Bases: sage.combinat.free_module.CombinatorialFreeModule
The weight ring, which is the group algebra over a weight lattice.
A Weyl character may be regarded as an element of the weight ring. In fact, an element of the weight ring is an element of the Weyl character ring if and only if it is invariant under the action of the Weyl group.
The advantage of the weight ring over the Weyl character ring is that one may conduct calculations in the weight ring that involve sums of weights that are not Weyl group invariant.
EXAMPLES:
sage: A2 = WeylCharacterRing(['A',2])
sage: a2 = WeightRing(A2)
sage: wd = prod(a2(x/2)a2(x/2) for x in a2.space().positive_roots()); wd
a2(1,1,0)  a2(1,0,1)  a2(1,1,0) + a2(1,0,1) + a2(0,1,1)  a2(0,1,1)
sage: chi = A2([5,3,0]); chi
A2(5,3,0)
sage: a2(chi)
a2(1,2,5) + 2*a2(1,3,4) + 2*a2(1,4,3) + a2(1,5,2) + a2(2,1,5)
+ 2*a2(2,2,4) + 3*a2(2,3,3) + 2*a2(2,4,2) + a2(2,5,1) + 2*a2(3,1,4)
+ 3*a2(3,2,3) + 3*a2(3,3,2) + 2*a2(3,4,1) + a2(3,5,0) + a2(3,0,5)
+ 2*a2(4,1,3) + 2*a2(4,2,2) + 2*a2(4,3,1) + a2(4,4,0) + a2(4,0,4)
+ a2(5,1,2) + a2(5,2,1) + a2(5,3,0) + a2(5,0,3) + a2(0,3,5)
+ a2(0,4,4) + a2(0,5,3)
sage: a2(chi)*wd
a2(1,3,6) + a2(1,6,3) + a2(3,1,6)  a2(3,6,1)  a2(6,1,3) + a2(6,3,1)
sage: sum((1)^w.length()*a2([6,3,1]).weyl_group_action(w) for w in a2.space().weyl_group())
a2(1,3,6) + a2(1,6,3) + a2(3,1,6)  a2(3,6,1)  a2(6,1,3) + a2(6,3,1)
sage: a2(chi)*wd == sum((1)^w.length()*a2([6,3,1]).weyl_group_action(w) for w in a2.space().weyl_group())
True
Bases: sage.combinat.free_module.CombinatorialFreeModuleElement
A class for weight ring elements.
Return the Cartan type.
EXAMPLES:
sage: A2=WeylCharacterRing("A2")
sage: a2 = WeightRing(A2)
sage: a2([0,1,0]).cartan_type()
['A', 2]
Assuming that self is invariant under the Weyl group, this will express it as a linear combination of characters. If self is not Weyl group invariant, this method will not terminate.
EXAMPLES:
sage: A2 = WeylCharacterRing(['A',2])
sage: a2 = WeightRing(A2)
sage: W = a2.space().weyl_group()
sage: mu = a2(2,1,0)
sage: nu = sum(mu.weyl_group_action(w) for w in W) ; nu
a2(1,2,0) + a2(1,0,2) + a2(2,1,0) + a2(2,0,1) + a2(0,1,2) + a2(0,2,1)
sage: nu.character()
2*A2(1,1,1) + A2(2,1,0)
Return the result of applying the Demazure operator \(\partial_w\) to self.
INPUT:
If \(w = s_i\) is a simple reflection, the operation \(\partial_w\) sends the weight \(\lambda\) to
where the numerator is divisible the denominator in the weight ring. This is extended by multiplicativity to all \(w\) in the Weyl group.
EXAMPLES:
sage: B2 = WeylCharacterRing("B2",style="coroots")
sage: b2=WeightRing(B2)
sage: b2(1,0).demazure([1])
b2(1,0) + b2(1,2)
sage: b2(1,0).demazure([2])
b2(1,0)
sage: r=b2(1,0).demazure([1,2]); r
b2(1,0) + b2(1,2)
sage: r.demazure([1])
b2(1,0) + b2(1,2)
sage: r.demazure([2])
b2(0,0) + b2(1,0) + b2(1,2) + b2(1,2)
Return the result of applying the DemazureLusztig operator \(T_i\) to self.
