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 Post subject: Some Tor and Ext calculations
PostPosted: Sun, 18 Mar 2012 22:55:55 UTC 
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Let k be a field. I'd like to calculate \text{Tor}_{k[x]}(k,k) and \text{Ext}_{k[x]}(k,k)

A good projective (free) resolution of k as a k(x)-module is given by
0 \to \cdots \to k[x] \stackrel{\eta}{\to} k[x] \stackrel{\epsilon} {\to}\to k \to 0

where \epsilon is the augmentation \epsilon(x)=0 and \eta is multiplication by x.

So to calculate Tor we get the sequence
0  \to k[x] \otimes_{k[x]} k \to k[x]\otimes_{k[x]} k \to 0 which is just
0 \to k \to k \to 0

My question is what is the map k \to k? It comes from \eta, but what happens when we use the isomoprhism k[x] \otimes_{k[x]} k \simeq k? (I think the map must be the zero map?)

Similar for \text{Ext}. We end up with \text{Hom}_{k[x]}(k[x],k). Since a homomorphism k[x] \to k is determined by where we send x and it can go anywhere in k, I think that \text{Hom}_{k[x]}(k[x],k) \simeq k, but then I'm not sure what the map k \to k should be.


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 Post subject: Re: Some Tor and Ext calculations
PostPosted: Mon, 19 Mar 2012 00:19:03 UTC 
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The tensor works by modding out by the action of x, so your multiplication by x is now multiplication by 0.

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 Post subject: Re: Some Tor and Ext calculations
PostPosted: Mon, 19 Mar 2012 02:22:37 UTC 
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qwirk wrote:
Let k be a field. I'd like to calculate \text{Tor}_{k[x]}(k,k) and \text{Ext}_{k[x]}(k,k)

A good projective (free) resolution of k as a k(x)-module is given by
0 \to \cdots \to k[x] \stackrel{\eta}{\to} k[x] \stackrel{\epsilon} {\to}\to k \to 0

where \epsilon is the augmentation \epsilon(x)=0 and \eta is multiplication by x.

So to calculate Tor we get the sequence
0  \to k[x] \otimes_{k[x]} k \to k[x]\otimes_{k[x]} k \to 0 which is just
0 \to k \to k \to 0

My question is what is the map k \to k? It comes from \eta, but what happens when we use the isomoprhism k[x] \otimes_{k[x]} k \simeq k? (I think the map must be the zero map?)

Similar for \text{Ext}. We end up with \text{Hom}_{k[x]}(k[x],k). Since a homomorphism k[x] \to k is determined by where we send x and it can go anywhere in k, I think that \text{Hom}_{k[x]}(k[x],k) \simeq k, but then I'm not sure what the map k \to k should be.


Hmm... you haven't seen dual map and the induced map on tensor products when you were doing linear algebra?

Shadow has done the Tor, so I'll do the Ext.

Recall the map \mathop{\mathrm{Hom}}_R(P^j,B)\to\mathop{\mathrm{Hom}}_R(P^{j+1},B) is defined as (P^j\xrightarrow{f}B)\mapsto(P^{j+1}\to P^j\xrightarrow{f}B).

So the map \mathop{\mathrm{Hom}}_{k[x]}(\underbrace{k[x]}_{P^0},k)\xrightarrow{\eta^*}\mathop{\mathrm{Hom}}_{k[x]}(\underbrace{k[x]}_{P^1},k) is defined as taking the map "evaluate at a\in k" and mapping it to "multiply by x then evaluate at a\in k". Of course, the multiplication by x is absorbed in the identification \mathop{\mathrm{Hom}}_{k[x]}(P^j,k)\cong k (j=0,1), so k\to k is the identity map.

Indeed, you wouldn't be asking the question had you written xk[x] instead of k[x] for your P^1 (although you will then have to be careful when you do the Tor functor calculation not to fall into the obvious trap).

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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: Some Tor and Ext calculations
PostPosted: Fri, 30 Mar 2012 09:43:34 UTC 
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Thanks a lot to both of you!


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