what can be supported in a general Jordan Algebra.
"""
-#from sage.algebras.finite_dimensional_algebras.finite_dimensional_algebra import FiniteDimensionalAlgebra
from sage.algebras.quatalg.quaternion_algebra import QuaternionAlgebra
-from sage.categories.finite_dimensional_algebras_with_basis import FiniteDimensionalAlgebrasWithBasis
+from sage.categories.magmatic_algebras import MagmaticAlgebras
from sage.combinat.free_module import CombinatorialFreeModule
from sage.matrix.constructor import matrix
from sage.misc.cachefunc import cached_method
from sage.misc.prandom import choice
+from sage.misc.table import table
from sage.modules.free_module import VectorSpace
from sage.rings.integer_ring import ZZ
from sage.rings.number_field.number_field import QuadraticField
from sage.rings.polynomial.polynomial_ring_constructor import PolynomialRing
from sage.rings.rational_field import QQ
from sage.structure.element import is_Matrix
-from sage.structure.category_object import normalize_names
from mjo.eja.eja_element import FiniteDimensionalEuclideanJordanAlgebraElement
from mjo.eja.eja_utils import _mat2vec
class FiniteDimensionalEuclideanJordanAlgebra(CombinatorialFreeModule):
+ # This is an ugly hack needed to prevent the category framework
+ # from implementing a coercion from our base ring (e.g. the
+ # rationals) into the algebra. First of all -- such a coercion is
+ # nonsense to begin with. But more importantly, it tries to do so
+ # in the category of rings, and since our algebras aren't
+ # associative they generally won't be rings.
+ _no_generic_basering_coercion = True
+
def __init__(self,
field,
mult_table,
"""
self._rank = rank
self._natural_basis = natural_basis
- self._multiplication_table = mult_table
+
if category is None:
- category = FiniteDimensionalAlgebrasWithBasis(field).Unital()
+ category = MagmaticAlgebras(field).FiniteDimensional()
+ category = category.WithBasis().Unital()
+
fda = super(FiniteDimensionalEuclideanJordanAlgebra, self)
fda.__init__(field,
range(len(mult_table)),
category=category)
self.print_options(bracket='')
+ # The multiplication table we're given is necessarily in terms
+ # of vectors, because we don't have an algebra yet for
+ # anything to be an element of. However, it's faster in the
+ # long run to have the multiplication table be in terms of
+ # algebra elements. We do this after calling the superclass
+ # constructor so that from_vector() knows what to do.
+ self._multiplication_table = [ map(lambda x: self.from_vector(x), ls)
+ for ls in mult_table ]
+
+
+ def _element_constructor_(self, elt):
+ """
+ Construct an element of this algebra from its natural
+ representation.
+
+ This gets called only after the parent element _call_ method
+ fails to find a coercion for the argument.
+
+ SETUP::
+
+ sage: from mjo.eja.eja_algebra import (JordanSpinEJA,
+ ....: RealCartesianProductEJA,
+ ....: RealSymmetricEJA)
+
+ EXAMPLES:
+
+ The identity in `S^n` is converted to the identity in the EJA::
+
+ sage: J = RealSymmetricEJA(3)
+ sage: I = matrix.identity(QQ,3)
+ sage: J(I) == J.one()
+ True
+
+ This skew-symmetric matrix can't be represented in the EJA::
+
+ sage: J = RealSymmetricEJA(3)
+ sage: A = matrix(QQ,3, lambda i,j: i-j)
+ sage: J(A)
+ Traceback (most recent call last):
+ ...
+ ArithmeticError: vector is not in free module
+
+ TESTS:
+
+ Ensure that we can convert any element of the two non-matrix
+ simple algebras (whose natural representations are their usual
+ vector representations) back and forth faithfully::
+
+ sage: set_random_seed()
+ sage: J = RealCartesianProductEJA(5)
+ sage: x = J.random_element()
+ sage: J(x.to_vector().column()) == x
+ True
+ sage: J = JordanSpinEJA(5)
+ sage: x = J.random_element()
+ sage: J(x.to_vector().column()) == x
+ True
+
+ """
+ if elt == 0:
+ # The superclass implementation of random_element()
+ # needs to be able to coerce "0" into the algebra.
+ return self.zero()
+
+ natural_basis = self.natural_basis()
+ if elt not in natural_basis[0].matrix_space():
+ raise ValueError("not a naturally-represented algebra element")
+
+ # Thanks for nothing! Matrix spaces aren't vector
+ # spaces in Sage, so we have to figure out its
+ # natural-basis coordinates ourselves.
