0 a particle that contains three quarks, especially a neutron or a proton
1 a particle (= small piece of matter that makes up an atom) that contains three quarks, esp. a neutron or a proton
If the baryon number is conserved, then only a small fraction of the energy content of matter can be extracted.
In these new approaches should be also added the conditions under which involving baryons might enhance the magnetic energy to even higher values.
The maximum unstable wavenumber simply shows a transition from higher to smaller values with increasing baryon loading.
But quantum non-locality means that the quantum tunnelling responsible for baryogenesis generates a uniform density of baryons on large scales.
This means that the baryons have essentially the same density on large scales everywhere in the universe.
I have shown that this large number of photons to baryons is a consequence of imposing the wrong boundary conditions in the very early universe.
Furthermore, the range of unstable wavenumbers is narrowest for an electron-positron plasma and becomes increasingly broader for increasing baryon loading, eventually extending to k = 0 for an electron-ion plasma.
They are baryons containing no up or down quarks.
