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  1. #1
    Raider of the lost time
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    Yang-Mills is close but no cigar

    The theory of isotopic or intrinsic spin gauge invariance was discovered independently by C.N. Yang and R.L. Mills in their joint monumental paper published in October 1, 1954, Volume 96, Number 1 of the Physical Review journal. They proposed the existence of a b field which satisfies nonlinear partial differential equations similar to that of electromagnetism. These field quanta have spin unity, isotopic spin unity, and electric charge ±e or zero where e is the electron charge normalized to unity.

    As a quantum theory of general electromagnetism, Yang-Mills theory is non-abelian and was renormalized by ‘t Hooft in the early 70s, see http://nobelprize.org/nobel_prizes/physics/laureates/1999/thooft-lecture.pdf. Quantum field theory (QFT) changed the wavefunctions of non-relativistic quantum mechanics (QM) into arbitrary field variables of relativistic QM. However, the independent variable of time remains a free parameter. Bad to worst, the operator character of position is demoted back to a free parameter while the operational status of linear momentum remains valid. Even with these changes, QFT still cannot unify its operational definitions with that of general relativity (GR). The inherent difficulties could be caused by the fact that quantum fields are described by complex matrices while the metric tensors of GR are real matrices with non-symmetric off diagonal elements. Both formalisms look for the second direction or dimension of time analogous to a genus 2 topology. Nonetheless, stated without proofs that to arrive at a 2nd power of time is simply to set the field variables proportional to the absolute acceleration with proportionality constant as square of vacuum light speed. This can be expressed in a simple partial differential equation as r×a=c² where r is the differential space-time metric, and a as the differential of the absolute acceleration. Logically, this inner product must also be true in the neighborhood of the local infinitesimal domain of space-time such that vectors r and a are orthogonal that is r×a=0 where and when the quantum nature of squares of energy is asymptotically free.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  2. #2
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    Smile Re: Yang-Mills is close but no cigar

    Spin begins with the immediate uprising of thought,there we should start and end our noble quest.



    regards michael.
    Humilty,coupled with boldness,surprises truth to
    reveal herself?

  3. #3
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    Re: Yang-Mills is close but no cigar

    Is there a Yin Mills?

  4. #4
    Raider of the lost time
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    Re: Yang-Mills is close but no cigar

    Quote Originally Posted by mkirkpatrick
    Spin begins with the immediate uprising of thought
    isotopic spin is abstract multidimensional and requires a reverse engineering to reach it.
    Quote Originally Posted by Profpat
    Is there a Yin Mills?
    The darkside of isotopic spin would be yin-mills. This is where and when the antimatter are hidden.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  5. #5
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    Re: Yang-Mills is close but no cigar

    I knew it had to be there somewhere. Is that the side the moss grows on?

  6. #6
    Raider of the lost time
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    Re: Yang-Mills is close but no cigar

    The side of a double Moebius moss growth and decay.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  7. #7
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    Re: Yang-Mills is close but no cigar

    Quote Originally Posted by AntonioLao View Post
    The side of a double Moebius moss growth and decay.
    But that will twist and turn, there is no dark side. Only one side.

  8. #8
    Raider of the lost time
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    Re: Yang-Mills is close but no cigar

    That's why we need another Moeblius twist to complement this existing twist. A double twists would be the square of energy.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  9. #9
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    Re: Yang-Mills is close but no cigar

    Quote Originally Posted by AntonioLao View Post
    That's why we need another Moeblius twist to complement this existing twist. A double twists would be the square of energy.
    Is energy therefore light speed? E = mc squared if there is no mass there would be no energy.

  10. #10
    Raider of the lost time
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    Re: Yang-Mills is close but no cigar

    Network access expire in 5 minutes. I think square square of light speed.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 
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