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Plane thermonuclear detonation waves initiated by proton beams and quasi-one-dimensional model of fast ignition

The one-dimensional (1D) problem on bilatiral irradiation by proton beams of the plane layer of condensed DT mixture with length $2H$ and density $ρ_0 \leqslant 100ρ_s$, where $ρ_s$ is the fuel solid-state density at atmospheric pressure and temperature of 4 K, is considered. The proton kinetic energy is 1 MeV, the beam intensity is $10^{19}$ W/cm$^2$ and duration is 50 ps. A mathematical model is based on the one-fluid two-temperature hydrodynamics with a wide-range equation of state of the fuel, electron and ion heat conduction, DT fusion reaction kinetics, self-radiation of plasma and plasma heating by alpha-particles. If the ignition occurs, a plane detonation wave, which is adjacent to the front of the rarefaction wave, appears. Upon reflection of this detonation wave from the symmetry plane, the flow with the linear velocity profile along the spatial variable $x$ and with a weak dependence of the thermodynamic functions of $x$ occurs. An appropriate solution of the equations of hydrodynamics is found analytically up to an arbitrary constant, which can be chosen so that the analytical solution describes with good accuracy the numerical one. The gain with respect to the energy of neutrons $G\approx 200$ at $Hρ_0 \approx 1$ g/cm$^2$, and $G>2000$ at $Hρ_0 \approx 5$ g/cm$^2$. To evaluate the ignition energy $E_{\mathrm{ig}}$ of cylindrical targets, the quasi-1D model, limiting trajectories of $α$-particles by a cylinder of a given radius, is suggested. The model reproduces the known theoretical dependence $E_{\mathrm{ig}} \sim ρ_0^{-2}$ and gives $E_{\mathrm{ig}} = 160$ kJ for $ρ_0 = 100ρ_s \approx 22$ g/cm$^3$.