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  1. #1
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    relativistic invariance

    Electric charges obey the principle of relativistic invariance. However, gravity charges do not. But the more important question is what about color charges? Do they or do they not obey the principle of relativistic invariance? Consequently, color charges are exclusive attributes of quarks and gluons (if they exist) while all other matter and antimatter are predominantly colorless.

    Another distinction is that electric charges are quantized but not gravity charges. In theory, gravity charges can become quantized if and only if the concept of a quantum of mass is validated. Experimentally, a continuous spectrum of relativistic mass values can always be measured. However, the same experiments only allow electric charges to exist only in 3 states: positive, negative, and neutral while color charges can only exist in 4 states: red, green, blue, and colorless. Nevertheless, only by empirical coincidences so do colorless matter and antimatter (e.g. mesons and hadrons) violate the principle of relativistic invariance. For the colorful quarks and gluons (if they exist), their relativistic invariance cannot yet be experimentally determined or verified.
    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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    Re: relativistic invariance

    How can a color charge be colorless. If it lacked color would it still be a color charge?

  3. #3
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    Re: relativistic invariance

    a color and its anticolor is colorless for all mesons. A red quark together with a green quark and a blue quark is also colorless for all baryons. This suggests that if your avatar is a baryon then it must be colorless.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

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    Re: relativistic invariance

    I would have thought they would be white.

  5. #5
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    Re: relativistic invariance

    White is technically defined as colorless as in sunlight or randomized electomagnetic polarization.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  6. #6
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    Re: relativistic invariance

    Quote Originally Posted by AntonioLao View Post
    White is technically defined as colorless as in sunlight or randomized electomagnetic polarization.
    Thank you for that " clarification "

  7. #7
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    Re: relativistic invariance

    But color charges are really not color in the physical sense. Properly defined I would rather call them directional invariance properties.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

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    Re: relativistic invariance

    To each their own Antonio. I like color charges better, it's more " colorful "

  9. #9
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    Re: relativistic invariance

    Then you have become a member of the majority of physicists with Gell-Mann at the top of the list. I wonder how is he doing? http://en.wikipedia.org/wiki/Murray_Gell-Mann
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  10. #10
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    Re: relativistic invariance

    Hopefully he's coming up with my An Idea, independently on his own.

 

 
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