INPUT:
If \(R\) is the parent WeightRing, the DemazureLusztig operator \(T_i\) is the linear map \(R \to R\) that sends (for a weight \(\lambda\)) \(R(\lambda)\) to
where the numerator is divisible by the denominator in \(R\). The DemazureLusztig operators give a representation of the Iwahori–Hecke algebra associated to the Weyl group. See
In the examples, we confirm the braid and quadratic relations for type \(B_2\).
EXAMPLES:
sage: P.<v> = PolynomialRing(QQ)
sage: B2 = WeylCharacterRing("B2",style="coroots",base_ring=P); b2 = B2.ambient()
sage: def T1(f) : return f.demazure_lusztig(1,v)
sage: def T2(f) : return f.demazure_lusztig(2,v)
sage: T1(T2(T1(T2(b2(1,1)))))
(v^2v)*b2(0,1) + v^2*b2(1,1)
sage: [T1(T1(f))==(v1)*T1(f)+v*f for f in [b2(0,0), b2(1,0), b2(2,3)]]
[True, True, True]
sage: [T1(T2(T1(T2(b2(i,j))))) == T2(T1(T2(T1(b2(i,j))))) for i in [2..2] for j in [1,1]]
[True, True, True, True, True, True, True, True, True, True]
Instead of an index \(i\) one may use a reduced word or Weyl group element:
sage: b2(1,0).demazure_lusztig([2,1],v)==T2(T1(b2(1,0)))
True
sage: W = B2.space().weyl_group(prefix="s")
sage: [s1,s2]=W.simple_reflections()
sage: b2(1,0).demazure_lusztig(s2*s1,v)==T2(T1(b2(1,0)))
True
Multiplies a weight by \(k\). The operation is extended by linearity to the weight ring.
INPUT:
EXAMPLES:
sage: g2 = WeylCharacterRing("G2",style="coroots").ambient()
sage: g2(2,3).scale(2)
g2(4,6)
Add \(\mu\) to any weight. Extended by linearity to the weight ring.
INPUT:
EXAMPLES:
sage: g2 = WeylCharacterRing("G2",style="coroots").ambient()
sage: [g2(1,2).shift(fw) for fw in g2.fundamental_weights()]
[g2(2,2), g2(1,3)]
Return the action of the Weyl group element w on self.
EXAMPLES:
sage: G2 = WeylCharacterRing(['G',2])
sage: g2 = WeightRing(G2)
sage: L = g2.space()
sage: [fw1, fw2] = L.fundamental_weights()
sage: sum(g2(fw2).weyl_group_action(w) for w in L.weyl_group())
2*g2(2,1,1) + 2*g2(1,1,2) + 2*g2(1,2,1) + 2*g2(1,2,1) + 2*g2(1,1,2) + 2*g2(2,1,1)
Return the Cartan type.
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: WeightRing(A2).cartan_type()
['A', 2]
Return the fundamental weights.
EXAMPLES:
sage: WeightRing(WeylCharacterRing("G2")).fundamental_weights()
Finite family {1: (1, 0, 1), 2: (2, 1, 1)}
Return the index of \(1\).
EXAMPLES:
sage: A3=WeylCharacterRing("A3")
sage: WeightRing(A3).one_basis()
(0, 0, 0, 0)
sage: WeightRing(A3).one()
a3(0,0,0,0)
Return the parent Weyl character ring.
EXAMPLES:
sage: A2=WeylCharacterRing("A2")
sage: a2=WeightRing(A2)
sage: a2.parent()
The Weyl Character Ring of Type A2 with Integer Ring coefficients
sage: a2.parent() == A2
True
Return the positive roots.
EXAMPLES:
sage: WeightRing(WeylCharacterRing("G2")).positive_roots()
[(0, 1, 1), (1, 2, 1), (1, 1, 0), (1, 0, 1), (1, 1, 2), (2, 1, 1)]
Return the product of basis elements indexed by a and b.
