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I had also tried, shortly after his death, to pay tribute to his great mind in another way by showing in a short paper arXiv:1901.10761 \u0026quot;On an idea of Michael Atiyah\u0026quot; the pertinence of his recent idea on iteration of the exterior power in the representation rings of finite groups of odd order. The great surprise there was to find "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/2482145272230695540\/comments\/default\/378197006671569819"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/2482145272230695540\/comments\/default\/378197006671569819"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2019\/10\/sir-michael-atiyah-knight-mathematician.html?showComment=1570874469246#c378197006671569819","title":""}],"author":[{"name":{"$t":"AC"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/11268275942327566512"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2019\/10\/sir-michael-atiyah-knight-mathematician.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-2482145272230695540","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/2482145272230695540","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-956390664"},{"name":"blogger.displayTime","value":"October 12, 2019 at 10:01 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-6037503184751849962"},"published":{"$t":"2017-04-14T15:09:47.602+00:00"},"updated":{"$t":"2017-04-14T15:09:47.602+00:00"},"title":{"type":"text","$t":"Thanks very much Alain for your post  about David...."},"summary":{"type":"text","$t":"Thanks very much Alain for your post  about David. He was a wonderful mathematician, a  very kind person,  and also a regular contributor to this blog who  generously shared his insights on various topics in number theory here. It is a big loss and we shall all miss him dearly. Rest in peace David!"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3605038603833189856\/comments\/default\/6037503184751849962"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3605038603833189856\/comments\/default\/6037503184751849962"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2017\/04\/david.html?showComment=1492182587602#c6037503184751849962","title":""}],"author":[{"name":{"$t":"Masoud Khalkhali"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03769072750559219167"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2017\/04\/david.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3605038603833189856","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3605038603833189856","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-605110258"},{"name":"blogger.displayTime","value":"April 14, 2017 at 3:09 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-3317233832464235678"},"published":{"$t":"2015-07-19T20:08:24.684+00:00"},"updated":{"$t":"2015-07-19T20:08:24.684+00:00"},"title":{"type":"text","$t":"Merci Alain, c\u0026#39;est un très beau texte."},"summary":{"type":"text","$t":"Merci Alain, c\u0026#39;est un très beau texte."},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/4236613683236361490\/comments\/default\/3317233832464235678"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/4236613683236361490\/comments\/default\/3317233832464235678"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/07\/uffe-haagerup.html?showComment=1437336504684#c3317233832464235678","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/02536056873037002420"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/07\/uffe-haagerup.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-4236613683236361490","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/4236613683236361490","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1116013664"},{"name":"blogger.displayTime","value":"July 19, 2015 at 8:08 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-6766268099161399878"},"published":{"$t":"2015-02-23T10:46:18.040+00:00"},"updated":{"$t":"2015-02-23T10:46:18.040+00:00"},"title":{"type":"text","$t":"Here is the bibliography: arxiv: 1412.4776 and 130..."},"summary":{"type":"text","$t":"Here is the bibliography: arxiv: 1412.4776 and 1306.4468"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6165547310508665931\/comments\/default\/6766268099161399878"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6165547310508665931\/comments\/default\/6766268099161399878"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/01\/quanta-of-geometry.html?showComment=1424688378040#c6766268099161399878","title":""}],"author":[{"name":{"$t":"cb"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03349828290008437401"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/01\/quanta-of-geometry.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6165547310508665931","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6165547310508665931","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1151436177"},{"name":"blogger.displayTime","value":"February 23, 2015 at 10:46 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-4998604273665734821"},"published":{"$t":"2015-02-23T10:43:32.844+00:00"},"updated":{"$t":"2015-02-23T10:43:32.844+00:00"},"title":{"type":"text","$t":"If the spectral noncommutative geometric program c..."