Stack Exchange network consists of 183 Q&A communities including Stack Overflow, the largest, most trusted online community for developers to learn, share their knowledge, and build their careers.
Another (nicer) way to get the product in Tate cohomology, from a pairing of (co-)chain complexes, appears in Definition 4.1.5 of Hesselholt, Lars; Madsen, Ib On the K-theory of local fields. Ann. of Math. (2) 158 (2003), no. 1, 1–113.
This is not what you ask for, but perhaps it is worth mentioning that there is an $E_\infty$-algebra $gr_{ev}^* S/I_\infty$ in $gr_{ev}^* S$-modules, corresponding to the even commutative $MU_* MU$-comodule algebra $MU_*/I_\infty$, so $gr_{ev}^* MU/I_\infty$ exists as an $E_\infty$-$MU$-algebra in that category.
The formula is usually given for $\zeta(1-n)$, with $K_{2n-2}$ in the numerator and $K_{2n-1]$ in the denominator. When written as a formula for $\zeta(-n)$, the denominator must involve $K_{2n+1}$.
@FShrike Yes, Fritsch and Puppe (1967) proved that for each simplicial set $X$ there exists a homeomorphism $|sd(X)| \cong |X|$, where sd is Kan's normal subdivision. See e.g. section 2.3 in mn.uio.no/math/personer/vit/rognes/papers/aoms186-nocrop.pdf for more history, references, and generalizations. We write Sd and B for your sd and S.
The construction for Witt vectors of finite fields was effectively given in "Schwänzl, R.; Vogt, R. M.; Waldhausen, F. Adjoining roots of unity to $\mathbb{E}_\infty$ ring spectra in good cases—a remark. Homotopy invariant algebraic structures (Baltimore, MD, 1998), 245–249, Contemp. Math., 239, Amer. Math. Soc., Providence, RI, 1999", and these authors also proved that $\mathbb{Z}[i]$ cannot be lifted to the sphere.
Are any of the slightly more recent references in Section 6 of Sullivan, Dennis René Thom's work on geometric homology and bordism. Bull. Amer. Math. Soc. (N.S.) 41 (2004), no. 3, 341–350 ams.org/journals/bull/2004-41-03/S0273-0979-04-01026-2 of use to you?
From the chromatic point of view, the case p=2 is perhaps a bit surprising, since \pi_1 of the K-local sphere is (Z/2)^2, and only one of these comes from \pi_1 of the sphere. The definition of the connective image-of-J spectrum j involves some tweaking (compared to taking the connective cover of L_K(S)), precisely to get rid of that extra Z/2.
For \pi_3^S, do you use the binary tetrahedral group as a superperfect cover of A_4? Why is this already in the stable range for H_3 (which I expect starts at A_8)?
Isn't Nakaoka's integral (co-)homological stability range for \Sigma_p --> \Sigma_\infty more like * \le p/2 than * \le 2p-2 ? The mod p stability range is better, as you write.