From mboxrd@z Thu Jan 1 00:00:00 1970 X-Msuck: nntp://news.gmane.io/gmane.science.mathematics.categories/915 Path: news.gmane.org!not-for-mail From: Philippe Gaucher Newsgroups: gmane.science.mathematics.categories Subject: computation in CPS Date: Mon, 9 Nov 1998 11:06:13 +0100 (MET) Message-ID: <199811091006.LAA04175@irma.u-strasbg.fr> NNTP-Posting-Host: main.gmane.org Mime-Version: 1.0 Content-Type: text/plain; charset=us-ascii Content-Transfer-Encoding: 8bit X-Trace: ger.gmane.org 1241017327 28290 80.91.229.2 (29 Apr 2009 15:02:07 GMT) X-Complaints-To: usenet@ger.gmane.org NNTP-Posting-Date: Wed, 29 Apr 2009 15:02:07 +0000 (UTC) To: categories@mta.ca Original-X-From: cat-dist Mon Nov 9 16:31:20 1998 Original-Received: (from Majordom@localhost) by mailserv.mta.ca (8.8.8/8.8.8) id PAA00232 for categories-list; Mon, 9 Nov 1998 15:09:35 -0400 (AST) X-Authentication-Warning: mailserv.mta.ca: Majordom set sender to cat-dist@mta.ca using -f Content-MD5: QqGGoKoDrptNPwmdXmVFYw== X-MIME-Autoconverted: from quoted-printable to 8bit by mailserv.mta.ca id GAA18911 Original-Sender: cat-dist@mta.ca Precedence: bulk Original-Lines: 74 Xref: news.gmane.org gmane.science.mathematics.categories:915 Archived-At: Bonjour, Here is a question about composable pasting schemes (CPS). In the omega-category In generated by the n-cube, is it possible to find a kind of "general" formula for the (n-1)-source (target) of the n-morphism corresponding to the interior of In ? I can do mechanical computation in low dimension but I am not able for the moment to imagine a formula for any dimension. In high dimension , computations become very long. For example, using notations of Crans/Johnson/Street etc..., in I2, we have (R(x) means the CPS generated by x, sometimes also denoted by (x)) : s_1(00)=R(-0,0+) (almost the definition in a CPS) and t_0(-0)=s_0(0+)=-+ => s_1(00)=R(-0) o_0 R(0+) (1) because the union is the composition in the framework of CPS. And t_1(00)=R(+0,0-)=R(0-) o_o R(+0) (2). Obvious with a picture. In I3, we have : s_2(000)=R(-00,0+0,00-)=R(-00,0++,-0-,0+0,00-,++0) t_0(-00)=s_0(0++) => R(-00,0++) = R(-00) o_0 R(0++) t_0(-0-)=s_0(0+0) => R(-0-,0+0) = R(-0-) o_0 R(0+0) t_0(00-)=s_0(++0) => R(00-,++0) = R(00-) o_0 R(++0) and t_1(R(-00) o_0 R(0++)) = t_1(-00) o_0 R(0++) (axiom of omegaCat) = (-0-) o_0 (-+0) o_0 (0++) with (2) s_1(R(-0-) o_0 R(0+0)) = R(-0-) o_0 s_1(0+0) (axiom of omegaCat) = (-0-) o_0 (-+0) o_0 (0++) with (1) => R(-00,0++,-0-,0+0) = R(-00,0++) o_1 R(-0-,0+0) and in the same way, we preove that t_1(R(-0-,0+0))=s_1(R(00-,++0)) => s_2(000) =((-00) o_0 (0++)) o_1 ((-0-) o_0 (0+0)) o_1 ((00-) o_0 (++0)) For t_2(000), read the above formula from the right to the left and replace - by +. Almost obvious with a picture. For I4 now : I have found a formula for s_3(0000)... A little bit long and not interesting. For I5 : Too long. More generally, the question is : for a CPS, is there a way to compute the source and target of a R({x}) using only compositions of elements like R({y}) ? Thanks in advance for your help. pg.