##### # # This file is ~steger/donald/SU21/C18p3/D.txt # ##### CASE: $(C_{18},p=3)$ The BASE FIELDS: k = \QQ[\sqrt{6}] \ell = k[\zeta_3] = k[\sqrt{-3}] = \QQ[\sqrt{6},\sqrt{-3}] = \QQ[\sqrt{-2},\sqrt{-3}] $k$~ramifies over~$\QQ$ only at the $2$-adic and $3$-adic places. $\ell$ doesn't ramify over~$k$ at any places. The EXTENSION FIELD used to present the division algebra: m = \QQ[\sqrt{6},\zeta_9] = \QQ[\sqrt{-2},\zeta_9] = k[\zeta_9] = k[Z]/(Z^6+Z^3+1) Here~$Z=\zeta_9$ is a primitive $9$'th root of unity. $m$~is a cylic Galois extension of degree~$6$ over~$k$ with Galois group \{ Z\mapsto Z, \mapsto Z^2, \mapsto Z^4, \mapsto Z^8, \mapsto Z^7, \mapsto Z^5 \} $m$~is also an extension of $\ell$, where we take: \sqrt{-3} = 1 + 2\zeta_3 = 1 + 2Z^3 The Galois group of~$m$ over~$\ell$ is generated by~$\phi$: \phi(Z) = Z^4 = \zeta_3 Z \phi(Z^j) = Z^{4j} = \zeta_3^j Z^j \phi^2(Z) = Z^{16} = \zeta_3^2 Z \phi^2(Z^j) = Z^{16j} = \zeta_3^{2j} Z^j Specifically, it's \{ Z\mapsto Z, \mapsto Z^4, \mapsto Z^{16} \} which is the unique subgroup of order~$3$ of the Galois group of $m$~over~$\ell$. The intersection of~$m$ with the reals is generated by~$\sqrt{6}$ and W = Z + Z^{-1} whose irreducible polynomial over~$\QQ$ (or over~$\ell$) is W^3 - 3W + 1 The discriminant of $W^3-3W+1$ is~$81$. \phi(W) = -W^2-W+2 \phi(W^2) = W+2 \phi^2(W) = W^2-2 \phi^2(W^2) = -W^2-W+4 Over~$\QQ$, $m$~ramifies at the $3$-adic place with ramification index $e=6$; at the $2$-adic place it ramifies with ramification index~$e=2$ Over~$k$, $m$~ramifies only at the $3$-adic place with ramification index $e=3$. Over~$\ell$, $m$ ramifies only at the $3$-adic places with ramification index $e=3$. The ramification at the $3$-adic place is \emph{wild} ramification. PRESENTATION of $\D$, degree three division algebra, central over~$\ell$: $\D$ is generated by~$m$ and~$\sigma$ where for $x\in m$ \sigma x \sigma^{-1} = \phi(x) \sigma^3 = (\sqrt{-3} + \sqrt{6}) / 3 = 1/3 + 2 Z^3/3 + \sqrt{6}/3 Then (1') $\D\otimes\ell_{3\pm}$ has Hasse invariant $\pm 1$; (2') $\D\otimes\ell_v$ splits at every other place~$v$. For any place~$v$ which is not $3$-adic, we know $\D\otimes\ell_v$ splits because $(\sqrt{-3}+\sqrt{6})/3$ has valuation zero at~$v$ and because $m$~doesn't ramify over~$\ell$ at~$v$. For the two $3$-adic place~$3\pm$ of~$\ell$, the calculations showing that~$\D$ does not split are more complicated. See Appendix~A. EMBEDDING of $\D$ in $\Mat_{3\time 3}(\CC)$: x 0 0 x \mapsto 0 \phi(x) 0 (for $x\in m$) 0 0 \phi^2(x) 0 1 0 \sigma \mapsto 0 0 1 (\sqrt{-3}+\sqrt{6})/3 0 0 For COMPLEX calculation: Z = 0.7660444431189780352023927 + 0.6427876096865393263226434 i W = Z + Z^{-1} = 1.5320888862379560704047853 (\sqrt{-3}+\sqrt(6))/3 = 0.8164965809277260327324280 + 0.5773502691896257645091488 i PRELIMINARY INVOLUTION of the second kind: \bar Z = Z^{-1} \bar W = W \overline{\sqrt{-3}} = -\sqrt{-3} \iota_0(x) = \bar x (for $x\in m$) \iota_0(\sigma) = \sigma^{-1} On complex matrices: \iota_0(A) = A^* INVOLUTION of the second kind: Because $\iota_0$ gives the compact group $PU(3)\times