DeRhamComputation/as_covers/as_form_class.sage
2024-12-20 12:12:21 +01:00

185 lines
6.5 KiB
Python

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