assume_associative=False,
category=None,
rank=None,
- natural_basis=None):
+ natural_basis=None,
+ inner_product=None):
n = len(mult_table)
mult_table = [b.base_extend(field) for b in mult_table]
for b in mult_table:
names=names,
category=cat,
rank=rank,
- natural_basis=natural_basis)
+ natural_basis=natural_basis,
+ inner_product=inner_product)
def __init__(self, field,
assume_associative=False,
category=None,
rank=None,
- natural_basis=None):
+ natural_basis=None,
+ inner_product=None):
"""
EXAMPLES:
"""
self._rank = rank
self._natural_basis = natural_basis
+ self._inner_product = inner_product
fda = super(FiniteDimensionalEuclideanJordanAlgebra, self)
fda.__init__(field,
mult_table,
return fmt.format(self.degree(), self.base_ring())
+ def inner_product(self, x, y):
+ """
+ The inner product associated with this Euclidean Jordan algebra.
+
+ Will default to the trace inner product if nothing else.
+ """
+ if (not x in self) or (not y in self):
+ raise TypeError("arguments must live in this algebra")
+ if self._inner_product is None:
+ return x.trace_inner_product(y)
+ else:
+ return self._inner_product(x,y)
+
+
def natural_basis(self):
"""
Return a more-natural representation of this algebra's basis.
raise NotImplementedError('irregular element')
+ def inner_product(self, other):
+ """
+ Return the parent algebra's inner product of myself and ``other``.
+
+ EXAMPLES:
+
+ The inner product in the Jordan spin algebra is the usual
+ inner product on `R^n` (this example only works because the
+ basis for the Jordan algebra is the standard basis in `R^n`)::
+
+ sage: J = JordanSpinSimpleEJA(3)
+ sage: x = vector(QQ,[1,2,3])
+ sage: y = vector(QQ,[4,5,6])
+ sage: x.inner_product(y)
+ 32
+ sage: J(x).inner_product(J(y))
+ 32
+
+ The inner product on `S^n` is `<X,Y> = trace(X*Y)`, where
+ multiplication is the usual matrix multiplication in `S^n`,
+ so the inner product of the identity matrix with itself
+ should be the `n`::
+
+ sage: J = RealSymmetricSimpleEJA(3)
+ sage: J.one().inner_product(J.one())
+ 3
+
+ Likewise, the inner product on `C^n` is `<X,Y> =
+ Re(trace(X*Y))`, where we must necessarily take the real
+ part because the product of Hermitian matrices may not be
+ Hermitian::
+
+ sage: J = ComplexHermitianSimpleEJA(3)
+ sage: J.one().inner_product(J.one())
+ 3
+
+ TESTS:
+
+ Ensure that we can always compute an inner product, and that
+ it gives us back a real number::
+
+ sage: set_random_seed()
+ sage: J = random_eja()
+ sage: x = J.random_element()
+ sage: y = J.random_element()
+ sage: x.inner_product(y) in RR
+ True
+
+ """
+ P = self.parent()
+ if not other in P:
+ raise TypeError("'other' must live in the same algebra")
+
+ return P.inner_product(self, other)
+
+
def operator_commutes_with(self, other):
"""
Return whether or not this element operator-commutes
"""
if not other in self.parent():
- raise ArgumentError("'other' must live in the same algebra")
+ raise TypeError("'other' must live in the same algebra")
A = self.operator_matrix()
B = other.operator_matrix()
# TODO: we can do better once the call to is_invertible()
# doesn't crash on irregular elements.
#if not self.is_invertible():
- # raise ArgumentError('element is not invertible')
+ # raise ValueError('element is not invertible')
# We do this a little different than the usual recursive
# call to a finite-dimensional algebra element, because we
if other is None:
other=self
elif not other in self.parent():
- raise ArgumentError("'other' must live in the same algebra")
+ raise TypeError("'other' must live in the same algebra")
L = self.operator_matrix()
M = other.operator_matrix()
Return the trace inner product of myself and ``other``.
