Symmetrize the upper and lower indices separately, and remove every upper-lower trace. The resulting representation has highest weight . Its dimension is
The subtraction is valid because contraction is onto: in the polynomial realization its adjoint, for the monomial-factorial inner product, is multiplication by the nonzero polynomial , an injective map. The resulting kernel contains the highest-weight constituent and has precisely its Weyl dimension formula dimension, hence is irreducible. This highest-weight constituent is not always the largest-dimensional constituent of the full mixed tensor.
The degree-three monomials , with , form a basis of this ten-dimensional highest-weight representation. Its highest monomial is , and and generate every basis monomial. Its Dynkin labels are , and the weight of a monomial is . In coordinates , the ten weights form four horizontal rows of lengths , all with weight multiplicity one. The baryon decuplet realizes this representation of approximate flavor symmetry.
// Target: special-relativity.bigb
For , the exact largest constituent dimension of a mixed SU(3) tensor representation is
Every constituent highest weight lies below , so its labels have the form for nonnegative integers . If both are positive, reducing each by their minimum increases both and strictly increases the dimension. The resulting boundary labels occur: antisymmetrize disjoint upper pairs into lower indices, or lower pairs into upper indices, then take the symmetric traceless component. This proves the maximum formula. For , the fully symmetric dimension is 21 but has dimension 24. For , the fully symmetric traceless dimension is the maximum.

Articles by others on the same topic (0)

There are currently no matching articles.