Abstract
In this paper, I have studied the properties of atomic and molecular world along with general and special theories of relativity. This is an attempt to merge Gravity into the standard model in order to complete the Grand Unification Theory. The merger of gravity into the other forces i.e. electromagnetic, strong and weak nuclear forces should be well defined and in the boundaries of Gauge Group theory. The Lorentz transformations used in the theory too are invariant under SU(2) type of space. The relative force exerted on two separate quantum systems is also discussed along with Dark matter and Dark energy at a quantum level. I have also tried to solve the Banach-Tarski theorem by applications of Heisenbergs Uncertainty principle in the later part of the paper. Detailed particle Chirality in standard model is redefined to fit in the criterion of operators used in the same process. Possible existence of a new quasi particle is also included in the paper along with its properties.
Highlights
The nature of matter has baffled physicists for a long time
The relative force exerted on two separate quantum systems is discussed along with Dark matter and Dark energy at a quantum level
Today’s physics is unable to explain why does the particle propagate the way it does in sub-space topologies? In order to tackle these problems and problems with higher magnitudes, we need to draw a link between the motion of particles and there dimensionalities
Summary
Quantum relativity is like quantum coupling but different in the sense that it takes dimensionality into consideration This way, a particle could certainly propagate through space and a higher dimension as well. Talking about Chiral symmetry, Vector gauge theories with mass less Dirac Fermion fields ψ exhibit chiral symmetry, i.e., rotating the left-handed and the right-handed components independently makes no difference to the theory. We can write this as the action of rotation on the fields:. From above it can be noted that chirality of particles u and d (taken in the example) differ from chirality observed when at steady state and in motion The parity symmetry or in this case anti-symmetry depends on the relativistic proportional operator
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