+ V = VectorSpace(elt.base_ring(), elt.nrows()*elt.ncols())
+ W = V.span_of_basis( _mat2vec(s) for s in natural_basis )
+ coords = W.coordinate_vector(_mat2vec(elt))
+ return self.from_vector(coords)
+
def _repr_(self):
"""
Ensure that it says what we think it says::
sage: JordanSpinEJA(2, field=QQ)
- Euclidean Jordan algebra of degree 2 over Rational Field
+ Euclidean Jordan algebra of dimension 2 over Rational Field
sage: JordanSpinEJA(3, field=RDF)
- Euclidean Jordan algebra of degree 3 over Real Double Field
+ Euclidean Jordan algebra of dimension 3 over Real Double Field
"""
- # TODO: change this to say "dimension" and fix all the tests.
- fmt = "Euclidean Jordan algebra of degree {} over {}"
+ fmt = "Euclidean Jordan algebra of dimension {} over {}"
return fmt.format(self.dimension(), self.base_ring())
def product_on_basis(self, i, j):
- ei = self.basis()[i]
- ej = self.basis()[j]
- Lei = self._multiplication_table[i]
- return self.from_vector(Lei*ej.to_vector())
+ return self._multiplication_table[i][j]
def _a_regular_element(self):
"""
r = self.rank()
n = self.dimension()
- # Construct a new algebra over a multivariate polynomial ring...
+ # Turn my vector space into a module so that "vectors" can
+ # have multivatiate polynomial entries.
names = tuple('X' + str(i) for i in range(1,n+1))
R = PolynomialRing(self.base_ring(), names)
- J = FiniteDimensionalEuclideanJordanAlgebra(
- R,
- tuple(self._multiplication_table),
- r)
-
- idmat = matrix.identity(J.base_ring(), n)
+ V = self.vector_space().change_ring(R)
+
+ # Now let x = (X1,X2,...,Xn) be the vector whose entries are
+ # indeterminates...
+ x = V(names)
+
+ # And figure out the "left multiplication by x" matrix in
+ # that setting.
+ lmbx_cols = []
+ monomial_matrices = [ self.monomial(i).operator().matrix()
+ for i in range(n) ] # don't recompute these!
+ for k in range(n):
+ ek = self.monomial(k).to_vector()
+ lmbx_cols.append(
+ sum( x[i]*(monomial_matrices[i]*ek)
+ for i in range(n) ) )
+ Lx = matrix.column(R, lmbx_cols)
+
+ # Now we can compute powers of x "symbolically"
+ x_powers = [self.one().to_vector(), x]
+ for d in range(2, r+1):
+ x_powers.append( Lx*(x_powers[-1]) )
+
+ idmat = matrix.identity(R, n)
W = self._charpoly_basis_space()
W = W.change_ring(R.fraction_field())
# We want the middle equivalent thing in our matrix, but use
# the first equivalent thing instead so that we can pass in
# standard coordinates.
- x = J(W(R.gens()))
-
- # Handle the zeroth power separately, because computing
- # the unit element in J is mathematically suspect.
- x0 = W.coordinate_vector(self.one().to_vector())
- l1 = [ x0.column() ]
- l1 += [ W.coordinate_vector((x**k).to_vector()).column()
- for k in range(1,r) ]
- l2 = [idmat.column(k-1).column() for k in range(r+1, n+1)]
- A_of_x = matrix.block(R, 1, n, (l1 + l2))
- xr = W.coordinate_vector((x**r).to_vector())
- return (A_of_x, x, xr, A_of_x.det())
+ x_powers = [ W.coordinate_vector(xp) for xp in x_powers ]
+ l2 = [idmat.column(k-1) for k in range(r+1, n+1)]
+ A_of_x = matrix.column(R, n, (x_powers[:r] + l2))
+ return (A_of_x, x, x_powers[r], A_of_x.det())
@cached_method
return x.trace_inner_product(y)
+ def multiplication_table(self):
+ """
+ Return a visual representation of this algebra's multiplication
+ table (on basis elements).
+
+ SETUP::
+
+ sage: from mjo.eja.eja_algebra import JordanSpinEJA
+
+ EXAMPLES::
+
+ sage: J = JordanSpinEJA(4)
+ sage: J.multiplication_table()
+ +----++----+----+----+----+
+ | * || e0 | e1 | e2 | e3 |
+ +====++====+====+====+====+
+ | e0 || e0 | e1 | e2 | e3 |
+ +----++----+----+----+----+
+ | e1 || e1 | e0 | 0 | 0 |
+ +----++----+----+----+----+
+ | e2 || e2 | 0 | e0 | 0 |
+ +----++----+----+----+----+
+ | e3 || e3 | 0 | 0 | e0 |
+ +----++----+----+----+----+
+
+ """
+ M = list(self._multiplication_table) # copy
+ for i in range(len(M)):
+ # M had better be "square"
+ M[i] = [self.monomial(i)] + M[i]
+ M = [["*"] + list(self.gens())] + M
+ return table(M, header_row=True, header_column=True, frame=True)
+
+
def natural_basis(self):
"""
Return a more-natural representation of this algebra's basis.
sage: J.one()
e0 + e1 + e2 + e3 + e4
- TESTS::
+ TESTS:
The identity element acts like the identity::
"""
def __init__(self, n, field=QQ):
- # The superclass constructor takes a list of matrices, the ith
- # representing right multiplication by the ith basis element
- # in the vector space. So if e_1 = (1,0,0), then right
- # (Hadamard) multiplication of x by e_1 picks out the first
- # component of x; and likewise for the ith basis element e_i.
