By Ruggero Maria Santilli
The scope of this monograph is to teach that our classical, quantum and cosmological wisdom of antimatter is at its starting with a lot but to be chanced on, and dedication to antimatter by means of experimentalists may be beneficial to antimatter technology. this can be additionally the 1st publication featuring the isodual thought of antimatter. it truly is aimed toward scientists and researchers in theoretical physics.
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Additional info for Isodual Theory of Antimatter: with applications to Antigravity, Grand Unification and Cosmology (Fundamental Theories of Physics)
41] because the lack of source implies the impossibility of importing into the theory the basic Newtonian potential. Under these conditions the representation of the Newtonian contribution is reduced to a religious belief, rather than a serious scientiﬁc statement. For these and numerous additional inconsistencies of Einstein’s gravitation or general relativity at large we refer the reader to Yilmaz , Wilhelm , Santilli , Alfv´en [49,50], Fock , Nordensen , and large literature quoted therein.
On the contrary, the assumption of hadronic constituents that can be fully deﬁned in our spacetime directly implies new clean energies. 1 The Negative Impact of General Relativity on Antimatter An important requirement of any consistent classical theory of antimatter is the existence of antigravity deﬁned as a gravitational repulsion experienced by antimatter in the ﬁeld of matter, and vice-versa. As we shall see in detail in Chapter 4, this is essentially due to the achievement in the classical treatment of antimatter of a full dynamical equivalence between electromagnetic and gravitational interactions, thus including the existence of both attraction and repulsion, which classical equivalence is generally lost when antimatter is solely treated in second quantization owing to the notorious absence of a consistent gravitational theory for that level of study.
A more rigorous deﬁnition of these two tensors will be given shortly. It should be indicated that, for a possible solution of Eq. 6), various explicit forms of the electromagnetic ﬁelds as well as of the short range ﬁelds originating the energy-momentum tensors are given in Ref. . Since both sources tensors are positive-deﬁnite, Ref. 7) with consequential general law mInert. ≥ mGrav. 8) where the equality solely applies for the electron. Finally, Ref. 1 for the exterior gravitational problem of a neutral massive body, such as a star, by showing that the situation is essentially the same as that for the π ◦ .