@TedShifrin I actually didn't know what he meant when he asked for a "simple" example of a manifold with $\pi_1 \neq 0$ and $H_1 = 0$. I started saying Poincare homology sphere and asked if I should give the construction but he didn't like it.
I have a group $G=\{f^rh^s: r=0,1;s=0,1,2\}$, where $f$ is map that reflects $(x,y)$ about y axis. $h$ rotates $(x,y)$ anti-clockwise by $2\pi/3$. A formula is to be found that expresses $(f^ih^j)*(f^sh^t)$ as $f^ah^b$
First you have to triangulate the CW complex. This can be done precisely because the complex you get by attaching 2-cells to a wedge of circles according to relators is a nice CW complex; the attaching maps are simplicial.
Next, any simplicial complex of dimension $n$ embeds in $\Bbb R^{2n+1}$. This is by using the twisted cubic, consider the curve $(t, t^2, t^3, \cdots, t^{2n+1})$. Pick any two different collection of $n$ points. Their convex hulls are always disjoint.
oh. it might be simpler to do it without coordinate formulas for f and h. or maybe jsut the single one you arguably need to move f past h (even then, arguable)
Here's what it is. Let $G = \langle g_1, \cdots, g_n | r_1, \cdots, r_n \rangle$ be any finitely presented group. Take $(S^1 \times S^3) \# \cdots \# (S^1 \times S^3)$, $n$ copies, indexed by $g_1, \cdots, g_n$. This is a manifold with fundamental group $F_n = F\langle g_1, \cdots, g_n \rangle$, because connected sum is along $S^3$'s, which do not contribute to $\pi_1$ @Thorgott
Now, pick a smooth embedded loop $\gamma$ representing $r_1$ in the fundamental group. Take a regular neighborhood of this, which is $\nu(\gamma) = S^1 \times D^3$. Throw it's interior out. This leaves a boundary of $S^1 \times S^2$; but plug a $D^2 \times S^2$ along it.
This is known as surgery, as you're aware. This gives a new manifold with fundamental group $\langle g_1, \cdots, g_n | r_1 \rangle$. Repeat with $r_2$, but you have to make sure that the embedded loop representing it does not hit the disk $D^2$ that $\gamma$ bounds in the first surgery operation. This is easy, as 1 + 2 = 3 < 4 quick maths.
So by transversality, you can keep repeating the argument, to get a 4-manifold with fundamental group $G$. This is exactly a closed handlebody version of the nbhd of 2-complex thing.
For a while I thought Balarka Sen was answering my question when they said let $G$ be any finitely presented group. I had also written presentation of G above :)
what would be an easy way to compute the homology of all subsimplices of dimension $\leq k \leq d$ (the $k$-skeleton) of some standard $d$-simplex $\Delta^d$?
@koro it seems like from what they're asking you want to push h to the right. but your fh = h^{-1} f formula will get you there. left multiply by h [getting hfh = f] then right multiply by h^{-1} [getting hf = fh^{-1}, or as h^3 = 1, hf = fh^2]
@BalarkaSen oh and it would be zero for $n = 1$ as well, so would the answer be $H_k$ would be free abelian on the $k$-subsimplices, and $H_0$ would be $\mathbb{Z}$?
@geocalc i'm not sure i understand the context. i note that your use of the term 'lattice' is slightly out of sync with another use of this term, although i guess i kind of understand it. i don't see much 'snapping into place' as s grows, i just see points being pushed down to the x axis as their x coordinates get bigger.
I'm actually kind of stuck at the beginning, where they define $A$ as an integer matrix being an element of the special linear group. I'm not sure how to translate this info if the lattice in my question doesn't have co-volume equal to 1
geocalc: it is the image under a diffeomorphism of a subset of a lattice of Z^2. these details start to matter if you want to consider groups (particularly matrix groups) acting on them
the sets of prime pairs, in Z^2, are not a lattice (e.g. because it is dramatically not closed under addition: if (p,q) is in there, (p,q) + (p,q) = (2p, 2q) will not be)
it doesn't really 'act on' that subset if it doesn't send that subset to itself. it just moves it from one place to another. i'm also not convinced that your definition plays nice with matrix multiplication.
what's the end goal here?
note, if you just want to compute the image of a R under a map, which you might regard as an "orbit" of f(1) if you regard the parameter t as time, you don't need groups or matrices to begin that project
i'm not sure what the purpose is, let alone whether you need the matrix stuff to do it
again, just for purposes of reconciling this with what you may be reading, 'flow on X,' 'acting on X' and related terms often require that X be mapped to itself for all inputs, which is not happening here
that's just terminology but i figured i would point it out