Press "Enter" to skip to content

Big Electromagnetic Bosons

Outline

Quark Models for ๐™’, ๐™• and ๐™ƒ

icon for big leptonic mesons

Here are some quark models of massive mesons. These particles include the charged ๐™’ bosons, the neutral particle ๐™•, and the Higgs boson ๐™ƒ. They are noteworthy because they contain hundreds of leptonic quarks, and very few rotating or baryonic quarks. EthnoPhysics analyzes the mechanics of these mesons using chains of events noted by \Psi = ( \mathsf{\Omega}_{1}, \, \mathsf{\Omega}_{2}, \, \mathsf{\Omega}_{3} \, \ldots ) where each repeated cycle \mathsf{\Omega} is composed of the following quarks.

Quark models of big bosons are shown in this spreadsheet screenshot.

The foregoing quark models completely specify quantum numbers for these big mesons. Their charge, angular momentum, baryon-number, lepton-number and strangeness are all correct. These models also produce accurate calculated values for the mass. Results that fall outside of experimental uncertainty are noted with an X in all tables.

Cores for ๐™’, ๐™• and ๐™ƒ

Some highly excited states contain so many quarks that it may be difficult to see how the models work. So to view the underlying pattern, we ignore most of the quark/anti-quark pairs. The \mathsf{q \overline{q}} pairs are needed for stability. But these field quarks obscure the minimum number of quarks required to identify a particle and account for its mass.ย  So we remove them and the remaining core quarks are shown in the table below. The mass depends on  \Delta n not  n. So  m is unchanged by any variation in the field of \mathsf{q \overline{q}} pairs. A particle’s rest mass is completely determined by its core quarks.

Experimentally observed values are taken from this reference .

Calculations for ๐™’, ๐™• and ๐™ƒ

Here is a spreadsheet that shows a step-by-step calculation for the characteristics of a big leptonic meson. For more detail about cell contents and formulae, click the download link at the bottom of the sheet. Then you can enter other quark-coefficients in the yellow cells to assess different particle models.