{"id":87,"date":"2010-07-30T09:05:48","date_gmt":"2010-07-30T13:05:48","guid":{"rendered":"http:\/\/blogs.nd.edu\/condensed-matter-physics\/"},"modified":"2010-08-28T00:27:06","modified_gmt":"2010-08-28T04:27:06","slug":"nanoscale","status":"publish","type":"page","link":"https:\/\/sites.nd.edu\/condensed-matter-physics\/research\/nanoscale\/","title":{"rendered":"Universal Emission: Blinking stars on nanoscale"},"content":{"rendered":"<p><strong><br \/>\n<\/strong><\/p>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=w6T6GPgQIQI<\/p>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=5wmher9NMLk<\/p>\n<p>Very few problems of early quantum mechanics remain unsolved today.      Fluorescence intermittency is one exception. At the dawn of modern  quantum mechanics, Niels Bohr predicted &#8220;quantum jumps&#8221;       of electrons between discrete energy levels of atoms and molecules.  Such jumps were observed directly only during the 1980s      with the advent of single ion traps. An ongoing series of  experiments brought spectacular progress to single molecule imaging,      raising more questions than answers about these emission &#8220;jumps&#8221;.<\/p>\n<p>Basically all known fluorophores studied to date exhibit  fluorescence intermittency.      They include single molecules, individual fluorescent proteins,  polymer segments, semiconductor nanoparticles,       nanorods and even nanowires. Such jumps, where the fluorophore  literally stops emitting light under continuous excitation,      are very different from those predicted by Bohr. Rather than  occurring on the micro to millisecond timescales,       they last seconds and even minutes. These experimentally observed  off-times are vastly longer than any timescale one would      retrieve from a standard quantum mechanical model. The &#8220;dark&#8221; states  live practically forever. After these very long periods       of darkness, the fluorophore eventually emerges into an emitting  state. The new emissive state would be impossible if off      periods were simply photobleaching events.<\/p>\n<p>Even more intriguing are the statistics of the intermittency. Whereas Bohr would have postulated exponential distributions      of &#8220;on&#8221;-times and &#8220;off&#8221;-times, universal power law on-time and off-time probability densities are actually observed.       For colloidal quantum dots, this power law extends over an extraordinarily wide range that spans nine orders of magnitude      in probability density and five to six orders of magnitude in time. This is remarkable for many reasons.       First, the experimentally observed distribution refuses to yield a time scale. Second, universality on a lesser scale      has revolutionized our understanding about phase transitions. Finally, such statistics arise from the behavior of single     fluorophores, not an ensemble. Given that single organic molecules      also blink and exhibit near-identical power law blinking kinetics,  it is tempting to speculate that such striking       similarity is not an accident. We therefore ask whether there exist  unrecognized points of commonality between seemingly      disparate entities such as molecules and semiconductor  nanostructures.       While the underlying mechanism for answering such questions remains a  mystery, we argue in this perspective that many, if not all,      key experiments have already been conducted and that substantial  theoretical progress has been made.<\/p>\n<p>The figures below show representative examples of blinking in quantum dots and nano-wires.      An emission &#8220;trajectory&#8221; from both systems is provided, plotting emission intensity as a function of time.       In both cases the intensity fluctuates.  When a threshold is used to distinguish on- from off-states,      second-to-minute long off-times are apparent.<\/p>\n<h3>Click on any of the six panels below for more details:<\/h3>\n<p style=\"text-align: center\"><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_a_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-107\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_a.jpg\" alt=\"\" width=\"297\" height=\"220\" \/><\/a><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_b_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-108\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_b-300x217.jpg\" alt=\"\" width=\"300\" height=\"217\" srcset=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_b-300x217.jpg 300w, https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_b.jpg 303w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<p style=\"text-align: center\"><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_c_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-111\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_c.jpg\" alt=\"\" width=\"297\" height=\"207\" \/><\/a><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_e_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-112\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_e-300x204.jpg\" alt=\"\" width=\"300\" height=\"204\" srcset=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_e-300x204.jpg 300w, https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_e.jpg 303w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<p style=\"text-align: center\"><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_d1.jpg\"><\/a><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_d_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-113\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_d.jpg\" alt=\"\" width=\"297\" height=\"205\" \/><\/a><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_f_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-114\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_f-300x202.jpg\" alt=\"\" width=\"300\" height=\"202\" srcset=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_f-300x202.jpg 