what can be supported in a general Jordan Algebra.
"""
+from sage.categories.magmatic_algebras import MagmaticAlgebras
+from sage.structure.element import is_Matrix
+from sage.structure.category_object import normalize_names
+
from sage.algebras.finite_dimensional_algebras.finite_dimensional_algebra import FiniteDimensionalAlgebra
from sage.algebras.finite_dimensional_algebras.finite_dimensional_algebra_element import FiniteDimensionalAlgebraElement
class FiniteDimensionalEuclideanJordanAlgebra(FiniteDimensionalAlgebra):
@staticmethod
- def __classcall__(cls, field, mult_table, names='e', category=None):
- fda = super(FiniteDimensionalEuclideanJordanAlgebra, cls)
- return fda.__classcall_private__(cls,
- field,
- mult_table,
- names,
- category)
+ def __classcall_private__(cls,
+ field,
+ mult_table,
+ names='e',
+ assume_associative=False,
+ category=None,
+ rank=None):
+ n = len(mult_table)
+ mult_table = [b.base_extend(field) for b in mult_table]
+ for b in mult_table:
+ b.set_immutable()
+ if not (is_Matrix(b) and b.dimensions() == (n, n)):
+ raise ValueError("input is not a multiplication table")
+ if not (b.is_symmetric()):
+ # Euclidean jordan algebras are commutative, so left/right
+ # multiplication is the same.
+ raise ValueError("multiplication table must be symmetric")
+ mult_table = tuple(mult_table)
+
+ cat = MagmaticAlgebras(field).FiniteDimensional().WithBasis()
+ cat.or_subcategory(category)
+ if assume_associative:
+ cat = cat.Associative()
+
+ names = normalize_names(n, names)
- def __init__(self, field, mult_table, names='e', category=None):
+ fda = super(FiniteDimensionalEuclideanJordanAlgebra, cls)
+ return fda.__classcall__(cls,
+ field,
+ mult_table,
+ assume_associative=assume_associative,
+ names=names,
+ category=cat,
+ rank=rank)
+
+
+ def __init__(self, field,
+ mult_table,
+ names='e',
+ assume_associative=False,
+ category=None,
+ rank=None):
+ self._rank = rank
fda = super(FiniteDimensionalEuclideanJordanAlgebra, self)
- fda.__init__(field, mult_table, names, category)
+ fda.__init__(field,
+ mult_table,
+ names=names,
+ category=category)
def _repr_(self):
"""
Return a string representation of ``self``.
"""
- return "Euclidean Jordan algebra of degree {} over {}".format(self.degree(), self.base_ring())
+ fmt = "Euclidean Jordan algebra of degree {} over {}"
+ return fmt.format(self.degree(), self.base_ring())
def rank(self):
"""
Return the rank of this EJA.
"""
- raise NotImplementedError
+ if self._rank is None:
+ raise ValueError("no rank specified at genesis")
+ else:
+ return self._rank
class Element(FiniteDimensionalAlgebraElement):
sage: (e0 - e1).degree()
2
+ In the spin factor algebra (of rank two), all elements that
+ aren't multiples of the identity are regular::
+
+ sage: set_random_seed()
+ sage: n = ZZ.random_element(1,10).abs()
+ sage: J = eja_ln(n)
+ sage: x = J.random_element()
+ sage: x == x.coefficient(0)*J.one() or x.degree() == 2
+ True
+
"""
return self.span_of_powers().dimension()
+ def subalgebra_generated_by(self):
+ """
+ Return the subalgebra of the parent EJA generated by this element.
+ """
+ # First get the subspace spanned by the powers of myself...
+ V = self.span_of_powers()
+ F = self.base_ring()
+
+ # Now figure out the entries of the right-multiplication
+ # matrix for the successive basis elements b0, b1,... of
+ # that subspace.
+ mats = []
+ for b_right in V.basis():
+ eja_b_right = self.parent()(b_right)
+ b_right_rows = []
+ # The first row of the right-multiplication matrix by
+ # b1 is what we get if we apply that matrix to b1. The
+ # second row of the right multiplication matrix by b1
+ # is what we get when we apply that matrix to b2...
+ for b_left in V.basis():
+ eja_b_left = self.parent()(b_left)
+ # Multiply in the original EJA, but then get the
+ # coordinates from the subalgebra in terms of its
+ # basis.
+ this_row = V.coordinates((eja_b_left*eja_b_right).vector())
+ b_right_rows.append(this_row)
+ b_right_matrix = matrix(F, b_right_rows)
+ mats.append(b_right_matrix)
+
+ return FiniteDimensionalEuclideanJordanAlgebra(F, mats)
+
+
def minimal_polynomial(self):
- return self.matrix().minimal_polynomial()
+ """
+ EXAMPLES::
+
+ sage: set_random_seed()
+ sage: n = ZZ.random_element(1,10).abs()
+ sage: J = eja_rn(n)
+ sage: x = J.random_element()
+ sage: x.degree() == x.minimal_polynomial().degree()
+ True
+
+ ::
+
+ sage: set_random_seed()
+ sage: n = ZZ.random_element(1,10).abs()
+ sage: J = eja_ln(n)
+ sage: x = J.random_element()
+ sage: x.degree() == x.minimal_polynomial().degree()
+ True
+
+ The minimal polynomial and the characteristic polynomial coincide
+ and are known (see Alizadeh, Example 11.11) for all elements of
+ the spin factor algebra that aren't scalar multiples of the
+ identity::
+
+ sage: set_random_seed()
+ sage: n = ZZ.random_element(2,10).abs()
+ sage: J = eja_ln(n)
+ sage: y = J.random_element()
+ sage: while y == y.coefficient(0)*J.one():
+ ....: y = J.random_element()
+ sage: y0 = y.vector()[0]
+ sage: y_bar = y.vector()[1:]
+ sage: actual = y.minimal_polynomial()
+ sage: x = SR.symbol('x', domain='real')
+ sage: expected = x^2 - 2*y0*x + (y0^2 - norm(y_bar)^2)
+ sage: bool(actual == expected)
+ True
+
+ """
+ V = self.span_of_powers()
+ assoc_subalg = self.subalgebra_generated_by()
+ # Mis-design warning: the basis used for span_of_powers()
+ # and subalgebra_generated_by() must be the same, and in
+ # the same order!
+ subalg_self = assoc_subalg(V.coordinates(self.vector()))
+ return subalg_self.matrix().minimal_polynomial()
+
def characteristic_polynomial(self):
return self.matrix().characteristic_polynomial()
Qs = [ matrix(field, dimension, dimension, lambda k,j: 1*(k == j == i))
for i in xrange(dimension) ]
- return FiniteDimensionalEuclideanJordanAlgebra(field,Qs)
+ return FiniteDimensionalEuclideanJordanAlgebra(field,Qs,rank=dimension)
def eja_ln(dimension, field=QQ):
Qi[0,0] = Qi[0,0] * ~field(2)
Qs.append(Qi)
- return FiniteDimensionalEuclideanJordanAlgebra(field,Qs)
+ return FiniteDimensionalEuclideanJordanAlgebra(field,Qs,rank=2)