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 Post subject: Fibers
PostPosted: Wed, 14 Dec 2011 14:04:03 UTC 
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I'm reading through the chapters in Algebraic Geometry, Harris, about Blow-ups and Resolving Singularities and he keeps mentioning fibers (for instance, in one example he says
the fiber over that point [the origin in \mathbb{A}^{2}] is a copy of \mathbb{P}^{1} corresponding to the lines through that point), however, he doesn't seem to ever actually define what a fiber is, only something called the fiber product (which I assume is also something I will need).

So if someone could tell me what he means that would be much appreciated (I also noticed he never actually explains what a homogeneous equation is, which I know is a really basic concept (and we have subsequently covered it in lectures so it doesn't matter), but still!)

Thank you very much!

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 Post subject: Re: Fibers
PostPosted: Wed, 14 Dec 2011 14:49:44 UTC 
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peccavi_2006 wrote:
I'm reading through the chapters in Algebraic Geometry, Harris, about Blow-ups and Resolving Singularities and he keeps mentioning fibers (for instance, in one example he says
the fiber over that point [the origin in \mathbb{A}^{2}] is a copy of \mathbb{P}^{1} corresponding to the lines through that point), however, he doesn't seem to ever actually define what a fiber is, only something called the fiber product (which I assume is also something I will need).

So if someone could tell me what he means that would be much appreciated (I also noticed he never actually explains what a homogeneous equation is, which I know is a really basic concept (and we have subsequently covered it in lectures so it doesn't matter), but still!)

Thank you very much!


Suppose p\colon E\to B. The fibre over b\in B is p^{-1}(b) in topology. However, in AG you need a bit more but that requires you to know about schemes (you have \mathop{\mathrm{Spec}}k(b)\hookrightarrow B, and the fibre of p over b is E\times_B\mathop{\mathrm{Spec}}k(b)).

A homogeneous equation is exactly what you think it means --- the total degree of every term appearing in the equation is the same.

So you blow up \mathbb{A}^2 at the origin, getting \mathop{\mathrm{Bl}}_{(0,0)}\mathbb{A}^2\subseteq\mathbb{A}^2\times\mathbb{P}^1\to\mathbb{A}^2, where \mathop{\mathrm{Bl}}_{(0,0)}\mathbb{A}^2=V(\{x_iX_j-x_jX_i\mid 1\leq i,j\leq 2\}), where x_1,x_2 are the coordinates for \mathbb{A}^2 and X_1,X_2 are the coordinates of \mathbb{P}^1. The fibre over any point of \mathbb{A}^2-\{(0,0)\} is still a point, but the fibre over (0,0) is the entire \mathbb{P}^1 since there isn't any condition on the X_1,X_2.

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\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


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 Post subject: Re: Fibers
PostPosted: Wed, 14 Dec 2011 15:30:04 UTC 
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So if I had a point p \in \mathbb{A}^{n} for some arbitrary n > 0, would the map \mathop{\mathrm{Bl}}_{p} \mathbb{A}^{n} \rightarrow \mathbb{A}^{n} be an isomorphism away from p, and at p, would that generalise to the fiber over p being \mathbb{P}^{n-1}?

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 Post subject: Re: Fibers
PostPosted: Wed, 14 Dec 2011 16:14:05 UTC 
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peccavi_2006 wrote:
So if I had a point p \in \mathbb{A}^{n} for some arbitrary n > 0, would the map \mathop{\mathrm{Bl}}_{p} \mathbb{A}^{n} \rightarrow \mathbb{A}^{n} be an isomorphism away from p, and at p, would that generalise to the fiber over p being \mathbb{P}^{n-1}?


If you are blowing up a point, yes. If you blow up along a subvariety you replace the subvariety by its projectivised normal bundle.

_________________
\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


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 Post subject: Re: Fibers
PostPosted: Wed, 14 Dec 2011 17:25:35 UTC 
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Excellent - thanks outermeasure :D

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"It's never crowded along the extra mile"

Graduated, and done with maths forever :P


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