AAWSAP DIRD, Negative Mass Propulsion, January 2011
DOW-UAP-D152 · page 35 of 43
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UNCLASSIFIED//fOR. 8FFI61.t..k W&i QJsll,¥ Furthermore, with the sum of all gravitational charges equal to zero, the cosmological constant A playing the role of a kind of charge, demands that also A = 0. Finally, with the negative entropy of the negative Planck masses playing the role of a kind of photographic negative for the positive entropy of the positive Planck masses, the total entropy, made up from the sum of the positive and negative Planck masses, would also be equal to zero. In summary we may write Lcharges = 0 (103) with the cosmological consequence Q-l=A=S=O . (104) The horizon problem is here resolved by superluminal electromagnetic and gravitational shock waves during the high density phase of the cosmological evolution, not by an inflationary expansion of space. 10. The Cusp/Core Problem in Galactic Halos We have seen that there appears to be strong evidence for the existence of negative matter in the universe. And we have also given reasons that negative matter might be hidden behind positive matter, forming pole-dipole Dirac spinor configurations neutralizing the negative matter. This still leaves open the question as to whether in certain regions of space there might be a surplus of negative over positive matter, and if negative matter can be "mined" from such regions. It has been conjectured by Forward [13) that negative matter might be located in the intergalactic voids, explaining the "bubble" structure of the metagalaxy. The negative mass in the voids would produce gravitational potential hills repelling all matter, positive and negative, like the positive matter of the galaxies produces gravitational potential wells attracting all matter, positive and negative. But the accumulation of negative matter in the gravitational wells of positive matter reduces and flattens the UNCLASSIFIED/fFOA OFFI&I.t.k W&li OJi,k¥ 31