- #1
lpetrich
- 988
- 178
I have a problem with doing that. I've discovered some formulas for doing that, which I've found by making certain plausible assumptions and requiring self-consistency in various special cases, like
adjoint -> (adjoint,scalar) + (scalar, adjoint) + (extra stuff)
but I haven't found anything in the literature on these formulas, though I don't have access to many journal articles.
I've created a Mathematica notebook that calculates Lie-algebra properties that a physicist may find useful, like breakdown of product representations and the aforementioned branching rules: breakdown of a irreducible representation (irrep) into irreps of subgroups.
Nearly all of that notebook's content except for branching-rule details is from Robert N. Cahn's book Semi-Simple Lie Algebras and their Representations, which he has generously placed online. I've been able to calculate Dynkin diagrams, Cartan matrices, irreducible representations' root and weight vectors from their highest weights, and decompositions of products of irreps (irreducible representations). My branching-rule calculations proceed much like the product-rep calculations, but instead with
(root vector in subalgebra) = (matrix).(root vector in original algebra)
(U(1) weight) = (vector).(root vector in original algebra)
The problem I have is demonstrating the correctness of the matrices and vectors I have found. I did so by making some reasonable assumptions and imposing self-consistency in simple cases, like fundamental and adjoint reps. Is anyone familiar enough with the professional literature on Lie-algebra branching rules to point me to some discussions of this question?
-
However, I've found general formulas for the matrices and vectors for all the infinite families (SU, SO, Sp), and explicit values of them for all the exceptional algebras (G2, F4, E6, E7, E8). These are valid for all the breakdowns, as far as I've been able to find out.
I can do demotion of roots, making them into U(1) weights and getting the subalgebras by removing those roots from the originals' Dynkin diagrams.
I can also do removing of roots from extended Dynkin diagrams, using those in Robert Cahn's book.
I can even do some additional cases: SO(7) -> G2 and SO(even) -> SO(odd) * SO(odd)
Does anyone want to see the explicit matrices and the formulas that I've found?
-
Here's a classic case of root demotion: the breaking of the gauge symmetry of the Georgi-Glashow GUT into the Standard-Model gauge symmetry:
SU(5) -> SU(3) * SU(2) * U(1)
Original Dynkin diagram: o - o - o - o
With demoted root (#3): o - o (o) o
Notice that it's broken down into SU(3), U(1), and SU(2) in that order.
I get the correct decompositions of these SU(5) irreps:
1 -> (1,1,0)
5 -> (3,1,2/5) + (1,2,-3/5)
10 -> (3,2,-1/5) + (3*,1,4/5) + (1,1,-6/5)
10* -> (3*,2,1/5) + (3,1,-4/5) + (1,1,6/5)
5* -> (3*,1,-2/5) + (1,2,3/5)
24 -> (8,1,0) + (1,3,0) + (3,2,1) + (3*,2,-1)
-
Here's a case of extension splitting that happens in string theory: E8 -> E6 * SU(3), something that's involved in some symmetry-breaking scenarios.
Dynkin diagram: o - o - o [ - o] - o - o - o - o
Extended Dynkin diagram: o - o - o [ - o] - o - o - o - o - o
Split at root #6: o - o - o [ - o] - o - o (x) o - o
You can see that it's broken down into E6 * SU(3).
Here's what the happens to the fundamental / adjoint irrep of E8, which one gets out of the E8*E8 heterotic superstring:
248 -> (78,1) + (1,8) + (27,3) + (27*,3*)
The first two parts are adjoints and scalars, while the remaining parts are fundamental * fundamental.
adjoint -> (adjoint,scalar) + (scalar, adjoint) + (extra stuff)
but I haven't found anything in the literature on these formulas, though I don't have access to many journal articles.
I've created a Mathematica notebook that calculates Lie-algebra properties that a physicist may find useful, like breakdown of product representations and the aforementioned branching rules: breakdown of a irreducible representation (irrep) into irreps of subgroups.
Nearly all of that notebook's content except for branching-rule details is from Robert N. Cahn's book Semi-Simple Lie Algebras and their Representations, which he has generously placed online. I've been able to calculate Dynkin diagrams, Cartan matrices, irreducible representations' root and weight vectors from their highest weights, and decompositions of products of irreps (irreducible representations). My branching-rule calculations proceed much like the product-rep calculations, but instead with
(root vector in subalgebra) = (matrix).(root vector in original algebra)
(U(1) weight) = (vector).(root vector in original algebra)
The problem I have is demonstrating the correctness of the matrices and vectors I have found. I did so by making some reasonable assumptions and imposing self-consistency in simple cases, like fundamental and adjoint reps. Is anyone familiar enough with the professional literature on Lie-algebra branching rules to point me to some discussions of this question?
-
However, I've found general formulas for the matrices and vectors for all the infinite families (SU, SO, Sp), and explicit values of them for all the exceptional algebras (G2, F4, E6, E7, E8). These are valid for all the breakdowns, as far as I've been able to find out.
I can do demotion of roots, making them into U(1) weights and getting the subalgebras by removing those roots from the originals' Dynkin diagrams.
I can also do removing of roots from extended Dynkin diagrams, using those in Robert Cahn's book.
I can even do some additional cases: SO(7) -> G2 and SO(even) -> SO(odd) * SO(odd)
Does anyone want to see the explicit matrices and the formulas that I've found?
-
Here's a classic case of root demotion: the breaking of the gauge symmetry of the Georgi-Glashow GUT into the Standard-Model gauge symmetry:
SU(5) -> SU(3) * SU(2) * U(1)
Original Dynkin diagram: o - o - o - o
With demoted root (#3): o - o (o) o
Notice that it's broken down into SU(3), U(1), and SU(2) in that order.
I get the correct decompositions of these SU(5) irreps:
1 -> (1,1,0)
5 -> (3,1,2/5) + (1,2,-3/5)
10 -> (3,2,-1/5) + (3*,1,4/5) + (1,1,-6/5)
10* -> (3*,2,1/5) + (3,1,-4/5) + (1,1,6/5)
5* -> (3*,1,-2/5) + (1,2,3/5)
24 -> (8,1,0) + (1,3,0) + (3,2,1) + (3*,2,-1)
-
Here's a case of extension splitting that happens in string theory: E8 -> E6 * SU(3), something that's involved in some symmetry-breaking scenarios.
Dynkin diagram: o - o - o [ - o] - o - o - o - o
Extended Dynkin diagram: o - o - o [ - o] - o - o - o - o - o
Split at root #6: o - o - o [ - o] - o - o (x) o - o
You can see that it's broken down into E6 * SU(3).
Here's what the happens to the fundamental / adjoint irrep of E8, which one gets out of the E8*E8 heterotic superstring:
248 -> (78,1) + (1,8) + (27,3) + (27*,3*)
The first two parts are adjoints and scalars, while the remaining parts are fundamental * fundamental.