{"id":170,"date":"2009-10-15T07:56:07","date_gmt":"2009-10-15T12:56:07","guid":{"rendered":"http:\/\/blog.richmond.edu\/physicsbunn\/2009\/10\/15\/is-the-lhc-doomed-by-signals-from-the-future\/"},"modified":"2009-10-15T07:56:07","modified_gmt":"2009-10-15T12:56:07","slug":"is-the-lhc-doomed-by-signals-from-the-future","status":"publish","type":"post","link":"https:\/\/blog.richmond.edu\/physicsbunn\/2009\/10\/15\/is-the-lhc-doomed-by-signals-from-the-future\/","title":{"rendered":"Is the LHC doomed by signals from the future?"},"content":{"rendered":"<p>I guess <a href=\"http:\/\/www.nytimes.com\/2009\/10\/13\/science\/space\/13lhc.html?_r=1&amp;em=&amp;pagewanted=all\">this piece in the NY Times<\/a> has been getting some attention lately.\u00a0 It&#8217;s about a c<a href=\"http:\/\/arxiv.org\/abs\/0910.0359\">razy theory<\/a> by Nelson and Ninomiya (NN for short) in which the laws of physics don&#8217;t &#8220;want&#8221; the Higgs boson to be created.\u00a0 According to this theory, states of the Universe in which lots of Higgses are created are automatically disfavored: if there are multiple different ways something can turn out, and one involves creating Higgses, then it&#8217;ll turn out some other way.\u00a0 Since the Large Hadron Collider is going to attempt to find the Higgs, this theory predicts that things will happen to it so that it fails to do so.<\/p>\n<p>Sean Carroll has a nice <a href=\"http:\/\/blogs.discovermagazine.com\/cosmicvariance\/2009\/10\/14\/spooky-signals-from-the-future-telling-us-to-cancel-the-lhc\/\">exegesis<\/a> of this.\u00a0 I urge you to go read it if you&#8217;re curious about this business.\u00a0 There&#8217;s a bit in the middle that explains the theory in a bit more detail than you might like (unless of course you like that sort of thing).\u00a0 If you find yourself getting bogged down when he talks about &#8220;imaginary action&#8221; and the like, just skip ahead a few paragraphs to about here:<\/p>\n<blockquote><p>So this model makes a strong prediction: we&#39;re not going to be producing any Higgs bosons. Not because the ordinary dynamical equations of physics prevent it (e.g., because the Higgs is just too massive), but because the specific trajectory on which the universe finds itself is one in which no Higgses are made.<\/p>\n<p>That, of course, runs into the problem that we have every intention of making Higgs bosons, for example at the LHC. Aha, say NN, but notice that we haven&#39;t yet! The Superconducting Supercollider, which could have found the Higgs long ago, was canceled by Congress. And in their <a href=\"http:\/\/arxiv.org\/abs\/0707.1919\">December 2007 paper<\/a> \u20ac\u201d before the LHC tried to turn on \u20ac\u201d they very explicitly say that a &quot;natural&quot; accident will come along and break the LHC if we try to turn it on. Well, we know how <a href=\"http:\/\/blogs.discovermagazine.com\/cosmicvariance\/2008\/09\/19\/lhc-first-magnet-failure\/\">that turned out<\/a>.<\/p><\/blockquote>\n<p>I think Sean&#8217;s overall point of view is pretty much right:<\/p>\n<blockquote><p>At the end of the day: this theory is crazy. There&#39;s no real reason to believe in an imaginary component to the action with dramatic apparently-nonlocal effects, and even if there were, the specific choice of action contemplated by NN seems rather contrived. But I&#39;m happy to argue that it&#39;s the good kind of crazy. The authors start with a speculative but well-defined idea, and carry it through to its logical conclusions. That&#39;s what scientists are supposed to do. I think that the Bayesian prior probability on their model being right is less than one in a million, so I&#39;m not going to take its predictions very seriously. But the process by which they work those predictions out has been perfectly scientific.<\/p><\/blockquote>\n<p>Because I&#8217;m obsessed with Bayesian probabilities, I want to pick up a bit on that aspect of things.\u00a0 NN propose an experiment to test their theory.\u00a0 We take a million-card deck of cards, in which one says &#8220;Don&#8217;t turn on the LHC.&#8221;\u00a0 We pick a card at random from the deck, and if we get that one card, we junk the LHC.