names='e',
assume_associative=False,
category=None,
- rank=None):
+ rank=None,
+ natural_basis=None):
n = len(mult_table)
mult_table = [b.base_extend(field) for b in mult_table]
for b in mult_table:
assume_associative=assume_associative,
names=names,
category=cat,
- rank=rank)
+ rank=rank,
+ natural_basis=natural_basis)
def __init__(self, field,
names='e',
assume_associative=False,
category=None,
- rank=None):
+ rank=None,
+ natural_basis=None):
"""
EXAMPLES:
"""
self._rank = rank
+ self._natural_basis = natural_basis
fda = super(FiniteDimensionalEuclideanJordanAlgebra, self)
fda.__init__(field,
mult_table,
fmt = "Euclidean Jordan algebra of degree {} over {}"
return fmt.format(self.degree(), self.base_ring())
+
+ def natural_basis(self):
+ """
+ Return a more-natural representation of this algebra's basis.
+
+ Every finite-dimensional Euclidean Jordan Algebra is a direct
+ sum of five simple algebras, four of which comprise Hermitian
+ matrices. This method returns the original "natural" basis
+ for our underlying vector space. (Typically, the natural basis
+ is used to construct the multiplication table in the first place.)
+
+ Note that this will always return a matrix. The standard basis
+ in `R^n` will be returned as `n`-by-`1` column matrices.
+
+ EXAMPLES::
+
+ sage: J = RealSymmetricSimpleEJA(2)
+ sage: J.basis()
+ Family (e0, e1, e2)
+ sage: J.natural_basis()
+ (
+ [1 0] [0 1] [0 0]
+ [0 0], [1 0], [0 1]
+ )
+
+ ::
+
+ sage: J = JordanSpinSimpleEJA(2)
+ sage: J.basis()
+ Family (e0, e1)
+ sage: J.natural_basis()
+ (
+ [1] [0]
+ [0], [1]
+ )
+
+ """
+ if self._natural_basis is None:
+ return tuple( b.vector().column() for b in self.basis() )
+ else:
+ return self._natural_basis
+
+
def rank(self):
"""
Return the rank of this EJA.
sage: set_random_seed()
sage: x = random_eja().random_element()
- sage: x.matrix()*x.vector() == (x^2).vector()
+ sage: x.operator_matrix()*x.vector() == (x^2).vector()
True
A few examples of power-associativity::
sage: x = random_eja().random_element()
sage: m = ZZ.random_element(0,10)
sage: n = ZZ.random_element(0,10)
- sage: Lxm = (x^m).matrix()
- sage: Lxn = (x^n).matrix()
+ sage: Lxm = (x^m).operator_matrix()
+ sage: Lxn = (x^n).operator_matrix()
sage: Lxm*Lxn == Lxn*Lxm
True
elif n == 1:
return self
else:
- return A.element_class(A, (self.matrix()**(n-1))*self.vector())
+ return A( (self.operator_matrix()**(n-1))*self.vector() )
def characteristic_polynomial(self):
if not other in self.parent():
raise ArgumentError("'other' must live in the same algebra")
- A = self.matrix()
- B = other.matrix()
+ A = self.operator_matrix()
+ B = other.operator_matrix()
return (A*B == B*A)
return self.span_of_powers().dimension()
- def matrix(self):
- """
- Return the matrix that represents left- (or right-)
- multiplication by this element in the parent algebra.
-
- We have to override this because the superclass method
- returns a matrix that acts on row vectors (that is, on
- the right).
