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Energie zu niedrigen Preisen durch lasergetriebene Kernfusion?

Energie zu niedrigen Preisen durch lasergetriebene Kernfusion?. Heinrich Hora University of New South Wales, Sydney, Australien.

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Energie zu niedrigen Preisen durch lasergetriebene Kernfusion?

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  1. Energie zu niedrigen Preisen durch lasergetriebene Kernfusion? Heinrich Hora University of New South Wales, Sydney, Australien

  2. Scheme for demonstration of the essential different geometry of the laser-plasma interaction volumes for subsequent volume-force nonlinear electron acceleration with separation by the ion charge Z.

  3. Nonlinear Force at Perpendicular Incidence Plasma in one dimension (x-direction) fNL = (n2 -1) E2 / 8p fNL = - (/x) (E2 + H2) / (8p)

  4. Force Density in Plasma f = fth + fNL thermokinetic force fth = - p General nonlinear force fNL = .[EE + HH - 0.5(E2+ H2)1 + (1 + /t)/)(n2 -1) EE]/(4p) - /t) E x H / (4pc) Reformulated Lorentz and gauge invariant and complete fNL = j x H/c + E + P.E/4p + (1/ )(/t) E.(n2 -1) E/(4p) + [1 + (1/ )(/t)] .(n2 -1) E.E/ 4p Lorentz term fNL = j x H/c Coulomb term fcoulomb = E Kelvin ponderomotive term fkelvin = P.E/4p = (n2 -1) E2/ 8p - (n2 -1) E x ( x E) / 4p New nonlinear terms

  5. Density ne(x) of a plasma with collisions exceeding the cut-off density with an incident purely penetrating laser beam (hv) which can also be constructed in this case by the WKB approximation. The variation of the quantity Ey2 + Hz2 results in the nonlinear forces fNL.

  6. Generation of blocks of deuterium plasma moving with velocities above 109 cm/s against the neodymium glass laser light (positive velocities v to the right) and moving into the plasma interior (negative velocities) at irradiation by a neodymium glass laser of 1018 W/cm2 intensity onto an initially 100eV and 100µm thick bi-Rayleigh profile with minimum internal reflection.

  7. Scheme of skin depth laser interaction where the non-linear force accelerates a plasma block against the laser light and another block towards the target interior. In front of the blocks are electron clouds of the thickness of the effective Debye lengths of less than 500 nm.

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