EXAMPLES:
sage: A2=WeylCharacterRing("A2")
sage: a2=WeightRing(A2)
sage: a2(1,0,0) * a2(0,1,0) # indirect doctest
a2(1,1,0)
Return the simple roots.
EXAMPLES:
sage: WeightRing(WeylCharacterRing("G2")).simple_roots()
Finite family {1: (0, 1, 1), 2: (1, 2, 1)}
Return some elements of self.
EXAMPLES:
sage: A3=WeylCharacterRing("A3")
sage: a3=WeightRing(A3)
sage: a3.some_elements()
[a3(1,0,0,0), a3(1,1,0,0), a3(1,1,1,0)]
Return the weight space realization associated to self.
EXAMPLES:
sage: E8 = WeylCharacterRing(['E',8])
sage: e8 = WeightRing(E8)
sage: e8.space()
Ambient space of the Root system of type ['E', 8]
Return the parent Weyl Character Ring. A synonym for self.parent().
EXAMPLES:
sage: A2=WeylCharacterRing("A2")
sage: a2=WeightRing(A2)
sage: a2.weyl_character_ring()
The Weyl Character Ring of Type A2 with Integer Ring coefficients
Return a string representing the irreducible character with highest weight vector wt. Uses coroot notation if the associated Weyl character ring is defined with style="coroots".
EXAMPLES:
sage: G2 = WeylCharacterRing("G2")
sage: [G2.ambient().wt_repr(x) for x in G2.fundamental_weights()]
['g2(1,0,1)', 'g2(2,1,1)']
sage: G2 = WeylCharacterRing("G2",style="coroots")
sage: [G2.ambient().wt_repr(x) for x in G2.fundamental_weights()]
['g2(1,0)', 'g2(0,1)']
Bases: sage.combinat.free_module.CombinatorialFreeModule
A class for rings of Weyl characters.
Let \(K\) be a compact Lie group, which we assume is semisimple and simplyconnected. Its complexified Lie algebra \(L\) is the Lie algebra of a complex analytic Lie group \(G\). The following three categories are equivalent: finitedimensional representations of \(K\); finitedimensional representations of \(L\); and finitedimensional analytic representations of \(G\). In every case, there is a parametrization of the irreducible representations by their highest weight vectors. For this theory of Weyl, see (for example):
Computations that you can do with these include computing their weight multiplicities, products (thus decomposing the tensor product of a representation into irreducibles) and branching rules (restriction to a smaller group).
There is associated with \(K\), \(L\) or \(G\) as above a lattice, the weight lattice, whose elements (called weights) are characters of a Cartan subgroup or subalgebra. There is an action of the Weyl group \(W\) on the lattice, and elements of a fixed fundamental domain for \(W\), the positive Weyl chamber, are called dominant. There is for each representation a unique highest dominant weight that occurs with nonzero multiplicity with respect to a certain partial order, and it is called the highest weight vector.
EXAMPLES:
sage: L = RootSystem("A2").ambient_space()
sage: [fw1,fw2] = L.fundamental_weights()
sage: R = WeylCharacterRing(['A',2], prefix="R")
sage: [R(1),R(fw1),R(fw2)]
[R(0,0,0), R(1,0,0), R(1,1,0)]
Here R(1), R(fw1), and R(fw2) are irreducible representations with highest weight vectors \(0\), \(\Lambda_1\), and \(\Lambda_2\) respecitively (the first two fundamental weights).
For type \(A\) (also \(G_2\), \(F_4\), \(E_6\) and \(E_7\)) we will take as the weight lattice not the weight lattice of the semisimple group, but for a larger one. For type \(A\), this means we are concerned with the representation theory of \(K = U(n)\) or \(G = GL(n, \CC)\) rather than \(SU(n)\) or \(SU(n, \CC)\). This is useful since the representation theory of \(GL(n)\) is ubiquitous, and also since we may then represent the fundamental weights (in sage.combinat.root_system.root_system) by vectors with integer entries. If you are only interested in \(SL(3)\), say, use WeylCharacterRing(['A',2]) as above but be aware that R([a,b,c]) and R([a+1,b+1,c+1]) represent the same character of \(SL(3)\) since R([1,1,1]) is the determinant.