-
- EXAMPLES:
-
- Test the first polarization identity from my notes, Koecher Chapter
- III, or from Baes (2.3)::
-
- sage: set_random_seed()
- sage: J = random_eja()
- sage: x = J.random_element()
- sage: y = J.random_element()
- sage: Lx = x.matrix()
- sage: Ly = y.matrix()
- sage: Lxx = (x*x).matrix()
- sage: Lxy = (x*y).matrix()
- sage: bool(2*Lx*Lxy + Ly*Lxx == 2*Lxy*Lx + Lxx*Ly)
- True
-
- Test the second polarization identity from my notes or from
- Baes (2.4)::
-
- sage: set_random_seed()
- sage: J = random_eja()
- sage: x = J.random_element()
- sage: y = J.random_element()
- sage: z = J.random_element()
- sage: Lx = x.matrix()
- sage: Ly = y.matrix()
- sage: Lz = z.matrix()
- sage: Lzy = (z*y).matrix()
- sage: Lxy = (x*y).matrix()
- sage: Lxz = (x*z).matrix()
- sage: bool(Lx*Lzy + Lz*Lxy + Ly*Lxz == Lzy*Lx + Lxy*Lz + Lxz*Ly)
- True
-
- Test the third polarization identity from my notes or from
- Baes (2.5)::
-
- sage: set_random_seed()
- sage: J = random_eja()
- sage: u = J.random_element()
- sage: y = J.random_element()
- sage: z = J.random_element()
- sage: Lu = u.matrix()
- sage: Ly = y.matrix()
- sage: Lz = z.matrix()
- sage: Lzy = (z*y).matrix()
- sage: Luy = (u*y).matrix()
- sage: Luz = (u*z).matrix()
- sage: Luyz = (u*(y*z)).matrix()
- sage: lhs = Lu*Lzy + Lz*Luy + Ly*Luz
- sage: rhs = Luyz + Ly*Lu*Lz + Lz*Lu*Ly
- sage: bool(lhs == rhs)
- True
-
- """
- fda_elt = FiniteDimensionalAlgebraElement(self.parent(), self)
- return fda_elt.matrix().transpose()
-
-
def minimal_polynomial(self):
"""
EXAMPLES::
return elt.minimal_polynomial()
+ def natural_representation(self):
+ """
+ Return a more-natural representation of this element.
+
+ Every finite-dimensional Euclidean Jordan Algebra is a
+ direct sum of five simple algebras, four of which comprise
+ Hermitian matrices. This method returns the original
+ "natural" representation of this element as a Hermitian
+ matrix, if it has one. If not, you get the usual representation.
+
+ EXAMPLES::
+
+ sage: J = ComplexHermitianSimpleEJA(3)
+ sage: J.one()
+ e0 + e5 + e8
+ sage: J.one().natural_representation()
+ [1 0 0 0 0 0]
+ [0 1 0 0 0 0]
+ [0 0 1 0 0 0]
+ [0 0 0 1 0 0]
+ [0 0 0 0 1 0]
+ [0 0 0 0 0 1]
+
+ """
+ B = self.parent().natural_basis()
+ W = B[0].matrix_space()
+ return W.linear_combination(zip(self.vector(), B))
+
+
+ def operator_matrix(self):
+ """
+ Return the matrix that represents left- (or right-)
+ multiplication by this element in the parent algebra.
+
+ We have to override this because the superclass method
+ returns a matrix that acts on row vectors (that is, on
+ the right).
+
+ EXAMPLES:
+
+ Test the first polarization identity from my notes, Koecher Chapter
+ III, or from Baes (2.3)::
+
+ sage: set_random_seed()
+ sage: J = random_eja()
+ sage: x = J.random_element()
+ sage: y = J.random_element()
+ sage: Lx = x.operator_matrix()
+ sage: Ly = y.operator_matrix()
+ sage: Lxx = (x*x).operator_matrix()
+ sage: Lxy = (x*y).operator_matrix()
+ sage: bool(2*Lx*Lxy + Ly*Lxx == 2*Lxy*Lx + Lxx*Ly)
+ True
+
+ Test the second polarization identity from my notes or from
+ Baes (2.4)::
+
+ sage: set_random_seed()
+ sage: J = random_eja()
+ sage: x = J.random_element()
+ sage: y = J.random_element()
+ sage: z = J.random_element()
+ sage: Lx = x.operator_matrix()
+ sage: Ly = y.operator_matrix()
+ sage: Lz = z.operator_matrix()
+ sage: Lzy = (z*y).operator_matrix()
+ sage: Lxy = (x*y).operator_matrix()
+ sage: Lxz = (x*z).operator_matrix()
+ sage: bool(Lx*Lzy + Lz*Lxy + Ly*Lxz == Lzy*Lx + Lxy*Lz + Lxz*Ly)
+ True
+
+ Test the third polarization identity from my notes or from
+ Baes (2.5)::
+
+ sage: set_random_seed()
+ sage: J = random_eja()
+ sage: u = J.random_element()
+ sage: y = J.random_element()
+ sage: z = J.random_element()
+ sage: Lu = u.operator_matrix()
+ sage: Ly = y.operator_matrix()
+ sage: Lz = z.operator_matrix()
+ sage: Lzy = (z*y).operator_matrix()
+ sage: Luy = (u*y).operator_matrix()
+ sage: Luz = (u*z).operator_matrix()
+ sage: Luyz = (u*(y*z)).operator_matrix()
+ sage: lhs = Lu*Lzy + Lz*Luy + Ly*Luz
+ sage: rhs = Luyz + Ly*Lu*Lz + Lz*Lu*Ly
+ sage: bool(lhs == rhs)
+ True
+
+ """
+ fda_elt = FiniteDimensionalAlgebraElement(self.parent(), self)
+ return fda_elt.matrix().transpose()
+
+
def quadratic_representation(self, other=None):
"""
Return the quadratic representation of this element.
