intro
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biblio.bib
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biblio.bib
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@article {acgm,
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AUTHOR = {Artal, E. and Cogolludo, J.I. and {Guerville-Ball\'e}, B. and Marco, M.\'A.},
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TITLE = {An arithmetic {Z}ariski pair of line arrangements with
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non-isomorphic fundamental group},
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JOURNAL = {Rev. R. Acad. Cienc. Exactas F\'is. Nat. Ser. A Mat. RACSAM},
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FJOURNAL = {Revista de la Real Academia de Ciencias Exactas, F\'isicas y
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Naturales. Serie A. Matematicas. RACSAM},
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VOLUME = {111},
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YEAR = {2017},
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NUMBER = {2},
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PAGES = {377--402},
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ISSN = {1578-7303,1579-1505},
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DOI = {10.1007/s13398-016-0298-y},
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URL = {https://doi.org/10.1007/s13398-016-0298-y},
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}
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@Article{Libgober1986,
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author = {A. Libgober},
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journal = {J. Reine Angew. Math.},
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title = {On the homotopy type of the complement to plane algebraic curves},
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year = {1986},
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pages = {103--114},
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volume = {367},
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fjournal = {Journal f{\"u}r die Reine und Angewandte Mathematik},
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}
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@article {andreotti1959,
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AUTHOR = {Andreotti, A. and Frankel, T.},
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TITLE = {The {L}efschetz theorem on hyperplane sections},
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JOURNAL = {Ann. of Math. (2)},
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FJOURNAL = {Annals of Mathematics. Second Series},
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VOLUME = {69},
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YEAR = {1959},
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PAGES = {713--717},
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ISSN = {0003-486X},
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DOI = {10.2307/1970034},
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URL = {https://doi.org/10.2307/1970034},
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}
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@Manual{Sagemath,
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title = {Sage {M}athematics {S}oftware ({V}ersion 10.10)},
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author = {Stein, W.A. and others},
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note = {{\tt http://www.sagemath.org}},
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organization = {The Sage Development Team},
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year = {2026},
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key = {Sage},
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}
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@ -35,7 +35,7 @@ decorations.markings, calc}
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\numberwithin{equation}{section}
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\numberwithin{equation}{section}
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%opening
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%opening
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\title[Retraction of the complement of a smooth curve]{Retraction of the complement of smooth projective hypersurfaces to a $n$-dimensional $\Delta$-complex.}
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\title[Retraction of the complement of a smooth curve]{Retraction of the complement of smooth projective hypersurfaces to an $n$-dimensional $\Delta$-complex.}
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\author[E. Artal]{Enrique Artal Bartolo}
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\author[E. Artal]{Enrique Artal Bartolo}
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\address{Departamento de Matem\'{a}ticas, IUMA \\
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\address{Departamento de Matem\'{a}ticas, IUMA \\
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Universidad de Zaragoza \\
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Universidad de Zaragoza \\
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@ -71,17 +71,29 @@ MICIU/AEI/10.13039/501100011033 and CEX2021-001142-S-20-9.}
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\begin{abstract}
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\begin{abstract}
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We give an explicit strong deformation retraction of the complement of a Fermat hypersurface of degree $d$ in the complex projective space of dimension $n$ into a $\Delta$-complex of real dimension~$n$.
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%Due to a result by Andreotti and Frankel \cite{andreotti1959}, it can be seen that the complement of a complex projective curve has the homotopy type of a $2$-dimensional CW complex. However, no general method has been given to compute explicitly this complex. Here we give a explicit construction of a $n$- dimensional $\Delta$-complex that is a strong deformation retract of the complement of a Fermat hypersurface of degree $d$ in the complex projective space of dimension $n$.
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Due to a result by Andreotti and Frankel \cite{andreotti1959}, it can be seen that the complement of a complex projective curve has the homotopy type of a $2$-dimensional CW complex. However, no general method has been given to compute explicitly this complex. Here we give a explicit construction of a $n$- dimensional $\Delta$-complex that is a strong deformation retract of the complement of a Fermat hypersurface of degree $d$ in the complex projective space of dimension $n$.