PU(3)$ at the real place, we need to adjust it. We use T = (3-3\sqrt{6}) + \sqrt{6} W + \sqrt{6} W^2 = 3 + \sqrt{6} (-1-\zeta_9^4-\zeta_9^5) \phi(T) = (3+\sqrt{6}) - \sqrt{6} W^2 = 3 + \sqrt{6} (-1+\zeta_9-\zeta_9^2+\zeta_9^4) === ERROR CORRECTED HERE ===> \phi^2(T) = (3-\sqrt{6}) - \sqrt{6} W = 3 + \sqrt{6} (-1-\zeta_9+\zeta_9^2+\zeta_9^5) The adjusted involution is: \iota(x) = T^-1 \iota_0(x) T \iota(x) = \bar x (for $x\in m$) \iota(\sigma) = T^{-1} \sigma^{-1} T = \phi^2(T)/T \sigma^{-1} = (-1 + 4W - \sqrt{6} W^2) \sigma^{-1} = ((-1-2\sqrt{6})+(4+\sqrt{6})Z+(-4-\Sqrt{6})Z^2 +\sqrt{6}Z^4-4Z^5) \sigma^-1 \iota(\sigma^{-1}) = T^-1 \sigma T = \phi(T)/T \sigma = (-1 -\sqrt{6}W + 2W^2) \sigma = (3+(-2-\sqrt{6})Z+(2+\sqrt{6})Z^2-2Z^4 +\sqrt{6}Z^5) \sigma On complex matrices: \iota(A) = F^{-1} A^* F for T 0 0 F = 0 \phi(T) 0 0 0 \phi^2(T) which means unitary matrices ought to preserve the form: T |v_1|^2 + \phi(T) |v_2|^2 + \phi^2(T) |v_3|^2 INTEGRALITY: We want elements of the form \sum_{i=0,1} \sum_{j=0,1,2,3,4,5} \sum_{l=-1,0,1} c_{ijl} \sqrt{-2}^i Z^j \sigma^l where the coefficients c_{ijl}\in\QQ satisfy integrality conditions as follows: (.) For any prime~$v$ except 2 or~3 the $c_{ijl}$ are integral in $\QQ_v$, i.e. no factors of~$v$ occur in the denominators. (.) Factors of~3 may appear in the denominators. However, the power of~3 which appears is bounded above. Almost certainly all such powers disappear if one multiplies the~$c_{ijl}$ by~729. (.) At the special prime~2 there are two possible conditions. The Type~1 (or hyperspecial) condition is simple: the $c_{ijl}$ mustn't have any factors of two in their denominators. For the Type~2 (or non-hyperspecial) condition one must use special conditions, as calculated in ~/donald/SU21/C18p3/padic.gap. The Type~1 condition amounts to requiring that an element of~$U(\D,\iota)$ fix a certain lattice in~$\ell_2^3$ which is self-dual relative to the sesquilinear form associated to~$\iota$. The Type~2 condition amounts to requiring that an element of~$U(\D,\iota)$ fix a certain pair of mutually dual lattices in~$\ell_2^3$, a pair which is also adjacent in the building of~$PGL(3,\ell_2)$. The Type~1 condition is the condition that the element of~$U(\D,\iota)$ fix a certain hyperspecial vertex of the tree, or in other words that its image in $\GG(\QQ_2)$ belong to a certain hyperspecial parahoric subgroup. Contrariwise, the Type~2 condition is the condition that the element fix a certain non-hyperspecial vertex on the tree; the condition that its image in $\GG(\QQ_2)$ belong to a certain non-hyperspecial parahoric. DETERMINANTS: Elements of $U(\D,\iota)$ can have determinant which is $1$, $\zeta_3$, or $\zeta_3^2$ multiplied by any power of~$(\sqrt{-3}+\sqrt{6})/3$. In~$PU$, one can always choose a representative where the power is~$0$ or~$\pm 1$. APPENDIX A: NON-SPLITTING OF $\D$ AT THE 3-ADIC PLACES We can write: \ell = \QQ[\sqrt{-2},\zeta_3] m = \QQ[\sqrt{-2},\zeta_9] As we do this, let us fix signs as follows and identify: \sqrt{-3} = 2\zeta_3+1 \sqrt{6} = -\sqrt{-3}\sqrt{-2} For