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ssTTsSTtRrriinInnnnNNNIiinngg



Construction of a K(pi_1)- space?


Does a function space construction always decrease the connectivity of a space?$pi_1(S^n)=0$ for $ngeq2$Question on part of the proof that $pi_1(X,x_0)$ is isomorphic to $pi_1(X,x_1)$A standard proof of $pi_1(mathbbS^1) = mathbbZ$ using universal covering spacesRole of the Thom space in the Pontryagin-Thom constructionShow $pi_1(SU(2)/H_8)$Construction of K(G,1) spaceHomotopy constructionProve that $pi_1(Xtimes Y, (x_0,y_0))$ is isomorphic to $pi_1(X,x_0)times pi_1(Y,y_0)$.The meaning of $pi_1(S^1,(1,0))$













1












$begingroup$


I was advised to post my question here. A colleague suggested a proof of a fact which I have hard time to believe. Since I am not a topologist by training I wonder if this can be true in such a generality.



Consider any finite CW-complex structure on the 𝑑-dimensional sphere $𝑆^𝑑$. Let $𝐾$ be $𝑆^𝑑$ with all strata of codimension at least 2 removed, i.e. we keep just 𝑑 and (𝑑−1)-dimensional strata of the complex under consideration.



Claim. K is contractible to a graph (the dual graph of the preserved strata). Thus it is a $K(pi_1, 1)$- space where $pi_1$ is a free group.



The claim is trivially true for d=2, but looks suspicious for higher d. Also if it is true then it might work for more general CW-complexes as well.



Best regards, Boris Shapiro/Stockholm University/










share|cite|improve this question









$endgroup$











  • $begingroup$
    What do you mean more precisely ? For instance for $d=2$ if you take the standard cell-structure with one $2$-cell and one $0$-cell, how do you un-collapse the boundary of the $2$-cell ?
    $endgroup$
    – Max
    Mar 21 at 8:02










  • $begingroup$
    Well, in this case you remove the point. The remaining part in the 2-disk which is contractible to a point. $pi_1$ is trivial. In general, in 2 dimensions, you remove a bunch of points (at least one). The remaining punched disc is homotopy equivalent to a wedge of circles.
    $endgroup$
    – user53092
    Mar 21 at 10:47










  • $begingroup$
    Oh ok so just literally remove. Sorry for my question, I thought you meant something more sophisticated.
    $endgroup$
    – Max
    Mar 21 at 10:58















1












$begingroup$


I was advised to post my question here. A colleague suggested a proof of a fact which I have hard time to believe. Since I am not a topologist by training I wonder if this can be true in such a generality.



Consider any finite CW-complex structure on the 𝑑-dimensional sphere $𝑆^𝑑$. Let $𝐾$ be $𝑆^𝑑$ with all strata of codimension at least 2 removed, i.e. we keep just 𝑑 and (𝑑−1)-dimensional strata of the complex under consideration.



Claim. K is contractible to a graph (the dual graph of the preserved strata). Thus it is a $K(pi_1, 1)$- space where $pi_1$ is a free group.



The claim is trivially true for d=2, but looks suspicious for higher d. Also if it is true then it might work for more general CW-complexes as well.



Best regards, Boris Shapiro/Stockholm University/










share|cite|improve this question









$endgroup$











  • $begingroup$
    What do you mean more precisely ? For instance for $d=2$ if you take the standard cell-structure with one $2$-cell and one $0$-cell, how do you un-collapse the boundary of the $2$-cell ?
    $endgroup$
    – Max
    Mar 21 at 8:02










  • $begingroup$
    Well, in this case you remove the point. The remaining part in the 2-disk which is contractible to a point. $pi_1$ is trivial. In general, in 2 dimensions, you remove a bunch of points (at least one). The remaining punched disc is homotopy equivalent to a wedge of circles.
    $endgroup$
    – user53092
    Mar 21 at 10:47










  • $begingroup$
    Oh ok so just literally remove. Sorry for my question, I thought you meant something more sophisticated.
    $endgroup$
    – Max
    Mar 21 at 10:58













1












1








1


1



$begingroup$


I was advised to post my question here. A colleague suggested a proof of a fact which I have hard time to believe. Since I am not a topologist by training I wonder if this can be true in such a generality.



Consider any finite CW-complex structure on the 𝑑-dimensional sphere $𝑆^𝑑$. Let $𝐾$ be $𝑆^𝑑$ with all strata of codimension at least 2 removed, i.e. we keep just 𝑑 and (𝑑−1)-dimensional strata of the complex under consideration.