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This retraction is performed in several steps, using the branched cover structure of the Fermat hypersurfaces to the degree $1$ case. Moreover, an implementation of the method in \texttt{Sagemath} is provided.
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The retraction is performed in several steps, using the branched cover structure of the Fermat hypersurfaces to the degree $1$ case.
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\end{abstract}
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\end{abstract}
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\maketitle
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\maketitle
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\section{Definition of the problem}
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\section*{Introduction}
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Given $C$ an affine hypersurface in $\CC^2$ (i.e. a curve), Libgober gave in \cite{libgober1986} a construction of a $2$-dimensional CW-complex that is a deformation retract of its complement. However, it is not clear how to extend that construction to the projective case (that is a curve in $\CC\PP^2$).
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A result of Andreotti and Frankel \cite{andreotti1959} asserts that any affine smooth variety of complex dimension~$n$ has the homotopy type of a CW-complex of real dimension~$n$. Using the Segre embedding, it is not hard
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to check that the complement of a hypersurface in $\PP^n$ is isomorphic to an affine variety.
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However, no general method has been given to compute explicitly this complex.
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Since there are hypersurfaces with equations in a number field $K$ whose embedding depend on the embedding $K\hookrightarrow\CC$ (even up to homotopy)~\cite{acgm}, a purely algebraic method cannot exist.
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In this work, we give a different construction to produce a specific $\Delta$-complex that is a deformation retract of the complement of a Fermat hypersurface in $\CC\PP^n$. Since any smooth hypersurface is isotopic to a Fermat hypersurface, this particular case solves the problemfor a general smooth hypersurface.
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Possibly the only known method applies to the following particular case.
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%One main problem is to provide such a CW-complex.
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Given $C$ an affine curve in $\CC^2$, Libgober gave in \cite{libgober1986} a construction of a $2$-dimensional CW-complex that is a deformation retract of its complement, using braid monodromy which is not an algebraic construction. In the previous language a complement of an affine curve ins $\CC^2$ is the complement of a projective curve~$C$ in $\PP^2$, where $C$ contains a line $L$ (which can be seen as the line at infinity).
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However, it is not clear how to extend that construction to the projective case, that is a curve in $\CC\PP^2$ such that no irreducible component is a line, e.g. a smooth curve of degree $>1$.
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In this work, we give a different construction to produce a specific $\Delta$-complex that is a deformation retract of the complement of a $d$-Fermat hypersurface in $\CC\PP^n$. Since any smooth hypersurface is isotopic to a Fermat hypersurface, this particular case gives a construction for the more general of smooth hypersurfaces.
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The actual construction starts with the trivial case $d=1$. In this case the complement is contractible and a point would suffice as $\Delta$-complex. Actually we will take a simplex of real dimension~$n$ which is also contractible.
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The main point is to understand the lifting of this complex by the Kummer cover $[x_0:\dots:x_n]\mapsto[x_0^d:\dots:x_n^d]$.
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\section{Smooth hypersurfaces}
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\section{Smooth hypersurfaces}
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@ -145,21 +157,11 @@ and the restriction of $r_{1t}$ to $M_1\cap\RR^{n+1}$ is the inclusion.
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%where $\Re$ and $\Im$ take the real and imaginary part of each coordinate of a point, respectively.
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%where $\Re$ and $\Im$ take the real and imaginary part of each coordinate of a point, respectively.
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Note that for $(x_0,\dots,x_n)\in M_1$, we already have that
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Note that for $(x_0,\dots,x_n)\in M_1$, we already have that
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<<<<<<< HEAD
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\begin{equation*}
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\begin{array}{lll}
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\sum x^r_j & = & 1 \\
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\sum x^i_j & = & 0 \\
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\end{array}
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\end{equation*}
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and therefore $r_1(x_0,\dots,x_n,t)\in M_1$ for all $t\in[0,1]$, and in particular, we get that $r_1(x_0,\dots,x_n,1)=(x^r_0,\dots,x^r_n)\in M_1\cap\RR^{n+1}$ for all $(x_0,\dots,x_n)\in M_1$.