},"summary":{"type":"text","$t":"If the spectral noncommutative geometric program could help astrophysicists and cosmologists to put their dark matter, dark energy and inflaton models on a unified coherent basis that would be fantastic opportunity. Meanwhile one can note that the mimetic dark matter hypothesis has already met some echo in the theoretical physics community. On the more phenomenological side of the possible "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6165547310508665931\/comments\/default\/4998604273665734821"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6165547310508665931\/comments\/default\/4998604273665734821"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/01\/quanta-of-geometry.html?showComment=1424688212844#c4998604273665734821","title":""}],"author":[{"name":{"$t":"cb"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03349828290008437401"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/01\/quanta-of-geometry.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6165547310508665931","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6165547310508665931","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1151436177"},{"name":"blogger.displayTime","value":"February 23, 2015 at 10:43 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-4172858524674262114"},"published":{"$t":"2015-01-02T20:18:45.591+00:00"},"updated":{"$t":"2015-01-02T20:18:45.591+00:00"},"title":{"type":"text","$t":"Very nice! Thank you Alain!! "},"summary":{"type":"text","$t":"Very nice! Thank you Alain!! "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6165547310508665931\/comments\/default\/4172858524674262114"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6165547310508665931\/comments\/default\/4172858524674262114"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/01\/quanta-of-geometry.html?showComment=1420229925591#c4172858524674262114","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/01874443969277514500"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2015\/01\/quanta-of-geometry.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6165547310508665931","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6165547310508665931","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-966421006"},{"name":"blogger.displayTime","value":"January 2, 2015 at 8:18 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-627252076409906311"},"published":{"$t":"2014-12-23T14:58:04.152+00:00"},"updated":{"$t":"2014-12-23T14:58:04.152+00:00"},"title":{"type":"text","$t":"In addition to a higher analog of the Hamiltonian ..."},"summary":{"type":"text","$t":"In addition to a higher analog of the Hamiltonian H, I also expect this new H to satisfy some form of the Schrodinger equation and some form of the Heisenberg equation. Perhaps could also find higher analogs for these two fundamental equations. Finally, there should also be a higher analog for each of the two commutation relations involving the Hamiltonian H (one uses [H,p] and the other has [H,q"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/627252076409906311"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/627252076409906311"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1419346684152#c627252076409906311","title":""}],"author":[{"name":{"$t":"Patrick Tam"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/12416782207086732341"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1647460199"},{"name":"blogger.displayTime","value":"December 23, 2014 at 2:58 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-3792409789976477300"},"published":{"$t":"2014-12-22T12:00:15.804+00:00"},"updated":{"$t":"2014-12-22T12:00:15.804+00:00"},"title":{"type":"text","$t":"So you have a higher analogues of position operato..."},"summary":{"type":"text","$t":"So you have a higher analogues of position operator, momentum operator, and canonical commutation relations. It seems to me that there should be a higher analogue of the Hamiltonian operator as well. Is the spectral action related to this higher Hamiltonian?"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/3792409789976477300"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/3792409789976477300"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1419249615804#c3792409789976477300","title":""}],"author":[{"name":{"$t":"Patrick Tam"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/12416782207086732341"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1647460199"},{"name":"blogger.displayTime","value":"December 22, 2014 at 12:00 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-3541294225826191344"},"published":{"$t":"2014-11-13T21:08:46.607+00:00"},"updated":{"$t":"2014-11-13T21:08:46.607+00:00"},"title":{"type":"text","$t":"It\u0026#39;s Uf\u0026#39;(U) not U*f\u0026#39;(U), sorry for the..."