elif not other in self.parent():
raise ArgumentError("'other' must live in the same algebra")
- return ( self.matrix()*other.matrix()
- + other.matrix()*self.matrix()
- - (self*other).matrix() )
+ L = self.operator_matrix()
+ M = other.operator_matrix()
+ return ( L*M + M*L - (self*other).operator_matrix() )
def span_of_powers(self):
sage: set_random_seed()
sage: x = random_eja().random_element()
sage: u = x.subalgebra_generated_by().random_element()
- sage: u.matrix()*u.vector() == (u**2).vector()
+ sage: u.operator_matrix()*u.vector() == (u**2).vector()
True
"""
s = 0
minimal_dim = V.dimension()
for i in xrange(1, V.dimension()):
- this_dim = (u**i).matrix().image().dimension()
+ this_dim = (u**i).operator_matrix().image().dimension()
if this_dim < minimal_dim:
minimal_dim = this_dim
s = i
# Beware, solve_right() means that we're using COLUMN vectors.
# Our FiniteDimensionalAlgebraElement superclass uses rows.
u_next = u**(s+1)
- A = u_next.matrix()
+ A = u_next.operator_matrix()
c_coordinates = A.solve_right(u_next.vector())
# Now c_coordinates is the idempotent we want, but it's in
# Beware, orthogonal but not normalized!
Sij = Eij + Eij.transpose()
S.append(Sij)
- return S
+ return tuple(S)
def _complex_hermitian_basis(n, field=QQ):
S.append(Sij_real)
Sij_imag = _embed_complex_matrix(I*Eij - I*Eij.transpose())
S.append(Sij_imag)
- return S
+ return tuple(S)
def _multiplication_table_from_matrix_basis(basis):
multiplication on the right is matrix multiplication. Given a basis
for the underlying matrix space, this function returns a
multiplication table (obtained by looping through the basis
- elements) for an algebra of those matrices.
+ elements) for an algebra of those matrices. A reordered copy
+ of the basis is also returned to work around the fact that
+ the ``span()`` in this function will change the order of the basis
+ from what we think it is, to... something else.
"""
# In S^2, for example, we nominally have four coordinates even
# though the space is of dimension three only. The vector space V
# Taking the span above reorders our basis (thanks, jerk!) so we
# need to put our "matrix basis" in the same order as the
# (reordered) vector basis.
- S = [ vec2mat(b) for b in W.basis() ]
+ S = tuple( vec2mat(b) for b in W.basis() )
Qs = []
for s in S:
Q = matrix(field, W.dimension(), Q_rows)
Qs.append(Q)
- return Qs
+ return (Qs, S)
def _embed_complex_matrix(M):
"""
S = _real_symmetric_basis(n, field=field)
- Qs = _multiplication_table_from_matrix_basis(S)
+ (Qs, T) = _multiplication_table_from_matrix_basis(S)
- return FiniteDimensionalEuclideanJordanAlgebra(field,Qs,rank=n)
+ return FiniteDimensionalEuclideanJordanAlgebra(field,
+ Qs,
+ rank=n,
+ natural_basis=T)
def ComplexHermitianSimpleEJA(n, field=QQ):
"""
S = _complex_hermitian_basis(n)
- Qs = _multiplication_table_from_matrix_basis(S)
- return FiniteDimensionalEuclideanJordanAlgebra(field, Qs, rank=n)
+ (Qs, T) = _multiplication_table_from_matrix_basis(S)
+ return FiniteDimensionalEuclideanJordanAlgebra(field,
+ Qs,
+ rank=n,
+ natural_basis=T)
def QuaternionHermitianSimpleEJA(n):
projects / sage.d.git / blobdiff