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=======
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\begin{align*}
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\begin{align*}
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\sum_{j=0}^n x^r_j & = 1 \\
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\sum_{j=0}^n x^r_j & = 1 \\
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\sum_{j=0}^n x^i_j & = 0 \\
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\sum_{j=0}^n x^i_j & = 0 \\
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\end{align*}
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\end{align*}
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and therefore $r_1(x_0,\dots,x_n,t)\in M_1$ for all $t\in[0,1]$, and in particular, we get that $r_1(x_0,\dots,x_n,1)=(x^r_0,\dots,x^r_n)\in M_1\cap\RR^{n+1}$ for all $(x_0,\dots,x_n)\in M_1$.
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and therefore $r_1(x_0,\dots,x_n,t)\in M_1$ for all $t\in[0,1]$, and in particular, we get that $r_1(x_0,\dots,x_n,1)=(x^r_0,\dots,x^r_n)\in M_1\cap\RR^{n+1}$ for all $(x_0,\dots,x_n)\in M_1$.
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>>>>>>> 2a87fee69dfb1e6fdd6e608f9b4ee957cc3f5a74
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Let us summarize it.
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Let us summarize it.
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@ -447,23 +449,6 @@ We have then proved that $S_d$ is a strong deformation retract of $M_d$.
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If $[x^d_0: \dots: x^d_n]$ is in $(+,\dots,+)$, the retraction is the identity, and therefore both representatives will stay the same and therefore go to the same class.
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If $[x^d_0: \dots: x^d_n]$ is in $(+,\dots,+)$, the retraction is the identity, and therefore both representatives will stay the same and therefore go to the same class.
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For the rest of the regions, we have
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For the rest of the regions, we have
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<<<<<<< HEAD
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\begin{equation}
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\begin{array}{lll}
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\tilde{r}_2([x_0\xi_0:\dots:x_n\xi_n], t)& =& \left[\sqrt[d]{(1-t)x^d_0+t\frac{x^d_0\chi_0}{1-\sum x^d_j(1-\chi_j)}}\xi_0:\dots:\sqrt[d]{(1-t)x^d_n+t\frac{x^d_n\chi_n}{1-\sum x^d_j(1-\chi_j)}}\xi_n\right]
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\end{array}
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\end{equation}
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Then, for the point $\lambda p$ we get
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\begin{equation}
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\begin{array}{lll}
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\tilde{r}_2([\lambda x_0\xi_0:\dots:\lambda x_n\xi_n], t)&=&\left[\sqrt[d]{(1-t)\lambda^d x^d_0+t\frac{\lambda^d x^d_0\chi_0}{1-\sum \lambda^d x^d_j(1-\chi_j)}}\xi_0:\dots:\sqrt[d]{(1-t)\lambda^d x^d_n+t\frac{\lambda^d x^d_n\chi_n}{1-\sum \lambda^d x^d_j(1-\chi_j)}}\xi_n\right]\\
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&=&\left[\sqrt[d]{(1-t)x^d_0+t\frac{x^d_0\chi_0}{1-\sum x^d_j(1-\chi_j)}}\xi_0:\dots:\sqrt[d]{(1-t)x^d_n+t\frac{x^d_n\chi_n}{1-\sum x^d_j(1-\chi_j)}}\xi_n\right]\\
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\end{array}
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\end{equation}
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=======
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\begin{equation*}
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\begin{equation*}
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\tilde{r}_2([x_0\xi_0:\dots:x_n\xi_n], t) =\left[H(x_0,\chi_0)\xi_0:\dots:H(x_n,\chi_n) \xi_n\right]
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\tilde{r}_2([x_0\xi_0:\dots:x_n\xi_n], t) =\left[H(x_0,\chi_0)\xi_0:\dots:H(x_n,\chi_n) \xi_n\right]
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\end{equation*}
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\end{equation*}
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@ -476,7 +461,6 @@ Then, for the point $\lambda p$ we get
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\tilde{r}_2([\lambda x_0\xi_0:\dots:\lambda x_n\xi_n], t)&=\left[H(\lambda x_0, \chi_0)\xi_0:\dots:H(\lambda x_n, \chi_n)\xi_n\right]\\
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\tilde{r}_2([\lambda x_0\xi_0:\dots:\lambda x_n\xi_n], t)&=\left[H(\lambda x_0, \chi_0)\xi_0:\dots:H(\lambda x_n, \chi_n)\xi_n\right]\\
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&=\left[H( x_0, \chi_0)\xi_0:\dots:H(x_n, \chi_n)\xi_n\right].