300w, https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig_1_f.jpg 303w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<h3>Below are static images and statistics of fluorescence intermittency for nanowires (click each image to see more detail):<\/h3>\n<p style=\"text-align: center\"><strong><strong><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_1_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-119\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_1-300x150.jpg\" alt=\"\" width=\"300\" height=\"150\" srcset=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_1-300x150.jpg 300w, https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_1.jpg 351w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_2_big.jpg\" target=\"_blank\"> <img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-140\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_2.jpg\" alt=\"\" width=\"251\" height=\"176\" \/><\/a> <a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_3_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-141\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_3-300x125.jpg\" alt=\"\" width=\"300\" height=\"125\" srcset=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_3-300x125.jpg 300w, https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_3.jpg 422w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/strong><\/strong><\/p>\n<p style=\"text-align: center\"><strong><strong><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_4_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-143\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_4.jpg\" alt=\"\" width=\"225\" height=\"298\" \/><\/a><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_5_big.jpg\" target=\"_blank\"> <img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-144\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_5.jpg\" alt=\"\" width=\"148\" height=\"298\" \/><\/a> <a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_6_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-medium wp-image-145\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_6-300x137.jpg\" alt=\"\" width=\"300\" height=\"137\" srcset=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_6-300x137.jpg 300w, https:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_6.jpg 651w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/strong><\/strong><\/p>\n<p style=\"text-align: center\"><strong><strong><a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_7_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-146\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_7.jpg\" alt=\"\" width=\"242\" height=\"121\" \/><\/a> <a href=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_8_big.jpg\" target=\"_blank\"><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-147\" src=\"http:\/\/sites.nd.edu\/condensed-matter-physics\/files\/2010\/07\/Fig3_8.jpg\" alt=\"\" width=\"118\" height=\"121\" \/><\/a><\/strong><\/strong><\/p>\n<p style=\"text-align: center\">\n<h3>Additional videos:<\/h3>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=JOH6iDu7HLw<\/p>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=nDnppIdPEbI<\/p>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=v_9uzz570yM<\/p>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=p4y6zhaHrx0<\/p>\n<p style=\"text-align: center\">httpv:\/\/www.youtube.com\/watch?v=d-YwnBXZnj8<\/p>\n<h3>This work was supported by:<\/h3>\n<ul>\n<li> <a href=\"http:\/\/www.google.com\/url?sa=t&amp;source=web&amp;cd=2&amp;ved=0CBYQFjAB&amp;url=http%3A%2F%2Fwww.nsf.gov%2Fcrssprgm%2Fnano%2F05610_nirt_38awards_web.xls&amp;ei=YB1TTOzVFdvpnQfEs8DyAw&amp;usg=AFQjCNErj2-Bpku24nA1ttmQq_eDv_vGeg\">The National Science Foundation NIRT Award 0609249 <\/a><\/li>\n<li> <a href=\"http:\/\/www.er.doe.gov\/bes\/BES.html\" target=\"_blank\">Department of Energy &#8211; Basic Energy Sciences <\/a><\/li>\n<li> <a href=\"Office of Naval Research \" target=\"_blank\">Office of Naval Research <\/a><\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>httpv:\/\/www.youtube.com\/watch?v=w6T6GPgQIQI httpv:\/\/www.youtube.com\/watch?v=5wmher9NMLk Very few problems of early quantum mechanics remain unsolved today. Fluorescence intermittency is one exception. At the dawn of modern quantum mechanics, Niels Bohr predicted &#8220;quantum jumps&#8221; of electrons between discrete energy levels of atoms and molecules. Such &hellip; <a href=\"https:\/\/sites.nd.edu\/condensed-matter-physics\/research\/nanoscale\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":42,"featured_media":0,"parent":3,"menu_order":1,"comment_status":"closed","ping_status":"open","template":"","meta":{"_monsterinsights_skip_tracking":false,"footnotes":""},"class_list":["post-87","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/pages\/87","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/users\/42"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/comments?post=87"}],"version-history":[{"count":63,"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/pages\/87\/revisions"}],"predecessor-version":[{"id":89,"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/pages\/87\/revisions\/89"}],"up":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/pages\/3"}],"wp:attachment":[{"href":"https:\/\/sites.nd.edu\/condensed-matter-physics\/wp-json\/wp\/v2\/media?parent=87"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}