Examples#
- Example: example1 (ex-e326da)#
We consider a newform of weight \(5\) and level \(7\), whose local representation at \(7\) is principal series.
> S := CuspidalSubspace(ModularSymbols(Gamma1(7), 5, 1)); > newforms := NewformDecomposition(S); > Eigenform(newforms[1], 15); q + q^2 - 15*q^4 + 49*q^7 - 31*q^8 + 81*q^9 - 206*q^11 + 49*q^14 + O(q^15) > pi := LocalComponent(newforms[1], 7); > pi; Ramified Principal Series Representation of GL(2,Q_7) > chi := CentralCharacter(pi); > Conductor(chi); 7 > parameters := PrincipalSeriesParameters(pi);
These are Dirichlet characters on \({\mathbb{Z}}/7{\mathbb{Z}}\) (the trivial character and the character of order \(2\)):
> Conductor(parameters[1]), Order(parameters[1]); 1 1 > Conductor(parameters[2]), Order(parameters[2]); 7 2
The principal series representation \(\pi\) is the induction up to \({\operatorname{GL}}_2({\mathbb{Q}}_7)\) of a character of the Borel subgroup inflated from a character of the diagonal group \({\mathbb{Q}}_7^{\times} \times {\mathbb{Q}}_7^{\times}.\) The restriction of this character to \({\mathbb{Z}}_7^{\times} \times {\mathbb{Z}}_7^{\times}\) gives the pair of Dirichlet characters above. We now compute the Galois representation.
> rho := WeilRepresentation(pi); rho; 2-dim Galois representation (2,0) with G=C2, I=C2, conductor 7^1 over Q7[40] > IsAbelian(Group(rho)); true
The Weil representation is simply the sum of the two characters above (up to unramified twists), considered as characters of the Galois group of \({\mathbb{Q}}_7\) via local class field theory.
> Decomposition(rho); [ 1-dim trivial Galois representation 1 over Q7[40], 1-dim Galois representation (1,-1) with G=C2, I=C2, conductor 7^1 over Q7[40] ]
- Example: example2 (ex-298b2e)#
We consider a supercuspidal representation of conductor \(121\), associated to a newform of weight \(2\) and level \(121.\)
> S := CuspidalSubspace(ModularSymbols(Gamma0(121), 2, 1)); > newforms := NewformDecomposition(S); > newforms; [ Modular symbols space for Gamma_0(121) of weight 2 and dimension 1 over Rational Field, Modular symbols space for Gamma_0(121) of weight 2 and dimension 1 over Rational Field, Modular symbols space for Gamma_0(121) of weight 2 and dimension 1 over Rational Field, Modular symbols space for Gamma_0(121) of weight 2 and dimension 1 over Rational Field, Modular symbols space for Gamma_0(121) of weight 2 and dimension 2 over Rational Field ] > Eigenform(newforms[2], 11); q + q^2 + 2*q^3 - q^4 + q^5 + 2*q^6 - 2*q^7 - 3*q^8 + q^9 + q^10 + O(q^11) > pi := LocalComponent(newforms[2], 11); > pi; Supercuspidal Representation of GL(2,Q_11)
This means the representation of the Weil group associated to pi is irreducible.
> Conductor(pi); 121 > W := CuspidalInducingDatum(pi); > W; GModule W of dimension 10 over Rational Field
\(W\) is a module over a group which is a quotient of \({\operatorname{GL}}_2({\mathbb{Z}}_{11}),\) namely \({\operatorname{GL}}_2({\mathbb{Z}}/{11{\mathbb{Z}}}).\) The representation \(\pi\) is induced from some extension of \(W\) to the open subgroup \({\mathbb{Q}}_{11}^{\times}{\operatorname{GL}}_2({\mathbb{Z}}_{11}).\)
> Group(W); MatrixGroup(2, IntegerRing(11)) of order 2^4 * 3 * 5^2 * 11 Generators: [2 0] [0 1] [1 1] [0 1] [ 0 1] [10 0] > Group(W) eq GL(2, Integers(11)); true > rho:=WeilRepresentation(pi);
This gives the full Weil representation attached to \(\pi\). The leading factor
Unr(-I)is the unramified twist by \(-1\) from the Loeffler-Weinstein rectifier, which fixes the action of Frobenius.> rho; 2-dim Galois representation Unr(-I)*(2,0,-1) with G=S3, I=C3, conductor 11^2 over Q11[10]
Since the Frobenius action is now determined, the local root number is available.
> RootNumber(rho); -1
- Example: example3 (ex-3e3aa7)#
We consider a supercuspidal representation of conductor \(3^3\), associated to a newform of weight \(4\) and level \(27\).
> S := CuspidalSubspace(ModularSymbols(Gamma0(27), 4, 1)); > newforms := NewformDecomposition(S); > Eigenform(newforms[1], 13); q + 3*q^2 + q^4 + 15*q^5 - 25*q^7 - 21*q^8 + 45*q^10 - 15*q^11 + O(q^13) > pi:=LocalComponent(newforms[1], 3); > pi; Supercuspidal Representation of GL(2,Q_3) > W:=CuspidalInducingDatum(pi); > W; GModule W of dimension 2 over Rational Field > Group(W); MatrixGroup(2, IntegerRing(9)) of order 2^2 * 3^5 Generators: [1 1] [0 1] [2 0] [0 1] [1 0] [0 2] [1 0] [3 1]
These matrices generate (topologically) the Iwahori subgroup of \({\operatorname{GL}}_2({\mathbb{Z}}_3)\) consisting of matrices which are upper-triangular modulo \(3\). \(W\) is an irreducible two-dimensional \(G\)-module. The representation \(\pi\) is induced from some extension of \(W\) to the normalizer of the Iwahori in \({\operatorname{GL}}_2({\mathbb{Q}}_3)\).
> E, chi:=AdmissiblePair(pi); > E; Totally ramified extension defined by the polynomial x^2 - 3 over 3-adic ring mod 3^10 > E.1^2; 3 > chi(1+E.1); -zeta_3 - 1
Note that
chican only be evaluated on units of \(E\), so thatchi(E.1)would result in an error.> WeilRepresentation(pi); 2-dim Galois representation Unr(-1/3*sqrt(3)*i)*(2,0,-1) with G=S3, I=S3, conductor 3^3 over Q3[10]