185 lines
6.5 KiB
Python
185 lines
6.5 KiB
Python
class as_form:
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def __init__(self, C, g):
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self.curve = C
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n = C.height
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F = C.base_ring
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RxyzQ, Rxyz, x, y, z = C.fct_field
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self.form = RxyzQ(g)
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def __repr__(self):
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return "(" + str(self.form)+") * dx"
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def __eq__(self, other):
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return self.expansion_at_infty() == other.expansion_at_infty()
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def expansion_at_infty(self, place = 0):
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C = self.curve
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delta = C.nb_of_pts_at_infty
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F = C.base_ring
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x_series = C.x_series[place]
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y_series = C.y_series[place]
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z_series = C.z_series[place]
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dx_series = C.dx_series[place]
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n = C.height
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RxyzQ, Rxyz, x, y, z = C.fct_field
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prec = C.prec
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Rt.<t> = LaurentSeriesRing(F, default_prec=prec)
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g = self.form
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sub_list = {x : x_series, y : y_series} | {z[j] : z_series[j] for j in range(n)}
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return g.substitute(sub_list)*dx_series
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def expansion(self, pt = 0):
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'''Same code as expansion_at_infty.'''
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C = self.curve
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F = C.base_ring
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x_series = C.x_series[pt]
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y_series = C.y_series[pt]
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z_series = C.z_series[pt]
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dx_series = C.dx_series[pt]
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n = C.height
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RxyzQ, Rxyz, x, y, z = C.fct_field
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prec = C.prec
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Rt.<t> = LaurentSeriesRing(F, default_prec=prec)
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g = self.form
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sub_list = {x : x_series, y : y_series} | {z[j] : z_series[j] for j in range(n)}
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return g.substitute(sub_list)*dx_series
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def __add__(self, other):
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C = self.curve
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g1 = self.form
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g2 = other.form
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return as_form(C, g1 + g2)
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def __sub__(self, other):
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C = self.curve
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g1 = self.form
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g2 = other.form
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return as_form(C, g1 - g2)
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def __neg__(self):
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C = self.curve
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g = self.form
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return as_form(C, -g)
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def __rmul__(self, constant):
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C = self.curve
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omega = self.form
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return as_form(C, constant*omega)
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def reduce(self):
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RxyzQ, Rxyz, x, y, z = self.curve.fct_field
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m = self.curve.quotient.exponent
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aux = as_reduction(self.curve, RxyzQ(y^m*self.form))
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return as_form(self.curve, aux/y^m)
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def group_action(self, elt):
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C = self.curve
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n = C.height
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aux = as_function(C, self.form)
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aux = aux.group_action(elt)
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return as_form(C, aux.function)
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def coordinates(self, basis = 0):
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"""Find coordinates of the given holomorphic form self in terms of the basis forms in a list holo."""
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self = self.reduce()
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print(self)
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C = self.curve
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if basis == 0:
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basis = C.holomorphic_differentials_basis()
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RxyzQ, Rxyz, x, y, z = C.fct_field
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# We need to have only polynomials to use monomial_coefficients in linear_representation_polynomials,
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# and sometimes basis elements have denominators. Thus we multiply by them.
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denom = LCM([denominator(omega.form) for omega in basis])
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basis = [denom*omega for omega in basis]
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self_with_no_denominator = denom*self
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print(denom, basis, self_with_no_denominator)
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return linear_representation_polynomials(Rxyz(self_with_no_denominator.form), [Rxyz(omega.form) for omega in basis])
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def trace(self, super=True):
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C = self.curve
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C_super = C.quotient
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n = C.height
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F = C.base_ring
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RxyzQ, Rxyz, x, y, z = C.fct_field
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result = as_form(C, 0)
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G = C.group.elts
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for a in G:
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result += self.group_action(a)
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result = result.form
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Rxy.<x, y> = PolynomialRing(F, 2)
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Qxy = FractionField(Rxy)
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result = as_reduction(C, result)
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if super:
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return superelliptic_form(C_super, Qxy(result))
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return as_form(C, Qxy(result))
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def residue(self, place=0):
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return self.expansion_at_infty(place = place).residue()
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def valuation(self, place=0):
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return self.expansion_at_infty(place = place).valuation()
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def serre_duality_pairing(self, fct):
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AS = self.curve
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return sum((fct*self).residue(place = _) for _ in range(AS.nb_of_pts_at_infty))
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def cartier(self):
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C = self.curve
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F = C.base_ring
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n = C.height
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ff = C.functions
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p = F.characteristic()
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C_super = C.quotient
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(RxyzQ, Rxyz, x, y, z) = C.fct_field
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fct = self.form
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Rxy.<x, y> = PolynomialRing(F, 2)
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RxyQ = FractionField(Rxy)
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x, y = Rxyz.gens()[0], Rxyz.gens()[1]
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z = Rxyz.gens()[2:]
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num = Rxyz(fct.numerator())
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den = Rxyz(fct.denominator())
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result = RxyzQ(0)
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#return (num, den, z, fct)
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if den in Rxy:
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sub_list = {x : x, y : y} | {z[j] : (z[j]^p - RxyzQ(ff[j].function)) for j in range(n)}
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num = RxyzQ(num.substitute(sub_list))
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den1 = Rxyz(num.denominator())
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num = Rxyz(num*den1^p)
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for monomial in Rxyz(num).monomials():
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degrees = [monomial.degree(z[i]) for i in range(n)]
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product_of_z = prod(z[i]^(degrees[i]) for i in range(n))
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monomial_divided_by_z = monomial/product_of_z
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product_of_z_no_p = prod(z[i]^(degrees[i]/p) for i in range(n))
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aux_form = superelliptic_form(C_super, RxyQ(monomial_divided_by_z/den))
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aux_form = aux_form.cartier()
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result += product_of_z_no_p * Rxyz(num).monomial_coefficient(monomial) * aux_form.form/den1
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return as_form(C, result)
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raise ValueError("Please present first your form as sum z^i omega_i, where omega_i are forms on quotient curve.")
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def is_regular_on_U0(self):
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AS = self.curve
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C = AS.quotient
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m = C.exponent
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RxyzQ, Rxyz, x, y, z = AS.fct_field
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if y^(m-1)*self.form in Rxyz:
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return True
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return False
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def are_forms_linearly_dependent(set_of_forms):
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from sage.rings.polynomial.toy_variety import is_linearly_dependent
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C = set_of_forms[0].curve
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F = C.base_ring
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n = C.height
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RxyzQ, Rxyz, x, y, z = C.fct_field
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denominators = prod(denominator(omega.form) for omega in set_of_forms)
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return is_linearly_dependent([Rxyz(denominators*omega.form) for omega in set_of_forms])
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def only_log_forms(C_AS):
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list1 = AS.at_most_poles_forms(0)
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list2 = AS.at_most_poles_forms(1)
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result = []
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for a in list2:
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if not(are_forms_linearly_dependent(list1 + result + [a])):
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result += [a]
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return result
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