← Back to 2.2.1.0a1.1

ex.24.7.2.44_93_114.e

Base Field
\(F = \) 2.2.1.0a1.1 \( = \mathbb{Q}_{ 2 }(a) = \mathbb{Q}_{ 2 }[x] / (x^{2} + x + 1 )\) View on LMFDB ↗
Description
exceptional, SL(2,3)
Construction
Extension to \(I_F\) of \( \tau = \operatorname{Ind}^{I_K}_{I_L} \chi \), with \(L, K\) and \(\chi\) as below
Semistability defect
\( e = 24\)
Conductor exponent
\( v(N) = 7\)
Character Order
4

Triply Field

The inertial type \(\tau\) becomes an induction (triply imprimitive) over: \( L = F(b) \), \(b\) a root of \(x^{3} + a\cdot 2 \)

Inducing Field

The inertial type \(\tau\) becomes reducible over \(K = L(c)\), \(c\) a root of \(x^{2} + ((a + 1)b^{3} )x + (b^{2} - 2a + 1)b \)

Underlying Character

Character \(\chi^A:\mathcal O_K^\times \to \mathbb C^\times\) with the following properties:

Order
4
Conductor exponent
11
Values on generators of \((\mathcal{O}_K/\mathfrak p^{ 11 })^\times/U_{\mathfrak{p}^{ 11 } }\) :
\(\begin{array}{l} \chi^A\left((4a - 3)c + 3a - 1 \right) &= i^{ 2 } \\ \chi^A\left(c + 1 \right) &= i^{ 2 } \\ \chi^A\left(2a\cdot b\cdot c + -2a - 3 \right) &= i^{ 2 } \\ \chi^A\left((b^{2} + (4a + 4))c + 1 \right) &= i^{ 1 } \\ \chi^A\left((a\cdot b^{2} + 4)c + 1 \right) &= i^{ 1 } \\ \chi^A\left(((2a + 3)b + (2a + 4))c + 2b + 4a + 1 \right) &= i^{ 0 } \\ \chi^A\left(((a + 2)b + (2a - 2))c + 2a\cdot b + 4a - 3 \right) &= i^{ 2 } \\ \chi^A\left(((2a + 2)b^{2} + (2a + 2)b + 2)c + (2a + 3)b^{2} + a\cdot b + a + 3 \right) &= i^{ 0 } \end{array} \)

Inertia Polynomial

The following polynomial defines a field \(L\) such that \(L^{un}\) is the fixed field of \(\tau\).
\( x^{24} + (4a + 4 )x^{21} + 4 x^{12} + 8a x^{9} + (4a + 4 )x^{6} + 2a \)
← Back to 2.2.1.0a1.1 Summary