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2:14 AM
Take K theory and try killing p as a K-algebra. There’s a sseq that starts with the free associative algebra over K_* on a generator in degree 1, the differential takes that generator to p. The Leibniz rule says x^2 is a cycle, and it survives. So now you have this junk in degree 2, so you gotta kill that with a new E_1-cell! That puts new junk in degree 4... now keep doing that forever. Then you’ve built K(1) as a K-algebra with infinitely many E_1-cells; one in each even degree
By no coincidence at all, that’s also what the cell structure of CP^infty looks like (as we see by looking at the Thom spectrum construction)
 
skd
3:12 AM
regardless of the choices of the v_i's you make, is there a unique spectrum with homotopy K(n)_*? (and similarly for E(n)_*)
unique as a spectrum, that is, with no additional structure
 
 
2 hours later…
5:37 AM
Maybe I’m misinterpreting but couldn’t you just take a wedge of EM spectra?
 
skd
6:08 AM
ah, yes, of course. i probably want to ask for uniqueness as an MU-module
 
 
2 hours later…
8:35 AM
@DylanWilson Where can I read about this. In particular this spectral sequence, is it in HA somewhere?
 
 
6 hours later…
2:54 PM
Here for example: arxiv.org/abs/1805.07184
Also I should’ve said there’s cells in odd degrees- but it’s still modeled on CP^infty cuz these E_k stories have a shift by k...
 
3:54 PM
@DylanWilson Thanks!
 
 
1 hour later…
5:17 PM
@skd As far as I understand you don't need to make a choice for the $v_i$'s in $BP$ and therefore in $E(n)$ (Johnson-Wilson), am I wrong?
Also for Lubin-Tate you usually choose the fgl on $Wk[[u_1,\dotsc,u_{n-1}]][u^{\pm 1}]$ so that $v_i$ is sent to $u_i u^{p^i-1}$ (or some other power if I got it wrong), right?
 
5:59 PM
we
 
6:19 PM
(sorry about that, problematic keyboard...)
 

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