{"id":378,"date":"2007-04-10T08:05:00","date_gmt":"2007-04-10T08:05:00","guid":{"rendered":"http:\/\/scientopia.org\/blogs\/goodmath\/2007\/04\/10\/degrees-and-exponents-of-infinities-in-the-surreal-numbers\/"},"modified":"2007-04-10T08:05:00","modified_gmt":"2007-04-10T08:05:00","slug":"degrees-and-exponents-of-infinities-in-the-surreal-numbers","status":"publish","type":"post","link":"http:\/\/www.goodmath.org\/blog\/2007\/04\/10\/degrees-and-exponents-of-infinities-in-the-surreal-numbers\/","title":{"rendered":"Degrees and Exponents of Infinities in the Surreal Numbers"},"content":{"rendered":"<p> When I first read about the sign-expanded form of the surreal numbers, my first thought was &#8220;cool, but what about infinity?&#8221; After all, one of the amazing things about the surreal numbers is the way that they make infinite and infinitessimal numbers a natural part of the number system in such an amazing way.<\/p>\n<p> Fortunately, it turns out to be very easy to play with infinities in sign-expanded form: you just need to use exponents of &omega;. Fortunately, exponents of &omega; are really cool! Getting to the point where we&#8217;ve really captured the meaning of exponents of infinity, so that we can talk about general infinities in terms of sign expansion for is going to take a bit of work. So as a bit of motivation, and to give you a first taste, since 1\/2 has a sign-expanded form of &#8220;+-&#8220;, (that is, integer part=0, binary fractional part or 0.1=1\/2), &omega;\/2 = +<sup>&omega;<\/sup>&#8211;<sup>&omega;<\/sup>.<\/p>\n<p><!--more--><\/p>\n<p> To get to the point where we can actually talk about sign-expanded forms of infinites or infinitessimals, we need to look a bit deeper into the structure of the surreal numbers, and how infinite numbers relate and behave. To make things easier, we&#8217;ll look only at the positive numbers; we can do the same thing with the negatives in an obvious way.<\/p>\n<p> We&#8217;ll start by defining a new kind of equivalence class based on a relationship called commensurance. Two numbers x and y are <em>comnmensurate<\/em> if and only if there exists some <em>integer<\/em> n such that x&lt;ny and y&lt;nx.<\/p>\n<p> What are the equivalence classes of the commensurance relation? Let&#8217;s start simple. Take any two finite real numbers, x and y greater than or equal to 1. There&#8217;s always some <em>integer<\/em> N for which x&lt;ny and y&lt;nx. So all of the finite numbers from one onward are part of a commensurate equivalence class. But &omega; isn&#8217;t part of that class. After all, &omega; isn&#8217;t an integer &#8211; integers, by definition in the surreals, have <em>finite<\/em> left and right sets &#8211; but &omega; has an infinite left set. So &omega; is part of a different commensurate equivalence class.<\/p>\n<p> And then, we can see the same thing happen with &omega; that we saw with the finite reals. There&#8217;s some set of values starting with &omega; where an integer multiplier can make the commensurance inequalities work. But then there&#8217;s another range beyond that &#8211; the places where an integer multiplier can&#8217;t reach. In fact, there&#8217;s a whole hierarchy of those &#8211; of infinities unreachable from other infinities!<\/p>\n<p> In each equivalence class of commensurate values, there&#8217;s a <em>simplest value<\/em> &#8211; that is, the value in the class with the earliest birthday. We call that value the <em>leader<\/em> of the class. So, for example, the first commensurate class is all of the finite positive numbers greater than one: because for any pair x and y, there is <em>some<\/em> integer z where x&lt;zy and y&lt;zx. The earliest-born number in that class is 1 &#8211; which for our purposes here, we can also write as &omega;<sup>0<\/sup>.<\/p>\n<p> The second two commensurate classes are the basic infinite and infinitessimals. There&#8217;s a commensurate class of basic infinite values, whose leader is &omega;, and there&#8217;s a commensurate class of basic infinitessimal values, whose leader is 1\/&omega;, which we&#8217;ll write &omega;<sup>-1<\/sup>. Then there&#8217;s another commensurate class of infinites &#8211; infinites that relate to &omega; in the same way that &omega; relates to 1. The leader of that, we call &omega;<sup>2<\/sup>. Note that this is not an exponent in the normal logarithmic sense &#8211; it&#8217;s <em>not<\/em> just &omega;&times;&omega; &#8211; it&#8217;s a number that&#8217;s a member of a second order of infinite values. And as we saw before, we can keep going, climbing the heirarchy of commensurance classes of infinity. For each successive class, we call the leader a <em>power<\/em> of &omega;. We can keep pushing this notion of &#8220;powers&#8221; of infinity as far as we like &#8211; there are &omega;<sup>n<\/sup> for all positive integers n. There&#8217;s also the equivalent notion going into infinitessimals. 1\/&omega; is written &omega;<sup>-1<\/sup>, and it&#8217;s the leader of the first commensurate class of infinitessimals. There are also greater degrees of infinitessimals formed in the same way &#8211; numbers so small that they&#8217;re infinitely smaller than the first infinitely small number &omega;<sup>-1<\/sup>; we call the leader of the second commensurate class of infinitessimals &omega;<sup>-2<\/sup>, and so on.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>When I first read about the sign-expanded form of the surreal numbers, my first thought was &#8220;cool, but what about infinity?&#8221; After all, one of the amazing things about the surreal numbers is the way that they make infinite and infinitessimal numbers a natural part of the number system in such an amazing way. Fortunately, [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":"","jetpack_publicize_message":"","jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":false,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2}},"categories":[62],"tags":[],"class_list":["post-378","post","type-post","status-publish","format-standard","hentry","category-surreal-numbers"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_shortlink":"https:\/\/wp.me\/p4lzZS-66","jetpack_sharing_enabled":true,"jetpack_likes_enabled":true,"_links":{"self":[{"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/posts\/378","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/comments?post=378"}],"version-history":[{"count":0,"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/posts\/378\/revisions"}],"wp:attachment":[{"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/media?parent=378"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/categories?post=378"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/www.goodmath.org\/blog\/wp-json\/wp\/v2\/tags?post=378"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}