\u00a0 Otherwise, we go ahead and search for the Higgs as planned.\u00a0 According to NN, if their theory is right, that card will come up because the Universe will want to &#8220;protect itself&#8221; from Higgses.<\/p>\n<p>I don&#8217;t think I buy this, though.\u00a0\u00a0 I don&#8217;t think there&#8217;s any circumstance in which this proposed experiment will provide a good test of NN&#8217;s theory.\u00a0 To see why, we have to dig into the probabilities a bit.<\/p>\n<p>Suppose that the Bayesian prior probability of NN&#8217;s theory being true (that is, our estimate of the probability before doing any tests) is p(NN).\u00a0 As Sean notes, p(NN) is a small number.\u00a0 Also, let p(SE) be the probability that Something Else (a huge fire, an earthquake, whatever) destroys the LHC before it finds the Higgs.\u00a0 Finally, let p(C) be the probability that we draw the bad card when we try the experiment.\u00a0 We get to choose p(C), of course, simply by choosing the number of cards in the deck.\u00a0 So how small should we make it?\u00a0 There are two constraints:<\/p>\n<ol>\n<li>We have to choose\u00a0 p(C) to be larger than p(SE).\u00a0 Otherwise, presumably, even if NN&#8217;s theory is true, the Universe is likely to save itself from the Higgs simply by causing the fire, so the card experiment is unlikely to tell us anything.<\/li>\n<li>We have to choose p(C) to besmaller than p(NN).\u00a0 The idea here is that if p(C) is too large, then our level of surprise when we pick that one card isn&#8217;t great enough to overcome our initial skepticism.\u00a0 That is, we still wouldn&#8217;t believe NN&#8217;s theory even after picking the card.\u00a0 Intuitively, I hope it makes sense that there must be such a constraint &#8212; if we did the experiment with 10 cards, it wouldn&#8217;t convince anyone!\u00a0 The fact that the constraint is that p(C)&lt;p(NN) comes from a little calculation using Bayes&#8217;s theorem.\u00a0 Pester me if you want details.<\/li>\n<\/ol>\n<p>In order for it to be possible to design an experiment that meets both of these constraints, we need p(SE)&lt;p(NN).\u00a0 That is, we need to believe, right now, that NN&#8217;s crazy theory is more likely than the union of all of the possible things that could go catastrophically wrong at the LHC. Personally, I think that&#8217;s extremely far from being the case,which means that NN&#8217;s proposed test of their theory is impossible even in principle.<\/p>\n<p>(Constraint 1 already makes the experiment impossible in practice: it says that we have to take a risk with the LHC that is greater than all the other risks.\u00a0 Good luck getting the hundreds of people whose careers are riding on the LHC to assume such a\u00a0 risk.)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>I guess this piece in the NY Times has been getting some attention lately.\u00a0 It&#8217;s about a crazy theory by Nelson and Ninomiya (NN for short) in which the laws of physics don&#8217;t &#8220;want&#8221; the Higgs boson to be created.\u00a0 According to this theory, states of the Universe in which lots of Higgses are created &hellip; <a href=\"https:\/\/blog.richmond.edu\/physicsbunn\/2009\/10\/15\/is-the-lhc-doomed-by-signals-from-the-future\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Is the LHC doomed by signals from the future?<\/span><\/a><\/p>\n","protected":false},"author":12,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-170","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"jetpack_featured_media_url":"","_links":{"self":[{"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/posts\/170","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/users\/12"}],"replies":[{"embeddable":true,"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/comments?post=170"}],"version-history":[{"count":0,"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/posts\/170\/revisions"}],"wp:attachment":[{"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/media?parent=170"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/categories?post=170"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blog.richmond.edu\/physicsbunn\/wp-json\/wp\/v2\/tags?post=170"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}