Higgs Boson Q: Implications for Weak Interactions & Standard Model

captain
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If the higgs boson is never found does that mean that the theory of weak interactions is partly useless because there is no local gauge invariance? If that this not the case then I really want to know what does it entail for the standard model and what would possibly have to be done to fix this error with the theory?
 
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to attain local gauge invariance a simple term is added into the relativistic wave equations which exactly cancels the mistakes caused by the equations' derivative operator. the term is: qA(x)φ(x)
what the higgs boson does is to make stop collision probabilities becoming greater than 1 (which is impossible). also, through it's non zero expectation value (the expectation value is the average value it holds at any point in a vacuum) it spontaneously breaks electroweak gauge symmetry giving mass to gauge bosons
 
https://arxiv.org/pdf/2503.09804 From the abstract: ... Our derivation uses both EE and the Newtonian approximation of EE in Part I, to describe semi-classically in Part II the advection of DM, created at the level of the universe, into galaxies and clusters thereof. This advection happens proportional with their own classically generated gravitational field g, due to self-interaction of the gravitational field. It is based on the universal formula ρD =λgg′2 for the densityρ D of DM...

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