{"id":4025,"date":"2024-09-19T21:51:30","date_gmt":"2024-09-19T21:51:30","guid":{"rendered":"https:\/\/workhouse.sweetdishy.com\/?p=4025"},"modified":"2024-09-24T11:07:50","modified_gmt":"2024-09-24T11:07:50","slug":"properties-of-the-density-operator","status":"publish","type":"post","link":"https:\/\/workhouse.sweetdishy.com\/index.php\/2024\/09\/19\/properties-of-the-density-operator\/","title":{"rendered":"Properties of the density operator"},"content":{"rendered":"\n<p>The density operator on a Hilbert space, de\ufb01ned by Equation 5.4 satis\ufb01es<\/p>\n\n\n\n<p>the following properties:<\/p>\n\n\n\n<p>1. \u02c6\u03c1 is Hermitian.<\/p>\n\n\n\n<p>Proof: \u02c6\u03c1<\/p>\n\n\n\n<p>\u2020<\/p>\n\n\n\n<p>=<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>\u2217<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>\u2020<\/p>\n\n\n\n<p>h\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|<\/p>\n\n\n\n<p>\u2020<\/p>\n\n\n\n<p>=<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>ih\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>| = \u02c6\u03c1. (5.11)<\/p>\n\n\n\n<p>2. \u02c6\u03c1 is non-negative, that is, for any vector |vi, hv|\u02c6\u03c1|vi \u2265 0. (This translates<\/p>\n\n\n\n<p>to its eigenvalues being non-negative, or det(\u03c1) \u2265 0.)<\/p>\n\n\n\n<p>Proof: hv|\u02c6\u03c1|vi =<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>hv|p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>ih\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|vi<\/p>\n\n\n\n<p>=<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|hv|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>i|<\/p>\n\n\n\n<p>2<\/p>\n\n\n\n<p>\u2265 0 (5.12)<\/p>\n\n\n\n<p>since the right side is a sum of numbers that are always positive or zero.<\/p>\n\n\n\n<p>3. It satis\ufb01es Tr\u02c6\u03c1 = 1.<\/p>\n\n\n\n<p>Proof: In an orthonormal basis {|ii},<\/p>\n\n\n\n<p>Tr\u03c1 =<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>hi|<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>ih\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|<\/p>\n\n\n\n<p>!<\/p>\n\n\n\n<p>|ii<\/p>\n\n\n\n<p>=<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>hi|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>ih\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|ii<\/p>\n\n\n\n<p>=<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>h\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>|iihi|<\/p>\n\n\n\n<p>!<\/p>\n\n\n\n<p>|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>=<\/p>\n\n\n\n<p>X<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>p<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>h\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>|\u03c8<\/p>\n\n\n\n<p>n<\/p>\n\n\n\n<p>i = 1 (5.13)<\/p>\n\n\n\n<p>In general, any operator on a Hilbert space satisfying these properties is<\/p>\n\n\n\n<p>de\ufb01ned as a density operator and can be used to predict the probabilities of<\/p>\n\n\n\n<p>outcomes of measurement on the system, bypassing the state-vector formalism<\/p>\n\n\n\n<p>altogether.<\/p>\n\n\n\n<p>Example 5.1.4. For a system described by continuous variables, for example<\/p>\n\n\n\n<p>position x, the density operator will be expressed as<\/p>\n\n\n\n<p>\u03c1 =<\/p>\n\n\n\n<p>Z<\/p>\n\n\n\n<p>dx dx<\/p>\n\n\n\n<p>0<\/p>\n\n\n\n<p>\u03c9(x, x<\/p>\n\n\n\n<p>0<\/p>\n\n\n\n<p>)|xihx<\/p>\n\n\n\n<p>Mixed States, Open Systems, and the Density Operator 83<\/p>\n\n\n\n<p>For a pure state, we will have<\/p>\n\n\n\n<p>\u03c1 =<\/p>\n\n\n\n<p>Z<\/p>\n\n\n\n<p>dx dx<\/p>\n\n\n\n<p>0<\/p>\n\n\n\n<p>\u03c8(x)\u03c8<\/p>\n\n\n\n<p>\u2217<\/p>\n\n\n\n<p>(x<\/p>\n\n\n\n<p>0<\/p>\n\n\n\n<p>)|xihx<\/p>\n\n\n\n<p>0<\/p>\n\n\n\n<p>|, (5.15)<\/p>\n\n\n\n<p>where \u03c8(x) = hx|\u03c8i.<\/p>\n\n\n\n<p>Another property of the density operator that will be useful to us is con-<\/p>\n\n\n\n<p>vexity:<\/p>\n\n\n\n<p>De\ufb01nition 5.3. Convexity: A set of operators {\u02c6\u03c1<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>} form a convex set if<\/p>\n\n\n\n<p>\u03c1 = \u03bb\u03c1<\/p>\n\n\n\n<p>1<\/p>\n\n\n\n<p>+ (1 \u2212 \u03bb)\u03c1<\/p>\n\n\n\n<p>2<\/p>\n\n\n\n<p>, 0 &lt; \u03bb &lt; 1, (5.16)<\/p>\n\n\n\n<p>for every pair \u03c1<\/p>\n\n\n\n<p>1<\/p>\n\n\n\n<p>, \u03c1<\/p>\n\n\n\n<p>2<\/p>\n\n\n\n<p>\u2208 {\u03c1<\/p>\n\n\n\n<p>i<\/p>\n\n\n\n<p>}.<\/p>\n\n\n\n<p>Convexity has a very simple meaning: any two members of a convex set<\/p>\n\n\n\n<p>can be connected by a straight line without leaving the set. (See Figure 5.1.)<\/p>\n\n\n\n<p>FIGURE 5.1: (a) A convex set, (b) A non-convex set.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The density operator on a Hilbert space, de\ufb01ned by Equation 5.4 satis\ufb01es the following properties: 1. \u02c6\u03c1 is Hermitian. Proof: \u02c6\u03c1 \u2020 = X n p \u2217 n |\u03c8 n i \u2020 h\u03c8 n | \u2020 = X n p n |\u03c8 n ih\u03c8 n | = \u02c6\u03c1. (5.11) 2. \u02c6\u03c1 is non-negative, that is, [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":4020,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[491],"tags":[],"class_list":["post-4025","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-5-grand-unification"],"jetpack_featured_media_url":"https:\/\/workhouse.sweetdishy.com\/wp-content\/uploads\/2024\/09\/quantum-1.png","_links":{"self":[{"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/posts\/4025","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/comments?post=4025"}],"version-history":[{"count":3,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/posts\/4025\/revisions"}],"predecessor-version":[{"id":4567,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/posts\/4025\/revisions\/4567"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/media\/4020"}],"wp:attachment":[{"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/media?parent=4025"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/categories?post=4025"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/workhouse.sweetdishy.com\/index.php\/wp-json\/wp\/v2\/tags?post=4025"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}