},"summary":{"type":"text","$t":"It\u0026#39;s Uf\u0026#39;(U) not U*f\u0026#39;(U), sorry for the typo."},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/3541294225826191344"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/3541294225826191344"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1415912926607#c3541294225826191344","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/14399939280602212683"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1443189012"},{"name":"blogger.displayTime","value":"November 13, 2014 at 9:08 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-4555305166121664694"},"published":{"$t":"2014-11-13T14:53:22.579+00:00"},"updated":{"$t":"2014-11-13T14:53:22.579+00:00"},"title":{"type":"text","$t":"Thank you for little exercise. I have done it and ..."},"summary":{"type":"text","$t":"Thank you for little exercise. I have done it and everything is as you say, so we have D=a+(1\/i)d\/dt densely defined on L^2(S^1) and U=mult by e^{it}, and [D,f(U)]=U*f\u0026#39;(U).\u003Cbr \/\u003E\u003Cbr \/\u003ENow if I understand correctly you are going to \u0026quot;slash\u0026quot; everyone and arrive at D slashed and Y. (By the way I like the fact that you need both Clifford algebras C_+ and C_-. Seems very natural not to "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/4555305166121664694"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/4555305166121664694"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1415890402579#c4555305166121664694","title":""}],"author":[{"name":{"$t":"Fabien Besnard"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/00975996576182366143"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1482919975"},{"name":"blogger.displayTime","value":"November 13, 2014 at 2:53 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-5338816572302581414"},"published":{"$t":"2014-11-13T13:07:14.155+00:00"},"updated":{"$t":"2014-11-13T13:07:14.155+00:00"},"title":{"type":"text","$t":"That was a long overdue : to see quaternions clear..."},"summary":{"type":"text","$t":"That was a long overdue : to see quaternions clearly entering on the stage of the quantum theater thanks to this postulated degree 4 analogue of the Heisenberg relation after past hints from the electroweak symmetry breaking (I think about the 1982 quaternionic Weinberg-Salam Theory of Katsusada Morita).\u003Cbr \/\u003ENow that the standard model Higgs boson is well established at the attoscale, I wish "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/5338816572302581414"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/5338816572302581414"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1415884034155#c5338816572302581414","title":""}],"author":[{"name":{"$t":"cb"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03349828290008437401"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1151436177"},{"name":"blogger.displayTime","value":"November 13, 2014 at 1:07 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-4442586193341533661"},"published":{"$t":"2014-11-12T17:59:49.235+00:00"},"updated":{"$t":"2014-11-12T17:59:49.235+00:00"},"title":{"type":"text","$t":"Dear Fabien\n\nI guess that a good way to see in whi..."},"summary":{"type":"text","$t":"Dear Fabien\u003Cbr \/\u003E\u003Cbr \/\u003EI guess that a good way to see in which way the equation is analogous to the canonical commutation relation is to start with the following toy case: it is the one dimensional case, one looks for irreducible representations of the following relation \u003Cbr \/\u003E     U^*[D,U]=1\u003Cbr \/\u003Ewhere U is a unitary operator in Hilbert space and D is self-adjoint. The exercice is to classify "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/4442586193341533661"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/4442586193341533661"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1415815189235#c4442586193341533661","title":""}],"author":[{"name":{"$t":"AC"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/11268275942327566512"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-956390664"},{"name":"blogger.displayTime","value":"November 12, 2014 at 5:59 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-1053842215914641684"},"published":{"$t":"2014-11-12T13:33:59.366+00:00"},"updated":{"$t":"2014-11-12T13:33:59.366+00:00"},"title":{"type":"text","$t":"I had read your paper already. It left me somewhat..."},"summary":{"type":"text","$t":"I had read your paper already. It left me somewhat puzzled so I thank you for giving additionnal insight here. That so much beautiful mathematics comes out of a single equation is certainly remarkable.\u003Cbr \/\u003EHowever, I still do not understand why 1) one should take Z for the conjugate momentum of D, 2) in which way is the 2-sided equation analogous to the canonical commutation relation.