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&=\left[H( x_0, \chi_0)\xi_0:\dots:H(x_n, \chi_n)\xi_n\right].
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\end{align*}
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\end{align*}
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>>>>>>> 2a87fee69dfb1e6fdd6e608f9b4ee957cc3f5a74
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So we see that $\tilde{r}_2$ also takes both representatives will end to the same point.
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So we see that $\tilde{r}_2$ also takes both representatives will end to the same point.
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\end{proof}
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\end{proof}
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@ -514,17 +498,10 @@ First, we give a detailed description of $\Delta$. We will denote the $0$-simpli
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X & = [v_0,\dots,v_n]
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X & = [v_0,\dots,v_n]
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\end{align*}
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\end{align*}
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The face maps of $X$ and $X^{(j_0,\dots,j_i)}$ are:
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The face maps of $X$ and $X^{(j_0,\dots,j_i)}$ are:
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<<<<<<< HEAD
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\begin{equation}
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\delta^i_k(X^{(j_0,\dots,j_i)}) =[v_{j_0},\dots,\hat{v},\dots,v_{j_i}]
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\end{equation}
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where $\hat{v}$ indicates that we take out the vertix in position $k$, for $k\leq i$.
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=======
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\begin{equation*}
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\begin{equation*}
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\delta^i_k(X^{(j_0,\dots,j_i)}) =[v_{j_0},\dots,\hat{v},\dots,v_{j_i}]
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\delta^i_k(X^{(j_0,\dots,j_i)}) =[v_{j_0},\dots,\hat{v},\dots,v_{j_i}]
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\end{equation*}
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\end{equation*}
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where $\hat{v}$ indicates that we take out the vertex in position $k$, for $k\leq i$.
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where $\hat{v}$ indicates that we take out the vertex in position $k$, for $k\leq i$.
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>>>>>>> 2a87fee69dfb1e6fdd6e608f9b4ee957cc3f5a74
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an the boundary maps are given by:
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an the boundary maps are given by:
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\begin{equation*}
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\begin{equation*}
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\partial^i =\sum (-1)^{k}\delta^i_k
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\partial^i =\sum (-1)^{k}\delta^i_k
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@ -553,20 +530,10 @@ X_{(1,\dots,\xi_i, 1, 1)}\cap\{x_j=1,\,\forall j\neq i\}.
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\]
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\]
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We can remark that $X_{(\xi_0, \dots, \xi_n)}=(\xi_0, \dots, \xi_n)\cdot X_{(1,\dots,1)}$, and therefore that we have a group action of $\mu^{n+1}_d$ over $S_d$.
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We can remark that $X_{(\xi_0, \dots, \xi_n)}=(\xi_0, \dots, \xi_n)\cdot X_{(1,\dots,1)}$, and therefore that we have a group action of $\mu^{n+1}_d$ over $S_d$.
