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The extreme ultraviolet (XUV) emission from dense plasmas generated with sub-10-fs laser pulses with varying peak intensities up to 3*10^16 W/cm^2 is investigated for different target materials. K shell spectra are obtained from low Z…

Plasma Physics · Physics 2009-11-13 J. Osterholz , F. Brandl , M. Cerchez , T. Fischer , D. Hemmers , B. Hidding , A. Pipahl , G. Pretzler , S. J. Rose , O. Willi

Direct laser acceleration (DLA) offers a compact source of high-charge, energetic electrons for generating secondary radiation or neutrons. While DLA in high-density plasma optimizes the energy transfer from a laser pulse to electrons, it…

Plasma Physics · Physics 2025-10-30 Talia Meir , Kale Weichman , Alexey Arefiev , John P. Palastro , Ishay Pomerantz

We determined the ultracold neutron (UCN) production rate by superthermal conversion in the solid deuterium (sD$_2$) moderator of the UCN source at the Paul Scherrer Institute (PSI). In particular, we considered low amounts of less than…

The authors report on the use of carbon nanofiber nanoemitters to ionize deuterium atoms for the generation of neutrons in a deuterium-deuterium reaction in a preloaded target. Acceleration voltages in the range of 50-80 kV are used. Field…

A neutron detector based on EJ301 liquid scintillator has been employed at EAST to measure the neutron energy spectrum for D-D fusion plasma. The detector was carefully characterized in different quasi-monoenergetic neutron fields generated…

Instrumentation and Detectors · Physics 2013-04-30 Xi Yuan , Xing Zhang , Xufei Xie , G. Gorini , Zhongjing Chen , Xingyu Peng , Jinxiang Chen , Guohui Zhang , Tieshuan Fan , Guoqiang Zhong , Liqun Hu , Baonian Wan

An experimental program is currently underway at the National Ignition Facility (NIF) to compress deuterium and tritium (DT) fuel to densities and temperatures sufficient to achieve fusion and energy gain. The primary approach being…

Plasma Physics · Physics 2021-11-09 J. S. Ross , J. E. Ralph , A. B. Zylstra , A. L. Kritcher , H. F. Robey , C. V. Young , O. A. Hurricane , D. A. Callahan , K. L. Baker , D. T. Casey , T. Doeppner , L. Divol , M. Hohenberger , S. Le Pape , A. Pak , P. K. Patel , R. Tommasini , S. J. Ali , P. A. Amendt , L. J. Atherton , B. Bachmann , D. Bailey , L. R. Benedetti , L. Berzak Hopkins , R. Betti , S. D. Bhandarkar , R. M. Bionta , N. W. Birge , E. J. Bond , D. K. Bradley , T. Braun , T. M. Briggs , M. W. Bruhn , P. M. Celliers , B. Chang , T. Chapman , H. Chen , C. Choate , A. R. Christopherson , D. S. Clark , J. W. Crippen , E. L. Dewald , T. R. Dittrich , M. J. Edwards , W. A. Farmer , J. E. Field , D. Fittinghoff , J. Frenje , J. Gaffney , M. Gatu Johnson , S. H. Glenzer , G. P. Grim , S. Haan , K. D. Hahn , G. N. Hall , B. A. Hammel , J. Harte , E. Hartouni , J. E. Heebner , V. J. Hernandez , H. Herrmann , M. C. Herrmann , D. E. Hinkel , D. D. Ho , J. P. Holder , W. W. Hsing , H. Huang , K. D. Humbird , N. Izumi , L. C. Jarrott , J. Jeet , O. Jones , G. D. Kerbel , S. M. Kerr , S. F. Khan , J. Kilkenny , Y. Kim , H. Geppert Kleinrath , V. Geppert Kleinrath , C. Kong , J. M. Koning , J. J. Kroll , O. L. Landen , S. Langer , D. Larson , N. C. Lemos , J. D. Lindl , T. Ma , M. J. MacDonald , B. J. MacGowan , A. J. Mackinnon , S. A. MacLaren , A. G. MacPhee , M. M. Marinak , D. A. Mariscal , E. V. Marley , L. Masse , K. Meaney , N. B. Meezan , P. A. Michel , M. Millot , J. L. Milovich , J. D. Moody , A. S. Moore , J. W. Morton , T. Murphy , K. Newman , J. -M. G. Di Nicola , A. Nikroo , R. Nora , M. V. Patel , L. J. Pelz , J. L. Peterson , Y. Ping , B. B. Pollock , M. Ratledge , N. G. Rice , H. Rinderknecht , M. Rosen , M. S. Rubery , J. D. Salmonson , J. Sater , S. Schiaffino , D. J. Schlossberg , M. B. Schneider , C. R. Schroeder , H. A. Scott , S. M. Sepke , K. Sequoia , M. W. Sherlock , S. Shin , V. A. Smalyuk , B. K. Spears , P. T. Springer , M. Stadermann , S. Stoupin , D. J. Strozzi , L. J. Suter , C. A. Thomas , R. P. J. Town , E. R. Tubman , P. L. Volegov , C. R. Weber , K. Widmann , C. Wild , C. H. Wilde , B. M. Van Wonterghem , D. T. Woods , B. N. Woodworth , M. Yamaguchi , S. T. Yang , G. B. Zimmerman

