60-fold longitudinal pulse compression of ion beams on the Neutralized Drift Compression Experiment (NDCX) [P. K. Roy et al., Phys. Rev. Lett. 95, 234801 (2005)]. To focus a space-charge-dominated charge bunch to sufficiently high intensities for ion-beam-heated warm dense matter and inertial fusion energy studies, simultaneous transverse and longitudinal compression to a coincident focal plane is required. Optimizing the compression under the appropriate constraints can deliver higher intensity per unit length of accelerator to the target, thereby facilitating the creation of more compact and cost-effective ion beam drivers. The experiments utilized a drift region filled with high-density plasma in order to neutralize the space charge and current of an ∼300 keV K+ beam and have separately achieved transverse and longitudinal focusing to a radius <2 mm and pulse duration <5 ns, respectively. Simulation predictions and recent experiments...
Applied Physics Letters | 2005
Emanuele Pedersoli; Francesco Banfi; Barbara Ressel; S. Pagliara; Claudio Giannetti; Gianluca Galimberti; S.M. Lidia; J. Corlett; Gabriele Ferrini; F. Parmigiani
Quantum Efficiency (QE) measurements of single photon photoemission from a Cu(111) single crystal and a Cu polycrystal photocathodes, irradiated by 150 fs-6.28 eV laser pulses, are reported over a broad range of incidence angle, both in s and p polarizations. The maximum QE (approx. = 4x10-4) for polycrystalline Cu is obtained in p polarization at an angle of incidence theta = 65 deg. We observe a QE enhancement in p polarization which can not be explained in terms of optical absorption, a phenomenon known as vectorial photoelectric effect. Issues concerning surface roughness and symmetry considerations are addressed. An explanation in terms of non local conductivity tensor is proposed.
SPIE's 1993 International Symposium on Optics, Imaging, and Instrumentation | 1993
Roger Carr; S.M. Lidia
We present here the design description of a new type of planar helical undulator, which we are constructing for the SPEAR storage ring at the Stanford Synchrotron Radiation Laboratory. It comprises four rows of pure permanent magnet blocks, one row in each quadrant about the axis defined by the electron beam. Rows may be translated longitudinally with respect to each other to change the helicity of the magnetic field they create at the position of the beam. They may also be translated longitudinally to vary the energy of the x-rays emitted, unlike designs where this function is performed by varying the gap between the rows. This work includes numerical calculations of the fields, electron trajectories, and x-ray spectra, including off-axis effects.
Review of Scientific Instruments | 2010
F.M. Bieniosek; E. Henestroza; S.M. Lidia; P. Ni
Intense beams of heavy ions are capable of heating volumetric samples of matter to high energy density. Experiments are performed on the resulting warm dense matter (WDM) at the NDCX-I ion beam accelerator. The 0.3 MeV, 30 mA K(+) beam from NDCX-I heats foil targets by combined longitudinal and transverse neutralized drift compression of the ion beam. Both the compressed and uncompressed parts of the NDCX-I beam heat targets. The exotic state of matter (WDM) in these experiments requires specialized diagnostic techniques. We have developed a target chamber and fielded target diagnostics including a fast multichannel optical pyrometer, optical streak camera, laser Doppler-shift interferometer (Velocity Interferometer System for Any Reflector), beam transmission diagnostics, and high-speed gated cameras. We also present plans and opportunities for diagnostic development and a new target chamber for NDCX-II.
Proceedings of the 1999 Particle Accelerator Conference (Cat. No.99CH36366) | 1999
S.M. Lidia; J. Gardelle; T. Lefevre; J.L. Rullier; J.T. Donohue; P. Gouard
A current experiment is underway to study beam dynamics and RF production in a 35-GHz relativistic klystron using a 1-kA, 7-MeV electron beam produced by the PIVAIR accelerator. We present simulations of transport in the PIVAIR accelerator, modulation from a free-electron laser interaction, post-wiggler solenoidal transport, and interaction with two RF cavities. These simulations are performed with a suite of various codes. Steady-state and transient effects are discussed. The calculated transverse and longitudinal profiles of the beam are compared with experimental diagnostic measurements.