\u003Cbr \/\u003EIt "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/1053842215914641684"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/3358862930369800100\/comments\/default\/1053842215914641684"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html?showComment=1415799239366#c1053842215914641684","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/14399939280602212683"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2014\/11\/particles-in-quantum-gravity.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-3358862930369800100","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/3358862930369800100","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1443189012"},{"name":"blogger.displayTime","value":"November 12, 2014 at 1:33 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-5764787476244093081"},"published":{"$t":"2013-11-22T02:51:46.424+00:00"},"updated":{"$t":"2013-11-22T02:51:46.424+00:00"},"title":{"type":"text","$t":"Hi. Just saw this. Thanks! Matt will be here in a ..."},"summary":{"type":"text","$t":"Hi. Just saw this. Thanks! Matt will be here in a couple of weeks so I can ask him more."},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6968793899696405243\/comments\/default\/5764787476244093081"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6968793899696405243\/comments\/default\/5764787476244093081"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/04\/wronski-vandermonde-and-moore_19.html?showComment=1385088706424#c5764787476244093081","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/17587441329676384897"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/04\/wronski-vandermonde-and-moore_19.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6968793899696405243","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6968793899696405243","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1628758237"},{"name":"blogger.displayTime","value":"November 22, 2013 at 2:51 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-2516234849711807788"},"published":{"$t":"2013-08-25T08:42:22.828+00:00"},"updated":{"$t":"2013-08-25T08:42:22.828+00:00"},"title":{"type":"text","$t":"Wonderful initiative! Let\u0026#39;s hope that with suc..."},"summary":{"type":"text","$t":"Wonderful initiative! Let\u0026#39;s hope that with such a tool more physicists get involved in checking by themselves if noncommutativity has diamonds in its pockets for physics behind the Standard Model  \/ in understanding if a noncommutative grand algebra  could not be more efficient than a supersymmetric group to find new particles  beyond the electroweak scale ..."},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6628586679337708619\/comments\/default\/2516234849711807788"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6628586679337708619\/comments\/default\/2516234849711807788"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/08\/website-noncommutative-geometry-and.html?showComment=1377420142828#c2516234849711807788","title":""}],"author":[{"name":{"$t":"cb"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03349828290008437401"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/08\/website-noncommutative-geometry-and.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6628586679337708619","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6628586679337708619","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1151436177"},{"name":"blogger.displayTime","value":"August 25, 2013 at 8:42 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-5833691205953101370"},"published":{"$t":"2013-07-11T21:04:18.648+00:00"},"updated":{"$t":"2013-07-11T21:04:18.648+00:00"},"title":{"type":"text","$t":"@Eric, here it is:\nhttp:\/\/www.dailymotion.com\/vide..."},"summary":{"type":"text","$t":"@Eric, here it is:\u003Cbr \/\u003Ehttp:\/\/www.dailymotion.com\/video\/xuiyfo_the-music-of-shapes_tech#.Ud8cCDu-2So"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/1941132621896146173\/comments\/default\/5833691205953101370"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/1941132621896146173\/comments\/default\/5833691205953101370"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/10\/the-music-of-spheres.html?showComment=1373576658648#c5833691205953101370","title":""}],"author":[{"name":{"$t":"nico"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/08672913336008027317"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/10\/the-music-of-spheres.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-1941132621896146173","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/1941132621896146173","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-125159881"},{"name":"blogger.displayTime","value":"July 11, 2013 at 9:04 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-3204561365891163213"},"published":{"$t":"2013-07-11T20:18:45.735+00:00"},"updated":{"$t":"2013-07-11T20:18:45.735+00:00"},"title":{"type":"text","$t":"Thanks David for this post!"},"summary":{"type":"text","$t":"Thanks David for this post!"