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Let
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Let
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<<<<<<< HEAD
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\begin{equation}
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\begin{array}{rll}
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X^{(j_0,\dots,j_i)}_{(1,\dots,1)} & = & X_{(1, \dots, 1)}\cap\{x_{j_k}\neq0 \forall k=0,\dots i\text{ and }x_{i}=0\text{ for the rest}\}\\
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X^j_{(1,\dots,1)} & = & X_{(1, \dots, 1)}\cap\{x_i=0\forall i\neq j\}\\
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\end{array}
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\end{equation}
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=======
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\begin{align*}
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\begin{align*}
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X^{(j_0,\dots,j_i)}_{(1,\dots,1)} & = X_{(1, \dots, 1)}\cap\{x_{j_k}\neq0,\, \forall k=0,\dots i\text{ and }x_{i}=0\text{ for the rest}\}\\
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X^{(j_0,\dots,j_i)}_{(1,\dots,1)} & = X_{(1, \dots, 1)}\cap\{x_{j_k}\neq0,\, \forall k=0,\dots i\text{ and }x_{i}=0\text{ for the rest}\}\\
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X^j_{(1,\dots,1)} & = X_{(1, \dots, 1)}\cap\{x_i=0,\,\forall i\neq j\}\\
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X^j_{(1,\dots,1)} & = X_{(1, \dots, 1)}\cap\{x_i=0,\,\forall i\neq j\}\\
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\end{align*}
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\end{align*}
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>>>>>>> 2a87fee69dfb1e6fdd6e608f9b4ee957cc3f5a74
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We can describe the chain complexes. They are abelian groups but they are also $R_d$-complexes
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We can describe the chain complexes. They are abelian groups but they are also $R_d$-complexes
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where $R_d$ is the group algebra $\ZZ[\mu_d^{n+1}]$. For the $n$-chains we have
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where $R_d$ is the group algebra $\ZZ[\mu_d^{n+1}]$. For the $n$-chains we have
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\[
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\[
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@ -795,31 +762,34 @@ Lastly, we will have $4$ $2-$simplices, $X_{[1:1:1]}=X_{[-1:-1:-1]}$, $X_{[1:1:-
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The face maps will be obtained by passing to the projective the face maps of $\Delta^d$.
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The face maps will be obtained by passing to the projective the face maps of $\Delta^d$.
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\end{example}
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\end{example}
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\begin{thebibliography}{99}
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\bibliographystyle{amsplain}
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\bibliography{biblio}
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\bibitem{andreotti1959}
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%\begin{thebibliography}{99}
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A. Andreotti and T. Frankel,
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%
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\textit{The Lefschetz theorem on hyperplane sections},
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%\bibitem{andreotti1959}
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Annals of Mathematics,
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%A. Andreotti and T. Frankel,
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Vol. 69, No. 3,
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%\textit{The Lefschetz theorem on hyperplane sections},
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pp. 713--717,
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%Annals of Mathematics,
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1959.
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%Vol. 69, No. 3,
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%pp. 713--717,
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\bibitem{libgober1986}
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%1959.
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A. Libgober,
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%
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\textit{On the homotopy type of the complement to plane algebraic curves},
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%\bibitem{libgober1986}
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J. Reine Angew. Math.,
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%A. Libgober,
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Vol. 367,
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%\textit{On the homotopy type of the complement to plane algebraic curves},
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pp. 103--114,
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%J. Reine Angew. Math.,
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1986.
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%Vol. 367,
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DOI: 10.1515/crll.1986.367.103
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%pp. 103--114,
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%1986.
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\end{thebibliography}
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%DOI: 10.1515/crll.1986.367.103
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%
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%\end{thebibliography}
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\appendix
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\appendix
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\section{SageMath code}
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\section{SageMath code}
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We have written a SageMath function allowing us to define the $\Delta$-complex associated to the complement of a projective Fermat hypersurface of degree $d$ in $\PP^n$.
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We have written a SageMath~\cite{Sagemath} function allowing us to define the $\Delta$-complex associated to the complement of a projective Fermat hypersurface of degree $d$ in $\PP^n$.
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The code for the function is:
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The code for the function is:
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\begin{python}
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\begin{python}
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