Bar resolution: Difference between revisions
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<math>\! \partial_1(h_0, h_1) = (h_1) - (h_0)</math> | <math>\! \partial_1(h_0, h_1) = (h_1) - (h_0)</math> | ||
The source of <math>\partial_1</math> is <math>\mathcal{B}_1(G)</math>, which is a free <math>\mathbb{Z}(G)</math> module on <math>(g)_{g \in G}</math>. The target of <math>\partial_1</math> is <math>\ | The source of <math>\partial_1</math> is <math>\mathcal{B}_1(G)</math>, which is a free <math>\mathbb{Z}(G)</math> module on <math>(g)_{g \in G}</math>. The target of <math>\partial_1</math> is <math>\mathcal{B}_0(G)</math>, which is simply <math>\mathbb{Z}G</math>. | ||
<math>\! \partial_1(g) = g \cdot () - ()</math> | <math>\! \partial_1(g) = g \cdot () - ()</math> | ||
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<math>\! \partial_2(h_0, h_1,h_2) = (h_1,h_2) - (h_0,h_2) + (h_0,h_1)</math> | <math>\! \partial_2(h_0, h_1,h_2) = (h_1,h_2) - (h_0,h_2) + (h_0,h_1)</math> | ||
The source of <math>\partial_2</math> is <math>\mathcal{B}_2(G)</math>, which is a free <math>\mathbb{Z}(G)</math>-module on <math>G \times G</math>. The target of <math>\partial_2</math> is <math>\ | The source of <math>\partial_2</math> is <math>\mathcal{B}_2(G)</math>, which is a free <math>\mathbb{Z}(G)</math>-module on <math>G \times G</math>. The target of <math>\partial_2</math> is <math>\mathcal{B}_1(G)</math>, which is the free <math>\mathbb{Z}G</math>-module on <math>G</math>. | ||
<math>\! \partial_2(g_1 \mid g_2) = g_1 \cdot (g_2) - (g_1g_2) + (g_1)</math> | <math>\! \partial_2(g_1 \mid g_2) = g_1 \cdot (g_2) - (g_1g_2) + (g_1)</math> | ||
Latest revision as of 03:27, 17 July 2010
Definition
Suppose is a group. The bar resolution of is a long exact sequence of -modules:
defined by the following information.
We denote the identity element of by .
The groups
The group is defined as the free abelian group on the set , with acting on it diagonally:
This group can thus be regarded as a -module.
As a -module, has a free generating set identified by by:
The notation with bars is termed the bar notation.
The derivation in the original notation
The derivation in the original notation is given by:
The derivation with the bar notation
The map is defined as follows:
In the more precise summation notation:
Particular cases
In the comma notation, we have:
The source of is , which is a free module on . The target of is , which is simply .
In the comma notation, we have:
The source of is , which is a free -module on . The target of is , which is the free -module on .
In the comma notation, we have:
In the bar notation, we have: