class heisenberg_function: def __init__(self, C, g): self.curve = C F = C.base_ring n = C.height variable_names = 'x, y' for i in range(n): variable_names += ', z' + str(i) Rxyz = PolynomialRing(F, n+2, variable_names) x, y = Rxyz.gens()[:2] z = Rxyz.gens()[2:] RxyzQ = FractionField(Rxyz) self.function = RxyzQ(g) #self.function = heisenberg_reduction(AS, RxyzQ(g)) def __repr__(self): return str(self.function) def __eq__(self, other): AS = self.curve RxyzQ, Rxyz, x, y, z = AS.fct_field aux = self - other aux = RxyzQ(aux.function) aux = aux.numerator() aux = heisenberg_function(AS, aux) aux = aux.expansion_at_infty() if aux.valuation() >= 1: return True return False def __add__(self, other): C = self.curve g1 = self.function g2 = other.function return heisenberg_function(C, g1 + g2) def __sub__(self, other): C = self.curve g1 = self.function g2 = other.function return heisenberg_function(C, g1 - g2) def __rmul__(self, constant): C = self.curve g = self.function return heisenberg_function(C, constant*g) def __neg__(self): C = self.curve g = self.function return heisenberg_function(C, -g) def __mul__(self, other): if isinstance(other, heisenberg_function): C = self.curve g1 = self.function g2 = other.function return heisenberg_function(C, g1*g2) if isinstance(other, heisenberg_form): C = self.curve g1 = self.function g2 = other.form return heisenberg_form(C, g1*g2) def __truediv__(self, other): C = self.curve g1 = self.function g2 = other.function return heisenberg_function(C, g1/g2) def __pow__(self, exponent): C = self.curve g1 = self.function return heisenberg_function(C, g1^(exponent)) 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] n = C.height variable_names = 'x, y' for j in range(n): variable_names += ', z' + str(j) Rxyz = PolynomialRing(F, n+2, variable_names) x, y = Rxyz.gens()[:2] z = Rxyz.gens()[2:] RxyzQ = FractionField(Rxyz) prec = C.prec Rt. = LaurentSeriesRing(F, default_prec=prec) g = self.function g = RxyzQ(g) sub_list = {x : x_series, y : y_series} | {z[j] : z_series[j] for j in range(n)} return g.substitute(sub_list) def expansion(self, pt = 0): C = self.curve delta = C.nb_of_pts_at_infty F = C.base_ring x_series = C.x_series[pt] y_series = C.y_series[pt] z_series = C.z_series[pt] n = C.height variable_names = 'x, y' for j in range(n): variable_names += ', z' + str(j) Rxyz = PolynomialRing(F, n+2, variable_names) x, y = Rxyz.gens()[:2] z = Rxyz.gens()[2:] RxyzQ = FractionField(Rxyz) prec = C.prec Rt. = LaurentSeriesRing(F, default_prec=prec) g = self.function g = RxyzQ(g) sub_list = {x : x_series, y : y_series} | {z[j] : z_series[j] for j in range(n)} return g.substitute(sub_list) def group_action(self, elt): AS = self.curve RxyzQ, Rxyz, x, y, z = AS.fct_field if elt == (0, 0, 0): return self if elt == (1, 0, 0): sub_list = {x : x, y : y} | {z[0] : z[0] + 1, z[1] : z[1], z[2]: z[2] + z[1]} g = self.function return heisenberg_function(AS, g.substitute(sub_list)) if elt == (0, 1, 0): sub_list = {x : x, y : y} | {z[0] : z[0] + 1, z[1] : z[1] + 1, z[2]: z[2]} g = self.function return heisenberg_function(AS, g.substitute(sub_list)) if elt == (0, 0, 1): sub_list = {x : x, y : y} | {z[0] : z[0], z[1] : z[1], z[2]: z[2] - 1} g = self.function return heisenberg_function(AS, g.substitute(sub_list)) if elt[0] > 0: elt1 = (elt[0] - 1, elt[1], elt[2]) return self.group_action(elt1).group_action((1, 0, 0)) if elt[1] > 0: elt1 = (elt[0], elt[1] - 1, elt[2]) return self.group_action(elt1).group_action((0, 1, 0)) if elt[2] > 0: elt1 = (elt[0], elt[1], elt[2] - 1) return self.group_action(elt1).group_action((0, 0, 1)) def trace(self): print('trace ') C = self.curve C_super = C.quotient n = C.height F = C.base_ring variable_names = 'x, y' for j in range(n): variable_names += ', z' + str(j) Rxyz = PolynomialRing(F, n+2, variable_names) x, y = Rxyz.gens()[:2] z = Rxyz.gens()[2:] RxyzQ = FractionField(Rxyz) result = heisenberg_function(C, 0) G = C.group for a in G: result += self.group_action(a) result = result.function Rxy. = PolynomialRing(F, 2) Qxy = FractionField(Rxy) result = heisenberg_reduction(C, result) #print(result) return superelliptic_function(C_super, Qxy(result)) def coordinates(self, prec = 100, basis = 0): "Return coordinates in H^1(X, OX)." AS = self.curve if basis == 0: basis = [AS.holomorphic_differentials_basis(), AS.cohomology_of_structure_sheaf_basis()] holo_diffs = basis[0] coh_basis = basis[1] f_products = [] for f in coh_basis: f_products += [[omega.serre_duality_pairing(f) for omega in holo_diffs]] product_of_fct_and_omegas = [] product_of_fct_and_omegas = [omega.serre_duality_pairing(self) for omega in holo_diffs] V = (F^(AS.genus())).span_of_basis([vector(a) for a in f_products]) coh_coordinates = V.coordinates(product_of_fct_and_omegas) return coh_coordinates def diffn(self): C = self.curve C_super = C.quotient n = C.height RxyzQ, Rxyz, x, y, z = C.fct_field fcts = C.functions f = self.function y_super = superelliptic_function(C_super, y) dy_super = y_super.diffn().form dz = [] for i in range(n): dfct = fcts[i].diffn().form dz += [-dfct] result = f.derivative(x) result += f.derivative(y)*dy_super for i in range(n): result += f.derivative(z[i])*dz[i] return heisenberg_form(C, result) def valuation(self, place = 0): '''Return valuation at i-th place at infinity.''' C = self.curve F = C.base_ring Rt. = LaurentSeriesRing(F) return Rt(self.expansion_at_infty(place = place)).valuation()