For more information, see the thematic tutorial Lie Methods and Related Combinatorics in Sage, available at:
http://www.sagemath.org/doc/thematic_tutorials/lie.html
Bases: sage.combinat.free_module.CombinatorialFreeModuleElement
A class for Weyl characters.
Return the \(r\)th Adams operation of self.
INPUT:
This is a virtual character, whose weights are the weights of self, each multiplied by \(r\).
EXAMPLES:
sage: A2=WeylCharacterRing("A2")
sage: A2(1,1,0).adams_operation(3)
A2(2,2,2)  A2(3,2,1) + A2(3,3,0)
Return the restriction of the character to the subalgebra. If no rule is specified, we will try to specify one.
INPUT:
See branch_weyl_character() for more information about branching rules.
EXAMPLES:
sage: B3 = WeylCharacterRing(['B',3])
sage: A2 = WeylCharacterRing(['A',2])
sage: [B3(w).branch(A2,rule="levi") for w in B3.fundamental_weights()]
[A2(0,0,0) + A2(1,0,0) + A2(0,0,1),
A2(0,0,0) + A2(1,0,0) + A2(1,1,0) + A2(1,0,1) + A2(0,1,1) + A2(0,0,1),
A2(1/2,1/2,1/2) + A2(1/2,1/2,1/2) + A2(1/2,1/2,1/2) + A2(1/2,1/2,1/2)]
Return the Cartan type of self.
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: A2([1,0,0]).cartan_type()
['A', 2]
The degree of self, that is, the dimension of module.
EXAMPLES:
sage: B3 = WeylCharacterRing(['B',3])
sage: [B3(x).degree() for x in B3.fundamental_weights()]
[7, 21, 8]
Return the \(k\)th exterior power of self.
INPUT:
The algorithm is based on the identity \(k e_k = \sum_{r=1}^k (1)^{k1} p_k e_{kr}\) relating the powersum and elementary symmetric polynomials. Applying this to the eigenvalues of an element of the parent Lie group in the representation self, the \(e_k\) become exterior powers and the \(p_k\) become Adams operations, giving an efficient recursive implementation.
EXAMPLES:
sage: B3=WeylCharacterRing("B3",style="coroots")
sage: spin=B3(0,0,1)
sage: spin.exterior_power(6)
B3(1,0,0) + B3(0,1,0)
Return the exterior square of the character.
EXAMPLES:
sage: A2 = WeylCharacterRing("A2",style="coroots")
sage: A2(1,0).exterior_square()
A2(0,1)
Return:
The FrobeniusSchur indicator of a character \(\chi\) of a compact group \(G\) is the Haar integral over the group of \(\chi(g^2)\). Its value is 1, 1 or 0. This method computes it for irreducible characters of compact Lie groups by checking whether the symmetric and exterior square characters contain the trivial character.
Todo
Try to compute this directly without actually calculating the full symmetric and exterior squares.
EXAMPLES:
sage: B2 = WeylCharacterRing("B2",style="coroots")
sage: B2(1,0).frobenius_schur_indicator()
1
sage: B2(0,1).frobenius_schur_indicator()
1
Compute the inner product with another character.
The irreducible characters are an orthonormal basis with respect to the usual inner product of characters, interpreted as functions on a compact Lie group, by Schur orthogonality.
INPUT:
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: [f1,f2]=A2.fundamental_weights()
sage: r1 = A2(f1)*A2(f2); r1
A2(1,1,1) + A2(2,1,0)
sage: r2 = A2(f1)^3; r2
A2(1,1,1) + 2*A2(2,1,0) + A2(3,0,0)
sage: r1.inner_product(r2)
3
Return the multiplicity of the trivial representation in self.
Multiplicities of other irreducibles may be obtained using multiplicity().
