A phenomenon caused by the existence of this quantity can be explained by viewing the vacuum as a dual superconductor, where magnetic monopoles condense in a fashion analogousto the Cooper pairs in a normal superconductor.
A phenomenon caused by the existence of this quantity can be explained by viewing the vacuum as a dual superconductor, where magnetic monopoles condense in a fashion analogousto the Cooper pairs in a normal superconductor. Minus one-sixth, one-third, one-half, or zero are the values for a set of "factors" named for this quantity which appear in the matrix elements of interactions which change it. The component of a meson's wavefunction corresponding to this quantity is a singlet state with a normalization factor of one over the square root of 3. This quantity gives rise to a potential with a short-range term proportional to minus four-thirds times one over distance and a long-range term linearly proportional to distance; thus, this property gives rise to asymptotic freedom and quark confinement. For 10 points, name this property that explains the strong force according to QCD.
A phenomenon caused by the existence of this quantity can be explained by viewing the vacuum as a dual superconductor, where magnetic monopoles condense in a fashion analogousto the Cooper pairs in a normal superconductor.
color charge [do not accept or prompt on "charge" or "electric charge"]