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|    sci.physics.research    |    Current physics research. (Moderated)    |    17,516 messages    |
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|    Message 15,787 of 17,516    |
|    ben6993@hotmail.com to Lawrence Crowell    |
|    Re: Quarkless QCD glueball decay    |
|    19 Aug 17 00:42:12    |
      On Thursday, August 17, 2017 at 6:35:27 AM UTC+1, Lawrence Crowell wrote:       > .... The connection with gravitons is interesting ....       > QCD is a very strong interaction and so this entanglement       > of gluons, or equivalently a bound state, is not stable. However       > an S-dual or in general an STU dual of this di-gluon with a very       > weak dual color QCD-like force could be a graviton.              Somewhere I read that any elementary particle with spin 2 must be       a graviton.       If you take that spin 2 particle and add QCD colour-anticolour,       that is colour-anticolour as for a gluon, would the QCD quality       automatically make the new particle a strong and short-range       force carrier or could the spin 2 quality determine it as a       long-range force carrier? If the former, then a new weak       colour force would be required (if a graviton did indeed exist       and have a weak colour element) but if the latter then QCD colour       could fit the bill? There could be two kinds of graviton, with       and without colour with different force properties.              Likewise, would a higgsball or graviball or darkball (all with       colour-anticolour properties) stretching out >galaxy-wide       have to have an inherently weak colour force? One of my naive       models for a dark particle has no properties except QCD colour.       It could form a darkball/graviball where only QCD colour is       exchanged at interactions.              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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