EXAMPLES:
sage: A2 = WeylCharacterRing("A2",style="coroots")
sage: rep = A2(1,0)^2*A2(0,1)^2; rep
2*A2(0,0) + A2(0,3) + 4*A2(1,1) + A2(3,0) + A2(2,2)
sage: rep.invariant_degree()
2
Return whether self is an irreducible character.
EXAMPLES:
sage: B3 = WeylCharacterRing(['B',3])
sage: [B3(x).is_irreducible() for x in B3.fundamental_weights()]
[True, True, True]
sage: sum(B3(x) for x in B3.fundamental_weights()).is_irreducible()
False
Return the multiplicity of the irreducible other in self.
INPUT:
EXAMPLES:
sage: B2 = WeylCharacterRing("B2",style="coroots")
sage: rep = B2(1,1)^2; rep
B2(0,0) + B2(1,0) + 2*B2(0,2) + B2(2,0) + 2*B2(1,2) + B2(0,4) + B2(3,0) + B2(2,2)
sage: rep.multiplicity(B2(0,2))
2
Return the \(k\)th symmetric power of self.
INPUT:
The algorithm is based on the identity \(k h_k = \sum_{r=1}^k p_k h_{kr}\) relating the powersum and complete symmetric polynomials. Applying this to the eigenvalues of an element of the parent Lie group in the representation self, the \(h_k\) become symmetric powers and the \(p_k\) become Adams operations, giving an efficient recursive implementation.
EXAMPLES:
sage: B3=WeylCharacterRing("B3",style="coroots")
sage: spin=B3(0,0,1)
sage: spin.symmetric_power(6)
B3(0,0,0) + B3(0,0,2) + B3(0,0,4) + B3(0,0,6)
Return the symmetric square of the character.
EXAMPLES:
sage: A2 = WeylCharacterRing("A2",style="coroots")
sage: A2(1,0).symmetric_square()
A2(2,0)
Produce the dictionary of weight multiplicities for the Weyl character self. The character does not have to be irreducible.
EXAMPLES:
sage: from pprint import pprint
sage: B2=WeylCharacterRing("B2",style="coroots")
sage: pprint(B2(0,1).weight_multiplicities())
{(1/2, 1/2): 1, (1/2, 1/2): 1, (1/2, 1/2): 1, (1/2, 1/2): 1}
Returns the adjoint representation as an element of the WeylCharacterRing”.
EXAMPLES:
sage: G2=WeylCharacterRing("G2",style="coroots")
sage: G2.adjoint_representation()
G2(0,1)
Returns the weight ring of self.
EXAMPLES:
sage: WeylCharacterRing("A2").ambient()
The Weight ring attached to The Weyl Character Ring of Type A2 with Integer Ring coefficients
Return the base ring of self.
EXAMPLES:
sage: R = WeylCharacterRing(['A',3], base_ring = CC); R.base_ring()
Complex Field with 53 bits of precision
Return the Cartan type of self.
EXAMPLES:
sage: WeylCharacterRing("A2").cartan_type()
['A', 2]
Construct a Weyl character from an invariant linear combination of weights.
INPUT:
OUTPUT: the corresponding Weyl character
EXAMPLES:
sage: from pprint import pprint
sage: A2 = WeylCharacterRing("A2")
sage: v = A2._space([3,1,0]); v
(3, 1, 0)
sage: d = dict([(x,1) for x in v.orbit()]); pprint(d)
{(1, 3, 0): 1,
(1, 0, 3): 1,
(3, 1, 0): 1,
(3, 0, 1): 1,
(0, 1, 3): 1,
(0, 3, 1): 1}
sage: A2.char_from_weights(d)
A2(2,1,1)  A2(2,2,0) + A2(3,1,0)
Compute the Demazure character.
INPUT:
Produces the Demazure character with highest weight hwv and word as an element of the weight ring. Only available if style="coroots". The Demazure operators are also available as methods of WeightRing elements, and as methods of crystals. Given a CrystalOfTableaux with given highest weight vector, the Demazure method on the crystal will give the equivalent of this method, except that the Demazure character of the crystal is given as a sum of monomials instead of an element of the WeightRing.
