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Related papers: Maximizing specific energy by breeding deuterium

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The mass of stars is enough to confine a plasma to fuse light atoms, but this is not possible to engineer on Earth. Fortunately, nuclear engineering can rely on the magnetic confinement of a plasma using superconducting coils so long as the…

Plasma Physics · Physics 2023-10-03 Vikram Goel , Soha Aslam , Sejal Dua

Global consumption of heat is vast and difficult to decarbonise, but it could present an opportunity for commercial fusion energy technology. The economics of supplying heat with fusion energy are explored in context of a future…

Physics and Society · Physics 2025-04-16 S. H. Ward , M. Majeed , N. J. Lopes Cardozo

Among the light elements created in the Big Bang, deuterium is one of the most difficult to detect but is also the one whose abundance depends most sensitively on the density of baryons. Thus, although we still have only a few positive…

Astrophysics · Physics 2007-05-23 Max Pettini

The primordial deuterium abundance probes fundamental physics during the Big Bang Nucleosynthesis and can be used to infer cosmological parameters. Observationally, the abundance can be measured using absorbing clouds along the lines of…

Cosmology and Nongalactic Astrophysics · Physics 2017-05-03 S. Riemer-Sørensen , S. Kotuš , J. K. Webb , K. Ali , V. Dumont , M. T. Murphy , R. F. Carswell

Deuterium enhancement of monodeuterated species has been recognized for more than 30 years as a result of the chemical fractionation that results from the difference in zero point energies of deuterated and hydrogenated molecules. The key…

Astrophysics · Physics 2009-11-11 Charlotte Vastel , T. G. Phillips , P. Caselli , C. Ceccarelli , L. Pagani

The kinematic lower bound for the single scattering of neutrons produced in DT fusion reactions produces a backscatter edge in the measured neutron spectrum. The energy spectrum of backscattered neutrons is dependent on the scattering ion…

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

Understanding gas-grain chemistry of deuterium in star-forming objects may help to explain their history and present state. We aim to clarify how processes in ices affect the deuterium fractionation. In this regard, we investigate a…

Astrophysics of Galaxies · Physics 2017-02-01 J. Kalvans , I. Shmeld , J. R. Kalnin , S. Hocuk

Nanostructured solid boron-hydrogen compounds have been suggested as target and fuel for laser fusion, offering improved laser-plasma coupling, avoiding cryogenic fuel handling and fuel pre-compression and ultimately allowing a transit from…

Plasma Physics · Physics 2024-01-15 Karl Lackner , Rainer Burhenn , Sina Fietz , Alexander von Müller

If fusion power reactors are to be feasible, it will still be necessary to convert the energy of the nuclear reaction into usable form. The heat produced will be removed from the reactor core by a primary coolant, which might be water,…

Physics and Society · Physics 2014-01-20 M. Kovari , C. Harrington , I. Jenkins , C. Kiely

Having previously argued that binary neutron star mergers are the principle source of ultrahigh energy cosmic rays~\citep{fBNS-prl25}, we exploit here the highly constrained initial conditions to make quantitative predictions for the cutoff…

High Energy Astrophysical Phenomena · Physics 2025-11-04 Glennys R. Farrar

This study focuses on a fuel cell composed of Lithium Deuteride (LiD) in a spherical geometry, in which isotropic monoenergetic neutrons of 0.025 eV (thermal neutrons) are generated at the center. The objective is to investigate the…

Instrumentation and Detectors · Physics 2025-03-14 Serena Fattori , Rino Persiani , Ugo Abundo

We simulate fusion in a Z-pinch; where the load is a xenon-plasma liner imploding onto a deuterium-tritium plasma target and the driver is a 2 MJ, 17 MA, 95 ns risetime pulser. The implosion system is modeled using the dynamic, 2-1/2 D,…

Plasma Physics · Physics 2009-11-13 H. U. Rahman , F. J. Wessel , N. Rostoker , P. Ney

The dependence of fusion dynamics on neutron excess for light nuclei is extracted. This is accomplished by comparing the average fusion cross-section at energies just above the fusion barrier for $^{12-15}$C + $^{12}$C with measurements of…

Nuclear Experiment · Physics 2020-07-23 R. T. deSouza , Varinderjit Singh , S. Hudan , Z. Lin , C. J. Horowitz

Theory predicts, and observations confirm, that the column density ratio of a molecule containing D to its counterpart containing H can be used as an evolutionary tracer in the low-mass star formation process. Since it remains unclear if…

Solar and Stellar Astrophysics · Physics 2015-05-27 F. Fontani , Aina Palau , P. Caselli , A. Sanchez-Monge , M. J. Butler , J. C. Tan , I. Jimenez-Serra , G. Busquet , S. Leurini , M. Audard

The idea of using a gas-mixture comprising atoms with high mass number in order to increase proton energies in laser induced plasma acceleration at under critical density is investigated by means of 2D PIC (Particle-In-Cell) simulations.…

Plasma Physics · Physics 2019-06-25 Tadzio Levato , Leonardo V. Goncalves , Vincenzo Giannini

Differential energy structure of a micro multi-charged-particle system and the beam internal potential energy is derived with consequent property and ecessary inference. Then by combining the energy differential structure with differential…

Accelerator Physics · Physics 2007-05-23 Ji Luo , Chuang Zhang

Thermal equilibrium rate can play an important role in the energy deposition of beam to the fuel in fast ignition due to high temperature difference between projectile ions and background plasma ions. In this study the temperature…

Plasma Physics · Physics 2017-12-14 M. Mahdavi , R. Azadifar , T. Khoorokhi

The deuteron binding energy is only 2.2 MeV. At the same time, its yield in Pb+Pb collisions at $\sqrt{s_{NN}} = $2.76 TeV corresponds to a thermal yield at the temperature around 155 MeV, which is too hot to keep deuterons bound. This…

High Energy Physics - Phenomenology · Physics 2019-05-07 Dmytro Oliinychenko , Long-Gang Pang , Hannah Elfner , Volker Koch

Nuclear batteries require radioisotopes with specific combinations of half-life, decay mode, and radiation properties, yet most candidate fuels lack scalable production routes. We show how the future availability of deuterium-tritium (D-T)…

Plasma Physics · Physics 2026-05-21 J. F. Parisi
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