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/3204561365891163213"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/3204561365891163213"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html?showComment=1373573925735#c3204561365891163213","title":""}],"author":[{"name":{"$t":"Masoud Khalkhali"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03769072750559219167"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6673466554412267563","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6673466554412267563","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-605110258"},{"name":"blogger.displayTime","value":"July 11, 2013 at 8:18 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-2322224313920461267"},"published":{"$t":"2013-07-11T16:36:18.272+00:00"},"updated":{"$t":"2013-07-11T16:36:18.272+00:00"},"title":{"type":"text","$t":"From Rudy: \nThe series \\sum_{a \\in A_+}a^{-1}C_a(z..."},"summary":{"type":"text","$t":"From Rudy: \u003Cbr \/\u003EThe series \\sum_{a \\in A_+}a^{-1}C_a(z) has a ``natural\u0026#39;\u0026#39; domain of convergence given by the image T of (-\\theta)^{1\/(q-1)}K_\\infty under\u003Cbr \/\u003Ethe Carlitz exponential. (NB. This is the domain of convergence considered by Anderson in his \u003Ci\u003Elog-algebraicity\u003C\/i\u003E paper.) The compact space T is the closure of all Carlitz torsion in \u003Cbr \/\u003E\u003Cbr \/\u003EK_\\infty((-\\theta)^{1\/(q-1)})$,\u003C"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/2322224313920461267"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/2322224313920461267"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html?showComment=1373560578272#c2322224313920461267","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/01874443969277514500"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6673466554412267563","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6673466554412267563","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-966421006"},{"name":"blogger.displayTime","value":"July 11, 2013 at 4:36 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-5236026989034241316"},"published":{"$t":"2013-07-11T16:22:41.748+00:00"},"updated":{"$t":"2013-07-11T16:22:41.748+00:00"},"title":{"type":"text","$t":""},"summary":{"type":"text","$t":"This comment has been removed by the author."},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/5236026989034241316"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/5236026989034241316"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html?showComment=1373559761748#c5236026989034241316","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/01874443969277514500"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6673466554412267563","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6673466554412267563","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.contentRemoved","value":"true"},{"name":"blogger.itemClass","value":"pid-966421006"},{"name":"blogger.displayTime","value":"July 11, 2013 at 4:22 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-2480635296370466949"},"published":{"$t":"2013-07-11T15:54:12.581+00:00"},"updated":{"$t":"2013-07-11T15:54:12.581+00:00"},"title":{"type":"text","$t":"The series $\\sum_{a \\in A_+}a^{-1}C_a(z)$ has a ``..."},"summary":{"type":"text","$t":"The series $\\sum_{a \\in A_+}a^{-1}C_a(z)$ has a ``natural\u0026#39;\u0026#39; domain of convergence given by the image $T$ of $(-\\theta)^{1\/(q-1)}K_\\infty$ under the Carlitz exponential. (NB. This is the domain of convergence considered by Anderson in his \u003Ci\u003Elog-algebraicity\u003C\/i\u003E paper.) The compact space $T$ is the closure of all Carlitz torsion in $K_\\infty((-\\theta)^{1\/(q-1)})$, and as such it is "},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/2480635296370466949"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/6673466554412267563\/comments\/default\/2480635296370466949"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html?showComment=1373558052581#c2480635296370466949","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/08375844566090841603"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2013\/07\/a-expansions.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-6673466554412267563","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/6673466554412267563","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-78924266"},{"name":"blogger.displayTime","value":"July 11, 2013 at 3:54 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-94070430942233519"},"published":{"$t":"2013-05-10T23:05:01.377+00:00"},"updated":{"$t":"2013-05-10T23:05:01.377+00:00"},"title":{"type":"text","$t":"The link to the video no longer works!  I would lo..."},"summary":{"type":"text","$t":"The link to the video no longer works!  I would love to see this lecture."},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/1941132621896146173\/comments\/default\/94070430942233519"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/1941132621896146173\/comments\/default\/94070430942233519"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/10\/the-music-of-spheres.html?showComment=1368227101377#c94070430942233519","title":""}],"author":[{"name":{"$t":"Anonymous"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/18161833581888531908"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/10\/the-music-of-spheres.