Refined higher norm formula for Rubin–Stark units

Let (L,S,V),(L,S,V)Ω(L,S,V),(L',S',V')\in\Omega with LLL\subset L', SSS\subset S', and VVV\supset V'. Put r=Vr=|V|, r=Vr'=|V'|, and d=rrd=r-r'. Let φv:L×QL/L1\varphi_v:L^\times\to Q_{L'/L}^1 be the local-reciprocity map defined in the source for vVv\in V, let sgn(V,V)\operatorname{sgn}(V,V') be the sign determined by the ordered exterior products, and let ii be the canonical injection. Refined higher norm conjecture. The higher norm descent conjecture holds, and

i1(NL/L(r,d)(εL,S,V))=sgn(V,V)(vSS(1Frv1))(vVVφv)(εL,S,V).i^{-1}\bigl(N_{L'/L}^{(r',d)}(\varepsilon_{L',S',V'})\bigr)=\operatorname{sgn}(V,V')\left(\prod_{v\in S'\setminus S}(1-\operatorname{Fr}_v^{-1})\right)\left(\bigwedge_{v\in V\setminus V'}\varphi_v\right)(\varepsilon_{L,S,V}).

This is the main refined compatibility prediction for Rubin–Stark units under extension and change of auxiliary data; the source gives no general resolution.

Sources & referencesView supporting material

Primary source

Takamichi Sano, “Refined abelian Stark conjectures and the equivariant leading term conjecture of Burns”, arXiv:1406.4623 (2014).

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