"""
if not other in self.parent():
- raise ArgumentError("'other' must live in the same algebra")
+ raise TypeError("'other' must live in the same algebra")
return (self*other).trace()
Qs = [ matrix(field, dimension, dimension, lambda k,j: 1*(k == j == i))
for i in xrange(dimension) ]
- return FiniteDimensionalEuclideanJordanAlgebra(field,Qs,rank=dimension)
+ return FiniteDimensionalEuclideanJordanAlgebra(field,
+ Qs,
+ rank=dimension,
+ inner_product=_usual_ip)
"""
n = M.nrows()
if M.ncols() != n:
- raise ArgumentError("the matrix 'M' must be square")
+ raise ValueError("the matrix 'M' must be square")
field = M.base_ring()
blocks = []
for z in M.list():
"""
n = ZZ(M.nrows())
if M.ncols() != n:
- raise ArgumentError("the matrix 'M' must be square")
+ raise ValueError("the matrix 'M' must be square")
if not n.mod(2).is_zero():
- raise ArgumentError("the matrix 'M' must be a complex embedding")
+ raise ValueError("the matrix 'M' must be a complex embedding")
F = QuadraticField(-1, 'i')
i = F.gen()
for j in xrange(n/2):
submat = M[2*k:2*k+2,2*j:2*j+2]
if submat[0,0] != submat[1,1]:
- raise ArgumentError('bad real submatrix')
+ raise ValueError('bad real submatrix')
if submat[0,1] != -submat[1,0]:
- raise ArgumentError('bad imag submatrix')
+ raise ValueError('bad imag submatrix')
z = submat[0,0] + submat[1,0]*i
elements.append(z)
return matrix(F, n/2, elements)
+# The usual inner product on R^n.
+def _usual_ip(x,y):
+ return x.vector().inner_product(y.vector())
+
+# The inner product used for the real symmetric simple EJA.
+# We keep it as a separate function because e.g. the complex
+# algebra uses the same inner product, except divided by 2.
+def _matrix_ip(X,Y):
+ X_mat = X.natural_representation()
+ Y_mat = Y.natural_representation()
+ return (X_mat*Y_mat).trace()
+
def RealSymmetricSimpleEJA(n, field=QQ):
"""
return FiniteDimensionalEuclideanJordanAlgebra(field,
Qs,
rank=n,
- natural_basis=T)
+ natural_basis=T,
+ inner_product=_matrix_ip)
def ComplexHermitianSimpleEJA(n, field=QQ):
"""
S = _complex_hermitian_basis(n)
(Qs, T) = _multiplication_table_from_matrix_basis(S)
+
+ # Since a+bi on the diagonal is represented as
+ #
+ # a + bi = [ a b ]
+ # [ -b a ],
+ #
+ # we'll double-count the "a" entries if we take the trace of
+ # the embedding.
+ ip = lambda X,Y: _matrix_ip(X,Y)/2
+
return FiniteDimensionalEuclideanJordanAlgebra(field,
Qs,
rank=n,
- natural_basis=T)
+ natural_basis=T,
+ inner_product=ip)
def QuaternionHermitianSimpleEJA(n):
In one dimension, this is the reals under multiplication::
- sage: J1 = JordanSpinSimpleEJA(1)
- sage: J2 = eja_rn(1)
- sage: J1 == J2
- True
+ sage: J1 = JordanSpinSimpleEJA(1)
+ sage: J2 = eja_rn(1)
+ sage: J1 == J2
+ True
"""
Qs = []
# The rank of the spin factor algebra is two, UNLESS we're in a
# one-dimensional ambient space (the rank is bounded by the
# ambient dimension).
- return FiniteDimensionalEuclideanJordanAlgebra(field, Qs, rank=min(n,2))
+ return FiniteDimensionalEuclideanJordanAlgebra(field,
+ Qs,
+ rank=min(n,2),
+ inner_product=_usual_ip)