k'=\QQ[\sqrt{-2}]=\QQ[S']/(S'^2+2) there are two $3$-adic places, $3+$ and~$3-$. Both $k'_{3+}$ and $k'_{3-}$ are copies of $\QQ_3$, and we can characterize the two places, respectively, by the conditions $S'=4 \mod~9$ and $S'=5 \mod~9$. For~$\ell$ there are likewise two $3$-adic places, still called $3+$ and~$3-$. $\ell_{3+}$ (respectively~$\ell_{3-}$) is a copy of $\QQ_3[\zeta_3]$, ramified of degree~$2$ over~$\QQ_3$. For~$m$ there are again two $3$-adic places, still called $3+$ and~$3-$. $m_{3+}$ (respectively~$m_{3-}$) is a copy of $\QQ_3[\zeta_9]$, ramified of degree~6 over $\QQ_3$ and of degree~3 over $\ell_{3+}$ (respectively $\ell_{3-}$). Let~$v=3+$ or~$3-$. Which elements of~$\ell_v$ are norms from~$m_v$? That is, what is $N_{m_v/\ell_v) (m_v)$? From general theory we know that [\ell_v^\times : N_{m_v/\ell_v) (m_v^\times)] = [m_v : \ell_v] = 3 One element of minimal positive valuation in~$\ell_v$ is~$\pi=1-\zeta_3$, which satisfies $\pi^2-3\pi+3=0$. Here are some particular norms: N_{m_v/\ell_v}(1-\zeta_9) = (1 - \zeta_9) (1 - \zeta_9\zeta_3) (1 - \zeta_9\zeta_3^2) = 1 - \zeta_9^3 = 1 -\zeta_3 = \pi N_{m_v/\ell_v}(-1) = (-1)^3 = -1 N_{m_v/\ell_v}(\zeta_9) = \zeta_9 \zeta_9\zeta_3 \zeta_9\zeta_3^2 = \zeta_9^3 = \zeta_3 = 1 - \pi N_{m_v/\ell_v} (1-\zeta_9\pi}) = (1-\zeta_9\pi) (1-\zeta_9\zeta_3\pi) (1-\zeta_9\zeta_3^2\pi) = 1-(\zeta_9\pi)^3 = 1-\zeta_3\pi^3 = 1-\pi^3 \mod 9 With the first three of these one sees that any element in $\ell_v^\times$ can be multiplied by norms to obtain first an element of valuation zero, next an element $=1 \mod \pi$, and finally an element $=1\mod 3$. If the final element is $=1 \mod 3\pi$ then it is a norm in~$\ell_v$. Indeed, using $N_{m_v/\ell_v} (1-\zeta_9\pi)$ one can further reduce it to an element $=1\mod 9$. The reduced element is now a cube in~$\ell_v$ --- use (1+3)^3 = 1+9 \mod 27 (1+3\pi)^3 = 1+9\pi \mod 81 (1+9)^3 = 1+27 \mod 243 (1+9\pi)^3 = 1+27\pi \mod 729 \dots Not all elements are norms, which implies that while elements $=1 \mod 3\pi$ are norms, elements $=4$ or $=7 \mod 3\pi$ are not. The element of interest is $\sigma^3 = (\sqrt{-3}+\sqrt{6})/3$. Multiply first by the norm $\pi=1-\zeta_3=(3-\sqrt{-3})/2$ to get \sigma^3 \pi = (\sqrt{-3}+\sqrt{6})/3 (3-\sqrt{-3}) / 2 = (1-\sqrt{-2}) \sqrt{-3} (3-\sqrt{-3} / 6 = (1-\sqrt{-2}) (1+\sqrt{-3}) / 2 = (1-\sqrt{-2}) (2-\pi) Let us analyse this for~$v=3-$ where $\sqrt{-2}=5 \mod 9$, whence \sigma^3 \pi = (1-5) (2-\pi) = 1+4\pi \mod 9 = 1+\pi \mod 3\pi Multiplying this by the norm $1-\pi$ we get \sigma^3 \pi (1-\pi) = 1-\pi^2 = 1-(1-\zeta_3)^2 = 1-(1-2\zeta_3+\zeta_3^2) = 1+3\zeta_3 = 1+3(1-\pi) = 4 \mod 3\pi According to the previous analysis $4 \mod 3\pi$ is not in fact a norm from~$m_v$ to~$\ell_v$. A similar analysis for $v=3+$ is doable, but it can be avoided. Indeed, the only difference in passing from~$3-$ to~$3+$ is a change in sign for $\sqrt{-2}$, which is equivalent to replacing~$\sigma^3$ with its inverse. Consequently, for~$v=3+$, $\sigma^3$ will be in the same $N_{m_v/\ell_v} m_v^\times$ coset as $1/4 = 7 \mod 9$.