-------- Original Message -------- Subject: Schreier theory discussion Date: Tue, 22 Nov 2005 18:01:42 +0100 (CET) From: Johannes Huebschmann <Johannes.Huebschmann@math.univ-lille1.fr> To: ronnie@ll319dg.fsnet.co.uk, baez@math.ucr.edu, jds@math.upenn.edu, derek@math.ucr.edu CC: Johannes Huebschmann <Johannes.Huebschmann@math.univ-lille1.fr> Dear Friends and Colleagues A few addenda to the Schreier theory discussion etc. which you might find interesting. (I am reacting to a message I received via J. Stasheff.) 1) As pointed out by R. Brwon, an approach to non-abelian cohomology may be phrased in terms of crossed modules. There is a notion more general than crossed modules, that of "crossed pair" which I introduced in the paper Group extensions, crossed pairs, and an eight term exact sequence, J. reine angew. Math. 321 (1981), 150--172. Crossed pairs may be used, for example, to explore group extensions, in particular, to examine differentials in the spectral sequence of a group extension. I worked this out in the paper Automorphisms of group extensions and differentials in the Lyndon--Hochschild--Serre spectral sequence, J. of Algebra 72 (1981), 296--334. I discovered later that the idea of crossed pair was in the literature before, under the name "pseudo module" in the 50's. Crossed pairs arise under other circumstances as well, for example in the Galois theory of Azumaya algebras. I have known this all my scientific life but never found the time to write it up properly. 2) I have worked out a rigorous approach to lattice gauge theory in the paper Extended moduli spaces, the Kan construction, and lattice gauge theory Topology 38 (1999), 555--596. In this paper, I discretize a space of based gauge equivalence classes of connections in terms of a combinatorial structure, and the resulting object is a COSIMPLICIAL space. The geometric realization of this space is G-equivariantly weakly homotopy equivalent to the space of based gauge equivalence classes of connections, where G refers to the structure group of the corresponding principal bundle. On such a space, for example, path integrals are well defined. As an illustration I worked out a calculation of the Chern-Simons invariant for lens spaces. The calculation involves identities among relations, a notion which arises in the structure theory of crossed modules. Best regards Johannes HUEBSCHMANN Johannes Professeur de Mathematiques USTL, UFR de Mathematiques UMR 8524 Laboratoire Paul Painleve F-59 655 Villeneuve d'Ascq Cedex France http://math.univ-lille1.fr/~huebschm TEL. (33) 3 20 43 41 97 (33) 3 20 43 42 33 (secretariat) (33) 3 20 43 48 50 (secretariat) Fax (33) 3 20 43 43 02 e-mail Johannes.Huebschmann@math.univ-lille1.fr --------------030708090300040304040700 Content-Type: text/html; charset=us-ascii Content-Transfer-Encoding: 7bit <!DOCTYPE html PUBLIC "-//W3C//DTD HTML 4.01 Transitional//EN"> <html> <head> <meta content="text/html;charset=ISO-8859-1" http-equiv="Content-Type"> <title></title> </head> <body bgcolor="#ffffff" text="#000000"> <br> <br> -------- Original Message -------- <table border="0" cellpadding="0" cellspacing="0"> <tbody> <tr> <th align="right" nowrap="nowrap" valign="baseline">Subject: </th> <td>Schreier theory discussion</td> </tr> <tr> <th align="right" nowrap="nowrap" valign="baseline">Date: </th> <td>Tue, 22 Nov 2005 18:01:42 +0100 (CET)</td> </tr> <tr> <th align="right" nowrap="nowrap" valign="baseline">From: </th> <td>Johannes Huebschmann <a class="moz-txt-link-rfc2396E" href="mailto:Johannes.Huebschmann@math.univ-lille1.fr"><Johannes.Huebschmann@math.univ-lille1.fr></a></td> </tr> <tr> <th align="right" nowrap="nowrap" valign="baseline">To: </th> <td><a class="moz-txt-link-abbreviated" href="mailto:ronnie@ll319dg.fsnet.co.uk">ronnie@ll319dg.fsnet.co.uk</a>, <a class="moz-txt-link-abbreviated" href="mailto:baez@math.ucr.edu">baez@math.ucr.edu</a>, <a class="moz-txt-link-abbreviated" href="mailto:jds@math.upenn.edu">jds@math.upenn.edu</a>, <a class="moz-txt-link-abbreviated" href="mailto:derek@math.ucr.edu">derek@math.ucr.edu</a></td> </tr> <tr> <th align="right" nowrap="nowrap" valign="baseline">CC: </th> <td>Johannes Huebschmann <a class="moz-txt-link-rfc2396E" href="mailto:Johannes.Huebschmann@math.univ-lille1.fr"><Johannes.Huebschmann@math.univ-lille1.fr></a></td> </tr> </tbody> </table> <br> <br> <pre>Dear Friends and Colleagues A few addenda to the Schreier theory discussion etc. which you might find interesting. (I am reacting to a message I received via J. Stasheff.) 1) As pointed out by R. Brwon, an approach to non-abelian cohomology may be phrased in terms of crossed modules. There is a notion more general than crossed modules, that of "crossed pair" which I introduced in the paper Group extensions, crossed pairs, and an eight term exact sequence, J. reine angew. Math. 321 (1981), 150--172. Crossed pairs may be used, for example, to explore group extensions, in particular, to examine differentials in the spectral sequence of a group extension. I worked this out in the paper Automorphisms of group extensions and differentials in the Lyndon--Hochschild--Serre spectral sequence, J. of Algebra 72 (1981), 296--334. I discovered later that the idea of crossed pair was in the literature before, under the name "pseudo module" in the 50's. Crossed pairs arise under other circumstances as well, for example in the Galois theory of Azumaya algebras. I have known this all my scientific life but never found the time to write it up properly. 2) I have worked out a rigorous approach to lattice gauge theory in the paper Extended moduli spaces, the Kan construction, and lattice gauge theory Topology 38 (1999), 555--596. In this paper, I discretize a space of based gauge equivalence classes of connections in terms of a combinatorial structure, and the resulting object is a COSIMPLICIAL space. The geometric realization of this space is G-equivariantly weakly homotopy equivalent to the space of based gauge equivalence classes of connections, where G refers to the structure group of the corresponding principal bundle. On such a space, for example, path integrals are well defined. As an illustration I worked out a calculation of the Chern-Simons invariant for lens spaces. The calculation involves identities among relations, a notion which arises in the structure theory of crossed modules. Best regards Johannes HUEBSCHMANN Johannes Professeur de Mathematiques USTL, UFR de Mathematiques UMR 8524 Laboratoire Paul Painleve F-59 655 Villeneuve d'Ascq Cedex France <a class="moz-txt-link-freetext" href="http://math.univ-lille1.fr/~huebschm">http://math.univ-lille1.fr/~huebschm</a> TEL. (33) 3 20 43 41 97 (33) 3 20 43 42 33 (secretariat) (33) 3 20 43 48 50 (secretariat) Fax (33) 3 20 43 43 02 e-mail <a class="moz-txt-link-abbreviated" href="mailto:Johannes.Huebschmann@math.univ-lille1.fr">Johannes.Huebschmann@math.univ-lille1.fr</a> </pre> </body> </html> --------------030708090300040304040700--