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-1941132621896146173","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/1941132621896146173","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1848478373"},{"name":"blogger.displayTime","value":"May 10, 2013 at 11:05 PM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-2908464238382518407"},"published":{"$t":"2013-04-17T10:24:49.340+00:00"},"updated":{"$t":"2013-04-17T10:24:49.340+00:00"},"title":{"type":"text","$t":"Thank you all for all the teaching in this Noncomm..."},"summary":{"type":"text","$t":"Thank you all for all the teaching in this Noncommutative geometry because i have learnt so well from it,Wishing that it will continue in this LINK..http\/\/www.unn.edu.ng. Thanks"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/2132605122112123023\/comments\/default\/2908464238382518407"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/2132605122112123023\/comments\/default\/2908464238382518407"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/07\/operatorscalar-fusion-in-finite.html?showComment=1366194289340#c2908464238382518407","title":""}],"author":[{"name":{"$t":"Mbanugo Ginika"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/07899503100421629527"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/07\/operatorscalar-fusion-in-finite.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-2132605122112123023","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/2132605122112123023","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1459653844"},{"name":"blogger.displayTime","value":"April 17, 2013 at 10:24 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-74043698161956128"},"published":{"$t":"2013-04-17T10:21:41.647+00:00"},"updated":{"$t":"2013-04-17T10:21:41.647+00:00"},"title":{"type":"text","$t":"Thank you all well for all the teachings so far th..."},"summary":{"type":"text","$t":"Thank you all well for all the teachings so far that i have learnt in Noncumulative geometry.Wishing that this teaching will continue in this LINK...http\/\/www.unn.edu.ng"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/2132605122112123023\/comments\/default\/74043698161956128"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/2132605122112123023\/comments\/default\/74043698161956128"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/07\/operatorscalar-fusion-in-finite.html?showComment=1366194101647#c74043698161956128","title":""}],"author":[{"name":{"$t":"Mbanugo Ginika"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/07899503100421629527"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/07\/operatorscalar-fusion-in-finite.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-2132605122112123023","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/2132605122112123023","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1459653844"},{"name":"blogger.displayTime","value":"April 17, 2013 at 10:21 AM"}]},{"id":{"$t":"tag:blogger.com,1999:blog-6912603287930240451.post-3556659374355661765"},"published":{"$t":"2013-03-17T19:50:11.039+00:00"},"updated":{"$t":"2013-03-17T19:50:11.039+00:00"},"title":{"type":"text","$t":"Could it be that the 125 GeV Higgs boson is the be..."},"summary":{"type":"text","$t":"Could it be that the 125 GeV Higgs boson is the best spectral herald from the (almost commutative?) atto-space to help us to understand the past and faraway cosmic music of Spheres which should be released soon by Planck space telescope and alpha magnetic spectrometer AMS02 ? Whatever, best wishes to the future phenomenological spectral model predictions and wait and see ... for a first signature"},"link":[{"rel":"edit","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/1941132621896146173\/comments\/default\/3556659374355661765"},{"rel":"self","type":"application/atom+xml","href":"http:\/\/www.blogger.com\/feeds\/6912603287930240451\/1941132621896146173\/comments\/default\/3556659374355661765"},{"rel":"alternate","type":"text/html","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/10\/the-music-of-spheres.html?showComment=1363549811039#c3556659374355661765","title":""}],"author":[{"name":{"$t":"cb"},"uri":{"$t":"https:\/\/www.blogger.com\/profile\/03349828290008437401"},"email":{"$t":"noreply@blogger.com"},"gd$image":{"rel":"http://schemas.google.com/g/2005#thumbnail","width":"16","height":"16","src":"https:\/\/img1.blogblog.com\/img\/b16-rounded.gif"}}],"thr$in-reply-to":{"xmlns$thr":"http://purl.org/syndication/thread/1.0","href":"http:\/\/noncommutativegeometry.blogspot.com\/2012\/10\/the-music-of-spheres.html","ref":"tag:blogger.com,1999:blog-6912603287930240451.post-1941132621896146173","source":"http://www.blogger.com/feeds/6912603287930240451/posts/default/1941132621896146173","type":"text/html"},"gd$extendedProperty":[{"name":"blogger.itemClass","value":"pid-1151436177"},{"name":"blogger.displayTime","value":"March 17, 2013 at 7:50 PM"}]}]}});