See WeightRing.Element.demazure() and sage.categories.classical_crystals.ClassicalCrystals.ParentMethods.demazure_character()
EXAMPLES:
sage: A2=WeylCharacterRing("A2",style="coroots")
sage: h=sum(A2.fundamental_weights()); h
(2, 1, 0)
sage: A2.demazure_character(h,word=[1,2])
a2(0,0) + a2(2,1) + a2(2,1) + a2(1,1) + a2(1,2)
sage: A2.demazure_character((1,1),word=[1,2])
a2(0,0) + a2(2,1) + a2(2,1) + a2(1,1) + a2(1,2)
Auxiliary function for product_on_basis().
Return a pair \([\epsilon, b]\) where \(b\) is a dominant weight and \(\epsilon\) is 0, 1 or 1. To describe \(b\), let \(w\) be an element of the Weyl group such that \(w(a + \rho)\) is dominant. If \(w(a + \rho)  \rho\) is dominant, then \(\epsilon\) is the sign of \(w\) and \(b\) is \(w(a + \rho)  \rho\). Otherwise, \(\epsilon\) is zero.
INPUT:
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: weights = sorted(A2(2,1,0).weight_multiplicities().keys(), key=str); weights
[(0, 1, 2), (0, 2, 1), (1, 0, 2), (1, 1, 1), (1, 2, 0), (2, 0, 1), (2, 1, 0)]
sage: [A2.dot_reduce(x) for x in weights]
[[0, (0, 0, 0)], [1, (1, 1, 1)], [1, (1, 1, 1)], [1, (1, 1, 1)], [0, (0, 0, 0)], [0, (0, 0, 0)], [1, (2, 1, 0)]]
Return the Dynkin diagram of self.
EXAMPLES:
sage: WeylCharacterRing("E7").dynkin_diagram()
O 2


OOOOOO
1 3 4 5 6 7
E7
Return the extended Dynkin diagram, which is the Dynkin diagram of the corresponding untwisted affine type.
EXAMPLES:
sage: WeylCharacterRing("E7").extended_dynkin_diagram()
O 2


OOOOOOO
0 1 3 4 5 6 7
E7~
Return the fundamental weights.
EXAMPLES:
sage: WeylCharacterRing("G2").fundamental_weights()
Finite family {1: (1, 0, 1), 2: (2, 1, 1)}
Return the highest_root.
EXAMPLES:
sage: WeylCharacterRing("G2").highest_root()
(2, 1, 1)
Return a string representing the irreducible character with highest weight vector hwv.
EXAMPLES:
sage: B3 = WeylCharacterRing("B3")
sage: [B3.irr_repr(v) for v in B3.fundamental_weights()]
['B3(1,0,0)', 'B3(1,1,0)', 'B3(1/2,1/2,1/2)']
sage: B3 = WeylCharacterRing("B3", style="coroots")
sage: [B3.irr_repr(v) for v in B3.fundamental_weights()]
['B3(1,0,0)', 'B3(0,1,0)', 'B3(0,0,1)']
The embedding of self into its weight ring.
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: A2.lift
Generic morphism:
From: The Weyl Character Ring of Type A2 with Integer Ring coefficients
To: The Weight ring attached to The Weyl Character Ring of Type A2 with Integer Ring coefficients
sage: x = A2(2,1,1)  A2(2,2,0) + A2(3,1,0)
sage: A2.lift(x)
a2(1,3,0) + a2(1,0,3) + a2(3,1,0) + a2(3,0,1) + a2(0,1,3) + a2(0,3,1)
As a shortcut, you may also do:
sage: x.lift()
a2(1,3,0) + a2(1,0,3) + a2(3,1,0) + a2(3,0,1) + a2(0,1,3) + a2(0,3,1)
Or even:
sage: a2 = WeightRing(A2)
sage: a2(x)
a2(1,3,0) + a2(1,0,3) + a2(3,1,0) + a2(3,0,1) + a2(0,1,3) + a2(0,3,1)
Expand the basis element indexed by the weight irr into the weight ring of self.
