Equality of SIC-generated fields with ray class fields
Prove that for any admissible tuple \(t=(d,r,Q)\), letting \(E = H^{\mathcal{O}_f}_{\bar{d}\,\infty_1\,\infty_2}\) be the ray class field of the order \(\mathcal{O}_f\) with modulus \(\bar{d}\) and both real places ramified, the SIC-generated field \(E_t\) satisfies \(\hat{E}_t = E_t = E\).
References
Empirically, it seems that E_t is actually equal to the ray class field E in \Cref{thm:RayClassField2}, and indeed a similar statement may be made when Q is not fundamental. As we do not know how to prove this from any form of the Stark conjectures in the literature, we state it as a separate conjecture. Let t=(d,r,Q)\sim(K,j,m,Q) be an admissible tuple, let d=d_{j,m}, and let f be the conductor of Q. Let E= H{\OO_f}_{\db\infty_1\infty_2} be the ray class field with level datum (\mcl{O}_f; \db \mcl{O}_f,(\infty_1,\infty_2)), as defined by \Cref{thm:rayclassfield}. Then \hat{E}_t = E_t = E.
The statements regarding the algebraic nature of these complex numbers remain conjectural.
The study of SIC fields has led to several conjectures, such as the so-called Ray Class Field Conjecture: Let d > 3, and let K_d = Q(√((d + 1)(d − 3))). Then E_{Π(v)} is an Abelian extension of K_d. Furthermore, there is at least one SIC-POVM whose corresponding SIC field is equal to R, the ray class field of K_d. Moreover, every other SIC field in dimension d is a finite Galois extension of Q containing R.