8. beam instrumentation workshop (BIW-98), Stanford, CA (United States), 4-7 May 1998 | 1998
T. Houck; D. E. Anderson; S. Eylon; E. Henestroza; S.M. Lidia; D. Vanecek; G. Westenskow; S.S. Yu
We are constructing a 1.2-kA, 1-MeV, electron induction injector as part of the RTA program, a collaborative effort between LLNL and LBNL to develop relativistic klystrons for Two-Beam Accelerator applications. The RTA injector will also be used in the development of a high-gradient, low-emittance, electron source and beam diagnostics for the second axis of the Dual Axis Radiographic Hydrodynamic Test (DARHT) Facility. The electron source will be a 3.5``-diameter, thermionic, flat-surface, m-type cathode with a maximum shroud field stress of approximately 165 kV/cm. Additional design parameters for the injector include a pulse length of over 150-ns flat top (1% energy variation), and a normalized edge emittance of less than 200 {pi}-mm-mr. Precise measurement of the beam parameters is required so that performance of the RTA injector can be confidently scaled to the 4-kA, 3-MeV, and 2-microsecond pulse parameters of the DARHT injector. Planned diagnostics include an isolated cathode with resistive divider for direct measurement of current emission, resistive wall and magnetic probe current monitors for measuring beam current and centroid position, capacitive probes for measuring A-K gap voltage, an energy spectrometer, and a pepper-pot emittance diagnostic. Details of the injector, beam line, and diagnostics are presented.
7. workshop on advanced accelerator concepts, Lake Tahoe, CA (United States), 12-18 Oct 1996 | 1997
S.M. Lidia; D. Anderson; S. Eylon; E. Henestroza; T. Houck; L. Reginato; D. Vanecek; G. Westenskow; Simon S. Yu
Construction of a prototype RF power source based on the RK-TBA concept, called the RTA, has commenced at the Lawrence Berkeley National Laboratory. This prototype will be used to study physics, engineering, and costing issues involved in the application of the RK-TBA concept to linear colliders. The status of the prototype is presented, specifically the 1-MV, 1.2-kA induction electron gun and the pulsed power system that are in assembly. The RTA program theoretical effort, in addition to supporting the development of the prototype, has been studying optimization parameters for the application of the RK-TBA concept to higher-energy linear colliders. An overview of this work is presented.
Lawrence Berkeley National Laboratory | 2009
S.M. Lidia; André Anders; J.J. Barnard; F.M. Bieniosek; M. Dorf; A. Faltens; A. Friedman; E.P. Gilson; W. Greenway; D.P. Grote; J.Y. Jung; T. Katayanagi; B.G. Logan; C.W. Lee; M. Leitner; P. Ni; A. Pekedis; M. J. Regis; P.K. Roy; P.A. Seidl; W.L. Waldron
HIFAN 1757 HEAVY ION FUSION SCIENCE VIRTUAL NATIONAL LABORATORY, 3rd QUARTER 2009 MILESTONE REPORT, Upgrade plasma source configuration and carry out initial experiments. Characterize improvements in focal spot beam intensity by S. Lidia, A. Anders, F.M. Bieniosek, A. Faltens, W. Greenway, J.Y. Jung, T. Katayanagi, B.G. Logan, C.W. Lee, M. Leitner, P. Ni, A. Pekedis, M. J. Regis, P. K. Roy, P. A. Seidl, W. Waldron Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA J.J. Barnard, A. Friedman, D. Grote, Lawrence Livermore National Laboratory, Livermore, CA 94550, USA M. Dorf, E. Gilson Princeton Plasma Physics Laboratory Accelerator Fusion Research Division Ernest Orlando Lawrence Berkeley National Laboratory University of California June 2009 This work was supported by the Director, Office of Science, Office of Fusion Energy Sciences, of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.
Archive | 2008
Hifs-Vnl; Peter Seidl; P. Seidl; J.J. Barnard; F.M. Bieniosek; J.E. Coleman; D.P. Grote; M. Leitner; E.P. Gilson; B.G. Logan; Steven M. Lund; S.M. Lidia; P. Ni; D. Ogata; P.K. Roy; W.L. Waldron; D.R. Welch; C. Wooton
This milestone has been met by: (1) calculating steering solutions and implementing them in the experiment using the three pairs of crossed magnetic dipoles installed in between the matching solenoids, S1-S4. We have demonstrated the ability to center the beam position and angle to<1 mm and<1 mrad upstream of the induction bunching module (IBM) gap, compared to uncorrected beam offsets of several millimeters and milli-radians. (2) Based on LSP and analytic study, the new IBM, which has twice the volt-seconds of our first IBM, should be accompanied by a longer drift compression section in order to achieve a predicted doubling of the energy deposition on future warm-dense matter targets. This will be accomplished by constructing a longer ferro-electric plasma source. (3) Because the bunched current is a function of the longitudinal phase space and emittance of the beam entering the IBM we have characterized the longitudinal phase space with a high-resolution energy analyzer.