Aesthetic fields—Null theory

Foundations of Physics 10 (11-12):887-903 (1980)
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Abstract

We have studied aesthetic field theory in the case where all invariants constructed from Γ jk i and involving g ij are zero. We studied such a “null” theory in 1972, but the cases we cited were plagued with singularities. By introducing complex fields the situation with respect to singularities improved. Complex fields are consistent with the basic “aesthetic principles” we outlined earlier. Within our null theory we see in two-dimensional spacetime a scattering of particles that was more involved than what we had seen before (regardless of dimensions). We see creation and annihilation of particles out of the vacuum. We also see a three-particle system within a small region of spacetime. In three spacetime dimensions we see a bound two-particle system. Another solution suggests a bound three-particle system. As well as we can tell the particles stay together (confinement) and do not give problems with attenuation. We observe in three dimensions one of the bound systems moving along a definite path in time. The four-dimensional spacetime results are not clear at this point. Whether “topological” bound systems of three particles exist has yet to be determined. A map in the four-dimensional case indicates a planar three maxminima confluence and the suggestion of a second such confluence

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Aesthetic fields—Null theory II.M. Muraskin - 1982 - Foundations of Physics 12 (1):93-100.

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A two-particle collision in aesthetic field theory.M. Muraskin & B. Ring - 1975 - Foundations of Physics 5 (3):513-523.
Sinusoidal solutions to the aesthetic field equations.M. Muraskin - 1980 - Foundations of Physics 10 (3-4):237-242.

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