Link to S5 and S4(m)

Ammar Husain

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{MeissnerNicolai18a} Krzysztof A. Meissner, Hermann Nicolai,

*Standard Model Fermions and Infinite-Dimensional R-Symmetries*, Phys. Rev. Lett. 121, 091601 (2018) (arXiv:1804.09606){#MeissnerNicolai18b} Krzysztof A. Meissner, Hermann Nicolai,

*Planck Mass Charged Gravitino Dark Matter*, Phys. Rev. D 100, 035001 (2019) (arXiv:1809.01441)

added pointer to

- Daniel Gratzer,
*Implementing Modal Dependent Type Theory*, talk at ICFP 19 (slides pdf)

I see how to do it “by hand” for the special case where

$G = \mathbb{Z}_2$

$V = \mathbb{R}^n_{\mathrm{sgn}} \coloneqq (\mathbb{R}^1_{sgn})^n$ a sign representation.

The corresponding representation torus $\mathbb{T}^n_{sgn} \coloneqq \mathbb{R}^n_{sgn}/\mathbb{Z}^n$ has $2^n$ fixed points (those points all whose coordinate components are in $\big\{[0 \, mod \, \mathbb{Z}],[\tfrac{1}{2}\, mod \, \mathbb{Z}] \big\}$) and every small enough disk around each of these is equivariantly isomorphic to the unit disk around the origin in $\mathbb{R}^n_{\mathrm{sgn}}$.

Hence at the start of the induction an equivariant map $(\mathbb{T}^n_{sgn})_+ \to S^{\mathbb{R}^n_{sgn}}$ is a choice in $(\mathbb{Z}_2)^{(2^{n})}$ saying whether a fixed point gets send to 0 or to $\infty$. This extends by sending a small disk around each fixed point going to 0 identically to $D(\mathbb{R}^n_{sgn}) \simeq S^{n}_{\mathrm{sgn}} \setminus \{\infty\}$ and sending all remaining points to $\infty$.

An illustration is here.

Hence, proceeding from here with tom Dieck’s proof, the full set of unstable equivariant Hopf degrees in this case should be

$\array{ \pi^{\mathbb{R}^n_{sgn}} \big( (\mathbb{T}^n_{sgn})_+ \big) &\underoverset{\simeq}{deg_{\mathbb{Z}_2}}{\longrightarrow}& (\mathbb{Z}_2)^{(2^{n})} \times \big( 2 \cdot \mathbb{Z} \big) \\ [\mathbb{T}^n_{sgn} \overset{c}{\to} S^n_{sgn}] &\mapsto& \big( deg(c^{\mathbb{Z}_2}), deg(c) \big) }$with the second factor $\mathbb{Z}$ being the ordinary Hopf degree of the full underlying map.

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Jason Gross

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Jason Gross

]]>And while the long list of articles by Jaworowski aim to relax the assumptions of the Tietze-Gleason extension theorem, they all assume (as far as I see) that the codomain is an absolute retract (non-equivariantly), hence contractible. So these stronger extension theorems all still yield the same situation as in #7, it seems.

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]]>splitting off this definition from *neighborhood retract*, for ease of linking, and in order to record the characterization AR = ANR+contractible

Hm, so the plain Tietze-Gleason extension theorem does *not* give all possible extensions: Since the theorem needs the function $(V/N)^G \overset{f}{\to} S^V$ to factor through the Euclidean $G$-space $V \subset S^V$, it only serves to extend those $f$ which take all fixed points to $0 \in V \subset S^V$, none to $\infty \in S^V$.

Now, for our application it would be very interesting if it turned out that equivariant Cohomotopy classes $(V/N)_+ \longrightarrow S^V$ had to necessarily take *all* fixed points of $(V/N)$ to $0 \in V$ (with $dim(V) \geq 2$). Might this be the case?! At least, the Tietze-Gleason theorem does not say otherwise.

Thanks!

]]>added statement of the basic Tietze-Gleason extension theorem (here), as in Palais 60, Theorem 1.4.3

]]>Thanks a lot, Toby! This looks very good.

]]>Yes, I agree the word should be “transitive”.

]]>Well, from one perspective there’s not much to say, since $V Cat$ is a 2-category and all of that is 2-categorical abstract nonsense. But I think there’s some particular discussion of enriched monads in Dubuc’s book Kan Extensions in Enriched Category Theory.

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The following is a conversation I am having with David Roberts, but everyone please join in if you feel like it:

So tomDieck 79, Sec 8.4 states the equivariant Hopf degree theorem for characterizing, say, equivariant Cohomotopy sets

$\pi^V(X) \;\coloneqq\; \pi_0 Maps^{\ast/}(X, S^V)^G$(for $X$ a pointed $G$-CW-complex which matches the given representation sphere $S^V$)

under the *simplifying assumption* (middle of p. 212) that the full fixed locus of $X$ has positive dimension: $dim\left(X^G\right) \geq 1$.

It seems pretty clear that the only difficulty for tom Dieck in removing that assumption would have been one of notation (dealing with the case distinctions that ensue), but for the record, I’d like to spell it out.

More concretely, the issue in removing the assumption $dim\left(X^G\right) \geq 1$ should all be in starting the induction (top of p. 214) in the proof of Theorem 8.4.1:

Given a map $f \colon X^G \longrightarrow S^V$ we need to see that this extends $W_G(H_1)$-equivariantly along $X_0 \coloneqq X^G \hookrightarrow X_1$, where $X_1 \subset X$ is the subspace of points whose isotropy groups are conjugate to at least the second largest subgroup $H_1$ (under some choice of linear ordering – bottom of p. 203 ).

I think the existence of that extension is all one needs to check in order to generalize to the case that $dim(X^G)$ may vanish, but let me know if I am mixed up.

For example if $X = S^V$ itself, the extension does exist, either as the constant map or the identity map, and we get the statement from #4.

Now how about the case that $X = ( V/N )_+$ is a Euclidean $G$-torus (as here)? Should be easy, but I still need to nail it down.

And more generally?

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]]>I have added pointers to these references:

Zalman Balanov,

*Equivariant Hopf theorem*, Nonlinear Analysis: Theory, Methods & Applications Volume 30, Issue 6, December 1997, Pages 3463-3474 (doi:10.1016/S0362-546X(97)00020-5)Davide L. Ferrario,

*On the equivariant Hopf theorem*,*Topology Volume 42, Issue 2, March 2003, Pages 447-465*(doi:10.1016/S0040-9383(02)00015-0)

(also at *equivariant cohomotopy*)