- Qs = [ matrix(field, n, n, lambda k,j: 1*(k == j == i))
- for i in xrange(n) ]
+ V = VectorSpace(field, n)
+ mult_table = [ [ V.gen(i)*(i == j) for j in range(n) ]
+ for i in range(n) ]
fdeja = super(RealCartesianProductEJA, self)
- return fdeja.__init__(field, Qs, rank=n)
+ return fdeja.__init__(field, mult_table, rank=n)
def inner_product(self, x, y):
return _usual_ip(x,y)
TESTS::
sage: random_eja()
- Euclidean Jordan algebra of degree...
+ Euclidean Jordan algebra of dimension...
"""
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. 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.
+ elements) for an algebra of those matrices.
"""
# In S^2, for example, we nominally have four coordinates even
# though the space is of dimension three only. The vector space V
V = VectorSpace(field, dimension**2)
W = V.span_of_basis( _mat2vec(s) for s in basis )
+ n = len(basis)
+ mult_table = [[W.zero() for j in range(n)] for i in range(n)]
+ for i in range(n):
+ for j in range(n):
+ mat_entry = (basis[i]*basis[j] + basis[j]*basis[i])/2
+ mult_table[i][j] = W.coordinate_vector(_mat2vec(mat_entry))
- Qs = []
- for s in basis:
- # Brute force the multiplication-by-s matrix by looping
- # through all elements of the basis and doing the computation
- # to find out what the corresponding row should be.
- Q_cols = []
- for t in basis:
- this_col = _mat2vec((s*t + t*s)/2)
- Q_cols.append(W.coordinates(this_col))
- Q = matrix.column(field, W.dimension(), Q_cols)
- Qs.append(Q)
-
- return Qs
+ return mult_table
def _embed_complex_matrix(M):
TESTS:
- The degree of this algebra is `(n^2 + n) / 2`::
+ The dimension of this algebra is `(n^2 + n) / 2`::
sage: set_random_seed()
sage: n = ZZ.random_element(1,5)
sage: J = RealSymmetricEJA(n)
- sage: J.degree() == (n^2 + n)/2
+ sage: J.dimension() == (n^2 + n)/2
True
The Jordan multiplication is what we think it is::
TESTS:
- The degree of this algebra is `n^2`::
+ The dimension of this algebra is `n^2`::
sage: set_random_seed()
sage: n = ZZ.random_element(1,5)
sage: J = ComplexHermitianEJA(n)
- sage: J.degree() == n^2
+ sage: J.dimension() == n^2
True
The Jordan multiplication is what we think it is::
TESTS:
- The degree of this algebra is `n^2`::
+ The dimension of this algebra is `n^2`::
sage: set_random_seed()
sage: n = ZZ.random_element(1,5)
sage: J = QuaternionHermitianEJA(n)
- sage: J.degree() == 2*(n^2) - n
+ sage: J.dimension() == 2*(n^2) - n
True
The Jordan multiplication is what we think it is::
"""
def __init__(self, n, field=QQ):
- Qs = []
- id_matrix = matrix.identity(field, n)
- for i in xrange(n):
- ei = id_matrix.column(i)
- Qi = matrix.zero(field, n)
- Qi.set_row(0, ei)
- Qi.set_column(0, ei)
- Qi += matrix.diagonal(n, [ei[0]]*n)
- # The addition of the diagonal matrix adds an extra ei[0] in the
- # upper-left corner of the matrix.
- Qi[0,0] = Qi[0,0] * ~field(2)
- Qs.append(Qi)
+ V = VectorSpace(field, n)
+ mult_table = [[V.zero() for j in range(n)] for i in range(n)]
+ for i in range(n):
+ for j in range(n):
+ x = V.gen(i)
+ y = V.gen(j)
+ x0 = x[0]
+ xbar = x[1:]
+ y0 = y[0]
+ ybar = y[1:]
+ # z = x*y
+ z0 = x.inner_product(y)
+ zbar = y0*xbar + x0*ybar
+ z = V([z0] + zbar.list())
+ mult_table[i][j] = z
# The rank of the spin algebra is two, unless we're in a
# one-dimensional ambient space (because the rank is bounded by
# the ambient dimension).
fdeja = super(JordanSpinEJA, self)
- return fdeja.__init__(field, Qs, rank=min(n,2))
+ return fdeja.__init__(field, mult_table, rank=min(n,2))
def inner_product(self, x, y):
return _usual_ip(x,y)