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The alpha-particle energy deposition mechanism modifies the ignition conditions of the thermonuclear Deuterium-Tritium fusion reactions, and constitutes a key issue in achieving high gain in Inertial Confinement Fusion implosions.…

Plasma Physics · Physics 2017-08-02 Mauro Temporal , Benoit Canaud , Withold Cayzac , Rafael Ramis , Robert L. Singleton

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

A novel capsule target design to improve the hot-spot pressure in the high-adiabat implosion for inertial confinement fusion is proposed, where a layer of comparatively high-density material is used as a pusher between the fuel and the…

Plasma Physics · Physics 2017-02-21 Dongguo Kang , Shaoping Zhu , Wenbing Pei , Shiyang Zou , Wudi Zheng , Jianfa Gu , Zhensheng Dai

The results from 2.5-dimensional Particle-in-Cell simulations for the interaction of a picosecond-long ignition laser pulse with a plasma pellet of 50-$\mu m$ diameter and 40 critical density are presented. The high density pellet is…

Plasma Physics · Physics 2009-11-11 C. Ren , M. Tzoufras , J. Tonge , W. B. Mori , F. S. Tsung , M. Fiore , R. A. Fonseca , L. O. Silva , J. -C. Adam , A. Heron

The success of direct laser-driven inertial confinement fusion (ICF) relies critically on the efficient coupling of laser light to plasma. At ignition scale, the absolute stimulated Raman scattering (SRS) instability can severely inhibit…

Plasma Physics · Physics 2020-08-19 A. V. Maximov , J. G. Shaw , J. P. Palastro

Why do we use nano-antennas for fusion? In three sentences: The present laser induced fusion plans use extreme mechanical shock compression to get one hotspot and then ignition. Still fusion burning spreads slower than expansion, and…

The neutron yields observed in inertial confinement fusion experiments for higher convergence ratios are about two orders of magnitude smaller than the neutron yields predicted by one-dimensional models, the discrepancy being attributed to…

Nuclear Experiment · Physics 2007-05-23 Silviu Olariu

Turbulence enhances fusion reactivity, enabling ignition at lower temperature. A modified Lawson-like ignition criterion is derived for inertially confined plasmas harboring turbulent kinetic energy. Remarkably, if small-scale turbulence is…

Plasma Physics · Physics 2025-07-28 Henry Fetsch , Nathaniel J. Fisch

To enhance the core heating efficiency in fast ignition laser fusion, the concept of relativistic electron beam guiding by external magnetic fields was evaluated by integrated simulations for FIREX class targets. For the cone-attached shell…

To quantify the sensitivity of diverse implosion designs to laser imprinting, we developed an equivalent perturbation model that maps laser imprinting as the target surface perturbation. By incorporating imperfections in target fabrication…

Plasma Physics · Physics 2026-03-03 Dongxue Liu , Jiaqin Dong , Yunxing Liu , Zhiyu He , Wei Wang , Yuqiu Gu , Xiuguang Huang , Jian Zheng

A practical formula for calculating laser intensity at the onset of beam spray is presented with application to inertial confinement fusion at the National Ignition Facility.

Plasma Physics · Physics 2007-05-23 Pavel M. Lushnikov , Harvey A. Rose

In a previous Letter [Phys. Rev. Lett. 96, 123401 (2006)] we have shown by means of three-dimensional particle-in-cell simulations and a simple rigid-sphere model that nonlinear resonance absorption is the dominant collisionless absorption…

Atomic and Molecular Clusters · Physics 2009-11-13 M. Kundu , D. Bauer

The attainment of ultrahigh electric potentials by suppressing the stepped leader breakdown of a highly charged conductor levitated in a spiraling Taylor flow opens up the possibility of order of magnitude larger driver energies for the…

Plasma Physics · Physics 2009-09-29 Friedwardt Winterberg

Burn efficiency is a key for commercial feasibility of fusion power station for inertial fusion energy, while burn efficiency is usually lower than 30% in the central ignition scheme of inertial confinement fusion (ICF). A recent conceptual…

Plasma Physics · Physics 2024-12-25 Yongsheng Li , Ke Lan , Hui Cao , Yao-Hua Chen , Xiaohui Zhao , Zhan Sui

Laser-induced breakdown with ultrashort laser pulses is isochoric and inertially confined. It is characterized by a sequence of nonlinear energy deposition and hydrodynamics events such as shock wave emission and cavitation bubble…

Fluid Dynamics · Physics 2025-01-24 Xiao-Xuan Liang , Alfred Vogel

Laser-plasma instabilities under ignition conditions for direct-drive inertial confinement fusion are studied using two-dimensional Particle-in-Cell simulations with a combination of in-plane (PP) and out-of-the-plane (SP) lasers. The…

Plasma Physics · Physics 2024-09-10 S. H. Cao , M. J. Rosenberg , A. A. Solodov , H. Wen , C. Ren

Pellets of frozen material travelling into a magnetically confined fusion plasma are accelerated by the so-called pellet rocket effect. The non-uniform plasma heats the pellet ablation cloud asymmetrically, producing pressure-driven,…

A completely rigorous first-principles calculation of the charged particle stopping power has recently been performed by Brown, Preston, and Singleton (BPS). This calculation is exact to leading and next-to-leading order in the plasma…

Plasma Physics · Physics 2008-02-21 Robert L. Singleton

Two-dimensional simulations of ion beam driven fast ignition are presented. Ignition energies of protons with Maxwellian spectrum and carbon ions with quasimonoenergetic and Maxwellian energy distributions are evaluated. The effect of the…

Plasma Physics · Physics 2009-10-08 J. J. Honrubia , J. C. Fernandez , M. Temporal , B. M. Hegelich , J. Meyer-ter-Vehn

The acceleration of lithium tube segments with the length one centimeter, diameter sixteen microns wall thickness one nanometer is considered. These segments are electrically charged by proton beams produced by an electron beam source.…

Plasma Physics · Physics 2013-11-22 S. N. Dolya