INPUT:
This is used to implement lift().
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: v = A2._space([2,1,0]); v
(2, 1, 0)
sage: A2.lift_on_basis(v)
2*a2(1,1,1) + a2(1,2,0) + a2(1,0,2) + a2(2,1,0) + a2(2,0,1) + a2(0,1,2) + a2(0,2,1)
This is consistent with the analoguous calculation with symmetric Schur functions:
sage: s = SymmetricFunctions(QQ).s()
sage: s[2,1].expand(3)
x0^2*x1 + x0*x1^2 + x0^2*x2 + 2*x0*x1*x2 + x1^2*x2 + x0*x2^2 + x1*x2^2
INPUT:
Returns a branching rule. In rare cases where there is more than one maximal subgroup (up to outer automorphisms) with the given Cartan type, the function returns a list of branching rules.
EXAMPLES:
sage: WeylCharacterRing("E7").maximal_subgroup("A2")
miscellaneous branching rule E7 => A2
sage: WeylCharacterRing("E7").maximal_subgroup("A1")
[iii branching rule E7 => A1, iv branching rule E7 => A1]
For more information, see the related method maximal_subgroups().
This method is only available if the Cartan type of self is irreducible and of rank no greater than 8. This method produces a list of the maximal subgroups of self, up to (possibly outer) automorphisms. Each line in the output gives the Cartan type of a maximal subgroup followed by a command that creates the branching rule.
EXAMPLES:
sage: WeylCharacterRing("E6").maximal_subgroups()
D5:branching_rule("E6","D5","levi")
C4:branching_rule("E6","C4","symmetric")
F4:branching_rule("E6","F4","symmetric")
A2:branching_rule("E6","A2","miscellaneous")
G2:branching_rule("E6","G2","miscellaneous")
A2xG2:branching_rule("E6","A2xG2","miscellaneous")
A1xA5:branching_rule("E6","A1xA5","extended")
A2xA2xA2:branching_rule("E6","A2xA2xA2","extended")
Note that there are other embeddings of (for example \(A_2\) into \(E_6\) as nonmaximal subgroups. These embeddings may be constructed by composing branching rules through various subgroups.
Once you know which maximal subgroup you are interested in, to create the branching rule, you may either paste the command to the right of the colon from the above output onto the command line, or alternatively invoke the related method maximal_subgroup():
sage: branching_rule("E6","G2","miscellaneous")
miscellaneous branching rule E6 => G2
sage: WeylCharacterRing("E6").maximal_subgroup("G2")
miscellaneous branching rule E6 => G2
It is believed that the list of maximal subgroups is complete, except that some subgroups may be not be invariant under outer automorphisms. It is reasonable to want a list of maximal subgroups that is complete up to conjugation, but to obtain such a list you may have to apply outer automorphisms. The group of outer automorphisms modulo inner automorphisms is isomorphic to the group of symmetries of the Dynkin diagram, and these are available as branching rules. The following example shows that while a branching rule from \(D_4\) to \(A_1 imes C_2\) is supplied, another different one may be obtained by composing it with the triality automorphism of \(D_4\):
sage: [D4,A1xC2]=[WeylCharacterRing(x,style="coroots") for x in ["D4","A1xC2"]]
sage: fw = D4.fundamental_weights()
sage: b = D4.maximal_subgroup("A1xC2")
sage: [D4(fw).branch(A1xC2,rule=b) for fw in D4.fundamental_weights()]
[A1xC2(1,1,0),
A1xC2(2,0,0) + A1xC2(2,0,1) + A1xC2(0,2,0),
A1xC2(1,1,0),
A1xC2(2,0,0) + A1xC2(0,0,1)]
sage: b1 = branching_rule("D4","D4","triality")*b
sage: [D4(fw).branch(A1xC2,rule=b1) for fw in D4.fundamental_weights()]
[A1xC2(1,1,0),
A1xC2(2,0,0) + A1xC2(2,0,1) + A1xC2(0,2,0),
A1xC2(2,0,0) + A1xC2(0,0,1),
A1xC2(1,1,0)]
Return the index of 1 in self.
