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

Step 6 of 9: The Gap Theorem: no room near the bottom
In plain words

Once the slices of MU((C8))MU^{((C_8))} are known explicitly (previous step), a short computation — the "Cell Lemma" — shows certain equivariant homotopy groups of these building blocks simply vanish in a narrow range near degree 00, because the relevant orbit spaces turn out to be simply connected.

Stacking this vanishing across every layer of the slice tower shows the homotopy groups of the whole detecting theory Ω\Omega vanish in that same narrow range — a "gap" with no room for anything to survive.

Ωi(pt)=0(0<i<4)\Omega^i(\mathrm{pt}) = 0 \quad (0 < i < 4)
Detailed analysis

The Cell Lemma (Lemma 1.14) computes that for G=C2nG = C_{2^n} and any slice cell S^\widehat S, the equivariant homotopy groups πkGHZ‾∧S^\pi_k^G H\underline{\mathbb{Z}} \wedge \widehat S vanish for −4<k<0-4 < k < 0; this reduces to the elementary fact that the orbit space SmρG/GS^{m\rho_G}/G is simply connected, being the suspension of a connected space.

Combining the Cell Lemma with the Slice Theorem's explicit description of the slices of MU((C8))MU^{((C_8))} (and hence of ΩO\Omega_{\mathbb{O}}), HHR show the C8C_8-fixed-point homotopy groups πiC8ΩO\pi_i^{C_8}\Omega_{\mathbb{O}} vanish for −4<i<0-4<i<0.

The Homotopy Fixed Point Theorem of a later step identifies these groups with πiΩ\pi_i \Omega itself, giving the Gap Theorem: Ωi(pt)=0\Omega^i(\mathrm{pt}) = 0 for 0<i<40<i<4 — exactly the vanishing range the final assembly step needs.

Terms in this step
Cell Lemma
A short computation showing that certain low-degree equivariant homotopy groups of Eilenberg-Mac Lane spectra smashed with slice cells vanish, because the relevant orbit space is simply connected.
Knowledge used in this step