Problems with the Higgs Detection

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The following points cast doubt on the validity of the Higgs boson identification of the recently found 125 GeV particle.
  1. A theoretical proof of inherent contradictions that exist in the Higgs boson mathematical structure has been published here . A generally accepted physical principle states that an acceptable physical theory should have a self-consistent mathematical structure. Therefore, it is concluded that the Higgs boson does not exist. (BTW. as of May 23, 2014, many people have seen the above mentioned article but no refutation of the proof described therein has been published appropriately.)

  2. A not very small number of CERN's LHC experts have used the Standard Model for a calculation of the Higgs boson width (see pp. 142-146 here ). It turns out that the experimental LHC width is about 1000 times greater than the theoretical value predicted for a 125 GeV Higgs boson. A hindsight attempt to explain this huge discrepancy as a property of the LHC machine is certainly not as good as a successful prediction of such a property. Furthermore, this argument says that the width prediction of the LHC people is analogous to a proposal to use a thermometer that measures temperature with an error of 1 0C as an element of a very important experiment that requires an accuracy of 0.001 0C. It is very hard to believe that the above mentioned CERN team of experts can really do such an unscientific work.

  3. The W, Z and the top quark are heavy particles whose mass belongs to the region of the new 125 GeV particle. The experimental width of each of these particles is not less than 2 GeV ( see here ). According to the Standard Model the W,Z are elementary particles that carry the weak interactions; the top quark is an elementary particle that participates in the strong, electromagnetic, weak and gravitational interactions; the Higgs boson explains why some fundamental particles have mass (see its Wikipedia item). Thus, according to the Standard Model, the four particles mentioned herein play three completely different physical tasks. Therefore, one wonders why all these inherently different heavy particles have such a similar width.
Remark: The ground state of the positronium as well as the pions are pairs of spin-1/2 particle-antiparticle bound state where jπ = 0- . These states are determined by the parity conserving electromagnetic and strong interactions, respectively. The even parity found for the 125 GeV particle does not exclude the possibility that it is a top-antitop bound state. Indeed, all the heavy particles: W, Z and the top quark decay under weak interactions and their width is quite large. it means that for the heavy particles, where momentum is also large, distances are quite small and the weak interactions become very big. The parity nonconservation attribute of these interactions indicates that 0+ is a reasonable ground state of a top-antitop bound pair.