EXAMPLES:
sage: WeylCharacterRing("A3").one_basis()
(0, 0, 0, 0)
sage: WeylCharacterRing("A3").one()
A3(0,0,0,0)
Return the positive roots.
EXAMPLES:
sage: WeylCharacterRing("G2").positive_roots()
[(0, 1, 1), (1, 2, 1), (1, 1, 0), (1, 0, 1), (1, 1, 2), (2, 1, 1)]
Compute the tensor product of two irreducible representations a and b.
EXAMPLES:
sage: D4 = WeylCharacterRing(['D',4])
sage: spin_plus = D4(1/2,1/2,1/2,1/2)
sage: spin_minus = D4(1/2,1/2,1/2,1/2)
sage: spin_plus * spin_minus # indirect doctest
D4(1,0,0,0) + D4(1,1,1,0)
sage: spin_minus * spin_plus
D4(1,0,0,0) + D4(1,1,1,0)
Uses the BrauerKlimyk method.
Return the rank.
EXAMPLES:
sage: WeylCharacterRing("G2").rank()
2
The partial inverse map from the weight ring into self.
EXAMPLES:
sage: A2 = WeylCharacterRing("A2")
sage: a2 = WeightRing(A2)
sage: A2.retract
Generic morphism:
From: The Weight ring attached to The Weyl Character Ring of Type A2 with Integer Ring coefficients
To: The Weyl Character Ring of Type A2 with Integer Ring coefficients
sage: v = A2._space([3,1,0]); v
(3, 1, 0)
sage: chi = a2.sum_of_monomials(v.orbit()); chi
a2(1,3,0) + a2(1,0,3) + a2(3,1,0) + a2(3,0,1) + a2(0,1,3) + a2(0,3,1)
sage: A2.retract(chi)
A2(2,1,1)  A2(2,2,0) + A2(3,1,0)
The input should be invariant:
sage: A2.retract(a2.monomial(v))
Traceback (most recent call last):
...
ValueError: multiplicity dictionary may not be Weyl group invariant
As a shortcut, you may use conversion:
sage: A2(chi)
A2(2,1,1)  A2(2,2,0) + A2(3,1,0)
sage: A2(a2.monomial(v))
Traceback (most recent call last):
...
ValueError: multiplicity dictionary may not be Weyl group invariant
Return the simple coroots.
EXAMPLES:
sage: WeylCharacterRing("G2").simple_coroots()
Finite family {1: (0, 1, 1), 2: (1/3, 2/3, 1/3)}
Return the simple roots.
EXAMPLES:
sage: WeylCharacterRing("G2").simple_roots()
Finite family {1: (0, 1, 1), 2: (1, 2, 1)}
Return some elements of self.
EXAMPLES:
sage: WeylCharacterRing("A3").some_elements()
[A3(1,0,0,0), A3(1,1,0,0), A3(1,1,1,0)]
Return the weight space associated to self.
EXAMPLES:
sage: WeylCharacterRing(['E',8]).space()
Ambient space of the Root system of type ['E', 8]
Return the dictionary of multiplicities for the irreducible character with highest weight \(\lambda\).
The weight multiplicities are computed by the Freudenthal multiplicity formula. The algorithm is based on recursion relation that is stated, for example, in Humphrey’s book on Lie Algebras. The multiplicities are invariant under the Weyl group, so to compute them it would be sufficient to compute them for the weights in the positive Weyl chamber. However after some testing it was found to be faster to compute every weight using the recursion, since the use of the Weyl group is expensive in its current implementation.
INPUT:
EXAMPLES:
sage: from pprint import pprint
sage: pprint(WeylCharacterRing("A2")(2,1,0).weight_multiplicities()) # indirect doctest
{(1, 1, 1): 2, (1, 2, 0): 1, (1, 0, 2): 1, (2, 1, 0): 1,
(2, 0, 1): 1, (0, 1, 2): 1, (0, 2, 1): 1}