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B electroweak asymptotic freedom

  1. Nov 12, 2017 #1
    First, the coupling constant of the strong force can be computed.. does it mean it should also (ought to be) for the electroweak?

    Also U(1) is not asymptotically free but electroweak SU(2)xU(1) is asymptotically free.. why is SU(2)xU(1) asymptotically free?
     
  2. jcsd
  3. Nov 17, 2017 at 6:00 PM #2
    Thanks for the thread! This is an automated courtesy bump. Sorry you aren't generating responses at the moment. Do you have any further information, come to any new conclusions or is it possible to reword the post? The more details the better.
     
  4. Nov 20, 2017 at 11:49 PM #3

    king vitamin

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    I don't believe that it is. In (3+1) dimensions, the U(1) coupling should grow in the UV.
     
  5. Nov 21, 2017 at 9:01 PM #4
    I queried this as a result of reading Peter Woit book "Not Even Wrong".. he quoted:

    "Why SU(3)xSU(2)xU(1)? A truly fundamental theory should explain where this precise set of symmetry groups is coming from. In addition, whereas QCD (the SU(3) part of this) has the beautiful property of having no free parameters, introducing the two other groups SU(2) and U(1)) introduces two free parameters and one would like some explanation of why they have the values they do. One of these is the fine structure constant a, and the question of where this number comes from goes back to the earliest days of QED. Another related concern is that the U(1) part of the gauge theory is not asymptotically free, and as a result it may not be completely mathematical consistent."

    I thought he meant that SU(2)xU(1) was asymptotically free.. if not.. why did he mentioned that "Another related concern is that the U(1) part of the gauge theory is not asymptotically free, and as a result it may not be completely mathematical consistent"? This statement implied SU(2)xU(1) was asymptotically free.
     
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