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Worked solution: Hill-Hopkins-Ravenel proof via equivariant stable homotopy theory (2009)

Step 5 of 9: The Slice Theorem: identifying the layers of MU((C8))MU^{((C_8))}
In plain words

Just as an ordinary space can be studied one Postnikov stage at a time, HHR filter their equivariant spectrum by "slices" — an equivariant analogue of the Postnikov tower, indexed not just by an integer but adapted to the group action.

The Slice Theorem is the single computational engine behind everything else: it says each layer of this filtration for MU((C8))MU^{((C_8))} is built purely from ordinary (non-equivariant) integer cohomology, glued together according to a completely explicit recipe — turning a hard equivariant question into bookkeeping with ordinary cohomology.

PnnMU((C8))≃HZ‾∧Wn(slice tower)P_n^n MU^{((C_8))} \simeq H\underline{\mathbb{Z}} \wedge W_n \quad (\text{slice tower})
Detailed analysis

The slice filtration (§4) associates to any equivariant spectrum XX a tower of "slice sections" PnXP^n X, built by attaching cells that kill all maps from cells of dimension greater than nn; the layers PnnXP_n^n X (the "slices") assemble into the slice spectral sequence computing π∗X\pi_* X.

The Slice Theorem (Theorem 1.13, proved via a Reduction Theorem in §6-7) identifies the slices of MU((C8))MU^{((C_8))} explicitly: PnnMU((C8))P_n^n MU^{((C_8))} is a wedge of copies of the equivariant Eilenberg-Mac Lane spectrum HZ‾H\underline{\mathbb{Z}} (for the constant Mackey functor Z‾\underline{\mathbb{Z}}) smashed with specific "slice cells" of dimension nn built from induced representation spheres.

Because every slice is this explicit, the slice spectral sequence for MU((C8))MU^{((C_8))} (and, after further work, for the detecting theory Ω\Omega) becomes a concrete, computable object — the basis for both the Gap Theorem (next step) and the Periodicity Theorem.

Terms in this step
Slice filtration
An equivariant analogue of the Postnikov tower that filters a GG-spectrum by "slice cells" built from induced representation spheres, rather than by ordinary dimension alone.
Eilenberg-Mac Lane spectrum (HZ‾H\underline{\mathbb{Z}})
The equivariant spectrum representing ordinary Bredon cohomology with coefficients in a Mackey functor, here the constant integer Mackey functor Z‾\underline{\mathbb{Z}}; the simplest possible building block a slice can be made from.
Knowledge used in this step