| shadow of X boson -
03-29-2007, 12:57 PM
Something is real when but not where it casts a shadow. Shadows could not materialize or dematerialize unless something is blocking the path of light rays. This requires interactions of light with matter. They are successfully described by QED, which is a theory about interactions between photons and negative/positive electrons.
From a relativistic quantum mechanical perspective, the appearance of shadow is the same as the absorption of a gauge boson. However, from a relativistic quantum field perspective, it is equivalent to field materialization, a reduction in the number of degrees of freedom. All non-interactive fields are presumed continuous with infinite degrees of freedom, for example, the field of the true vacuum. Once the fields begin to interact with themselves or with other fields, their infinite degrees of freedom reduce to finite degrees and three things materialize: (1) matter, (2) energy, or (3) both matter and energy. Since matter is just concentrated energy, E=mc˛, the shadows must then be higher powers of energy. For theoretical simplification, the non-interactive shadows are all squares of energy.
Time independence: [∂E(g)]˛=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c˛
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