Claim. K is contractible to a graph (the dual graph of the preserved strata). Thus it is a $K(pi_1, 1)$- space where $pi_1$ is a free group.



The claim is trivially true for d=2, but looks suspicious for higher d. Also if it is true then it might work for more general CW-complexes as well.



Best regards, Boris Shapiro/Stockholm University/










share|cite|improve this question









$endgroup$




I was advised to post my question here. A colleague suggested a proof of a fact which I have hard time to believe. Since I am not a topologist by training I wonder if this can be true in such a generality.



Consider any finite CW-complex structure on the 𝑑-dimensional sphere $𝑆^𝑑$. Let $𝐾$ be $𝑆^𝑑$ with all strata of codimension at least 2 removed, i.e. we keep just 𝑑 and (𝑑−1)-dimensional strata of the complex under consideration.



Claim. K is contractible to a graph (the dual graph of the preserved strata). Thus it is a $K(pi_1, 1)$- space where $pi_1$ is a free group.



The claim is trivially true for d=2, but looks suspicious for higher d. Also if it is true then it might work for more general CW-complexes as well.



Best regards, Boris Shapiro/Stockholm University/







homotopy-theory






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Mar 21 at 6:30









user53092user53092

62




62











  • $begingroup$
    What do you mean more precisely ? For instance for $d=2$ if you take the standard cell-structure with one $2$-cell and one $0$-cell, how do you un-collapse the boundary of the $2$-cell ?
    $endgroup$
    – Max
    Mar 21 at 8:02










  • $begingroup$
    Well, in this case you remove the point. The remaining part in the 2-disk which is contractible to a point. $pi_1$ is trivial. In general, in 2 dimensions, you remove a bunch of points (at least one). The remaining punched disc is homotopy equivalent to a wedge of circles.
    $endgroup$
    – user53092
    Mar 21 at 10:47










  • $begingroup$
    Oh ok so just literally remove. Sorry for my question, I thought you meant something more sophisticated.
    $endgroup$
    – Max
    Mar 21 at 10:58
















  • $begingroup$
    What do you mean more precisely ? For instance for $d=2$ if you take the standard cell-structure with one $2$-cell and one $0$-cell, how do you un-collapse the boundary of the $2$-cell ?
    $endgroup$
    – Max
    Mar 21 at 8:02










  • $begingroup$
    Well, in this case you remove the point. The remaining part in the 2-disk which is contractible to a point. $pi_1$ is trivial. In general, in 2 dimensions, you remove a bunch of points (at least one). The remaining punched disc is homotopy equivalent to a wedge of circles.
    $endgroup$
    – user53092
    Mar 21 at 10:47










  • $begingroup$
    Oh ok so just literally remove. Sorry for my question, I thought you meant something more sophisticated.
    $endgroup$
    – Max
    Mar 21 at 10:58















$begingroup$
What do you mean more precisely ? For instance for $d=2$ if you take the standard cell-structure with one $2$-cell and one $0$-cell, how do you un-collapse the boundary of the $2$-cell ?
$endgroup$
– Max
Mar 21 at 8:02




$begingroup$
What do you mean more precisely ? For instance for $d=2$ if you take the standard cell-structure with one $2$-cell and one $0$-cell, how do you un-collapse the boundary of the $2$-cell ?
$endgroup$
– Max
Mar 21 at 8:02












$begingroup$
Well, in this case you remove the point. The remaining part in the 2-disk which is contractible to a point. $pi_1$ is trivial. In general, in 2 dimensions, you remove a bunch of points (at least one). The remaining punched disc is homotopy equivalent to a wedge of circles.
$endgroup$
– user53092
Mar 21 at 10:47




$begingroup$
Well, in this case you remove the point. The remaining part in the 2-disk which is contractible to a point. $pi_1$ is trivial. In general, in 2 dimensions, you remove a bunch of points (at least one). The remaining punched disc is homotopy equivalent to a wedge of circles.
$endgroup$
– user53092
Mar 21 at 10:47












$begingroup$
Oh ok so just literally remove. Sorry for my question, I thought you meant something more sophisticated.
$endgroup$
– Max
Mar 21 at 10:58




$begingroup$
Oh ok so just literally remove. Sorry for my question, I thought you meant something more sophisticated.
$endgroup$
– Max
Mar 21 at 10:58










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