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Related papers: Advances towards pB11 Fusion with the Dense Plasma…

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Fusion with p11B has many advantages, including the almost complete lack of radioactivity and the possibility of direct conversion of charged particle energy to electricity, without expensive steam turbines and generators. But two major…

Plasma Physics · Physics 2007-05-23 Eric J. Lerner

Proton-Boron 11 (pB11) fusion is relatively safe and clean, but difficult to use for net power production, since bremsstrahlung radiation tends to radiate away power more quickly than it can be generated by fusion power, particularly once…

Plasma Physics · Physics 2025-11-17 I. E. Ochs , E. J. Kolmes , A. S. Glasser , N. J. Fisch

Recent work on the revised Gratton-Vargas model has demonstrated that there are some aspects of Dense Plasma Focus (DPF) which are not sensitive to details of plasma dynamics and are well captured in an oversimplified model assumption which…

Plasma Physics · Physics 2017-01-04 S K H Auluck

Aneutronic and nonradioactive properties make the proton-boron fusion a prospective candidate for fusion energy production through reactions following p+$^{11}$B$\rightarrow$3${\alpha}$ (p-$^{11}$B). However, it is difficult to achieve a…

The possibility of fusion ignition in proton-Boron$^{11}$ plasma is strongly enhanced if the energy from the fusion-produced $\alpha$ particles is channeled to fast protons, but in an environment in which most of the protons are thermally…

Plasma Physics · Physics 2022-12-05 E. J. Kolmes , I. E. Ochs , N. J. Fisch

Inertial Confinement Fusion is a promising option to provide massive, clean, and affordable energy for mankind in the future. The present status of research and development is hindered by hydrodynamical instabilities occurring at the…

Plasma Physics · Physics 2018-10-17 L. P. Csernai , N. Kroo , I. Papp

We report on 3D-3V particle-in-cell simulations of fast-ion energy-loss rates in cold, weakly-magnetized, weakly-coupled plasma where the electron gyroradius, $\rho_{e}$, is comparable to or less than the Debye length, $\lambda_{De}$, and…

Plasma Physics · Physics 2018-05-09 E. S. Evans , S. A. Cohen , D. R. Welch

Controlled fusion with advanced fuels requires average electron and ion energies above 100 keV (equivalent to 1.1 billion K) in a dense plasma. We have met this requirement and demonstrated electron and ion energies over 100 keV in a…

Plasma Physics · Physics 2007-05-23 Eric J. Lerner

We present hybrid PIC simulations of fast electron transport and energy deposition in pre-compressed fusion targets, taking full account of collective magnetic effects and the hydrodynamic response of the background plasma. Results on…

Plasma Physics · Physics 2009-11-13 J. J. Honrubia , J. Meyer-ter-Vehn

The proton-boron (p-$^{11}$B) reaction is regarded as the holy grail of advanced fusion fuels, since the primary reaction produces three $\alpha$ particles with few neutrons and induced radio-activities from second order reactions. Compared…

While magnetic confinement fusion (MCF) and inertial confinement fusion (ICF) remain the primary routes toward controlled fusion, progress is still constrained by energy loss, plasma instabilities, and the cost and complexity of large-scale…

Plasma Physics · Physics 2026-04-13 Yinjian Zhao , Zhe Liu , Qiang Sun , Qianhong Zhou , Guangrui Sun

The MCNP program used to simulate the hard x-ray emission from KSU dense plasma focus device, an electron beam spectrum of maximum energy 100 keV was used to hit anode target. The bremsstrahlung radiation was measured using the F2 tally…

Instrumentation and Detectors · Physics 2015-03-11 Amgad E. Mohamed

The emission of multi-MeV ($\gamma$-ray) photons from the interaction of a high-powered laser pulse with a dense plasma target is studied using particle-in-cell simulations. A new set of diagnostic techniques is presented and applied to…

Plasma Physics · Physics 2021-07-02 A. H. Younis , A. Davidson , B. Hafizi , D. F. Gordon

Energizing background ions plays a pivotal role in all forms of thermal nuclear fusion, as it can increase the fusion reaction rate without affecting the overall mechanical equilibrium. This is particularly critical for p11B fusion due to…

Relativistic electrons generated by the interaction of petawatt-class short laser pulses with solid targets can be used to generate bright X-rays via bremsstrahlung. The efficiency of laser energy transfer into these electrons depends on…

An optically thin $p$-$^{11}$B plasma loses more energy to bremsstrahlung than it gains from fusion reactions, unless the ion temperature can be elevated above the electron temperature. In thermal plasmas, the temperature differences…

Plasma Physics · Physics 2015-12-09 Michael J. Hay , Nathaniel J. Fisch

Extreme beams of charged particles and photons, reaching ultrahigh densities or producing intense gamma-ray bursts, are central to accelerator physics, laboratory astrophysics, and strong-field quantum electrodynamics research. Yet their…

Plasma densification through magnetic compression has been suggested for time-resolved control of the wave properties in plasma-based accelerators. Using particle in cell simulations with real mass ratio, the practicality of large magnetic…

Plasma Physics · Physics 2016-04-20 Renaud Gueroult , Nathaniel J. Fisch

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

We study the effects of redistributing superthermal electrons on Bremsstrahlung radiation from hot relativistic plasma. We consider thermal and nonthermal distribution of electrons with an energy cutoff in the phase space and explore the…

Plasma Physics · Physics 2023-06-13 Vadim R. Munirov , Nathaniel J. Fisch
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