Generation of high-energy proton bunch from interaction of an intense short circularly polarized(CP) laser pulse with a gas-filled cone target(GCT) is investigated using two-dimensional particle-in-cell simulation. The GCT target consists…

Plasma Physics · Physics 2015-05-28 H. Y. Wang , F. L. Zheng , Y. R. Lu , Z. Y. Guo , X. T. He , J. E. Chen , X. Q. Yan

Ultra-cold neutrons (UCN), neutrons with energies low enough to be confined by the Fermi potential in material bottles, are playing an increasing role in measurements of fundamental properties of the neutron. The ability to manipulate UCN…

We propose to produce neutron-rich nuclei in the range of the astrophysical r-process around the waiting point N=126 by fissioning a dense laser-accelerated thorium ion bunch in a thorium target (covered by a CH2 layer), where the light…

Nuclear Experiment · Physics 2015-05-19 D. Habs , P. G. Thirolf , M. Gross , K. Allinger , J. Bin , A. Henig , D. Kiefer , W. Ma , J. Schreiber

Using a real-time formalism of equilibrium and nonequilibrium quantum-field theory, we derive the reaction-rate formula for neutrino-conversion ($\nu \to \nu'$) process and $\nu \bar{\nu}'$ annihilation process, which take place in a hot…

High Energy Physics - Phenomenology · Physics 2009-11-07 N. Asida , A. Niégawa , H. Ozaki , M. Kubota

The production of light nuclei in relativistic heavy-ion collisions is well described by both the thermal model, where light nuclei are in equilibrium with all other hadron species present in a fireball, and by the coalescence model, where…

Nuclear Theory · Physics 2020-09-08 Stanislaw Mrowczynski , Patrycja Slon

The deuteron-deuteron (D-D) thermonuclear reaction rates in metallic environments (considering the electron screening effects) is calculated using the S-factor functions which were obtained by fitting to low-energy data on D-D reactions.…

Nuclear Theory · Physics 2025-06-03 Faisal Etminan

Relativistic temperature electrons higher than 0.5 MeV are generated typically with laser intensities of about 10$^{18}$ W/cm$^{2}$. Their generation with high repetition rate lasers that operate at non-relativistic intensities…

We present the detection of directional muon beams produced using a PW laser at the Lawrence Berkeley National Laboratory. The muon source is a multi-GeV electron beam generated in a 30 cm laser plasma accelerator interacting with a high-Z…

A diamond-like carbon circular target is proposed to improve the $\gamma$-ray emission and pair production with lasers intensity of $8\times 10^{22} ~\mathrm{W/cm^2}$ by using two-dimensional particle-in-cell simulations with quantum…

Plasma Physics · Physics 2019-09-04 Ya-Juan Hou , Bai-Song Xie , Chong Lv , Feng Wan , Li Wang , Nureli Yasen , Hai-Bo Sang , Guo-Xing Xia

The performance of the solid deuterium ultra-cold neutron source at the pulsed reactor TRIGA Mainz with a maximum peak energy of 10 MJ is described. The solid deuterium converter with a volume of V=160 cm3 (8 mol), which is exposed to a…

Instrumentation and Detectors · Physics 2015-06-16 J. Karch , Yu. Sobolev , M. Beck , K. Eberhardt , G. Hampel , W. Heil , R. Kieser , T. Reich , N. Trautmann , M. Ziegner

Frequency up-conversion of a few low-energy photons into a single high-energy photon contributes to imaging, light sources, and detection. However, the up-converting of many photons exhibits negligible efficiency. Up-conversion through…

Optics · Physics 2018-09-03 Dafna Granot , Nimrod Kruger , Assaf Manor , Carmel Rotschild

A large area (0.5~m $\times$ 0.5~m) thermal neutron detector was developed based on 0.32~mm-thick $^{6}$LiF:ZnS(Ag) scintillator sheets. The detector was constructed for measurements of seasonal variations in low intensity thermal neutron…

Instrumentation and Detectors · Physics 2018-07-24 Alexandre Kozlov , Dmitry Chernyak

We demonstrate a compact, non-toxic, low-cost neutron-yield diagnostic for pulsed D--T fusion systems using an undoped fused-silica (SiO$2$) rod as both activation target and Cherenkov radiator. D--T neutrons (14.1 MeV) activate $^{28}$Si…

Instrumentation and Detectors · Physics 2026-03-06 N. Kaneshige , S. Alawabdeh , W. Hennig , D. Cech , M. Hua , R. Grazioso

The work presented in this thesis forms part of a program at the Paul Scherrer Institute (PSI) to construct a high intensity superthermal ultra-cold neutron (UCN) source based on solid deuterium as UCN production medium. We carried out a…

Nuclear Experiment · Physics 2007-05-23 Malgorzata Kasprzak