{"version":"1.0","provider_name":"Professor Talat S. Rahman","provider_url":"https:\/\/sciences.ucf.edu\/physics\/rahman-group","author_name":"Eric Switzer","author_url":"https:\/\/sciences.ucf.edu\/physics\/rahman-group\/author\/er583361\/","title":"A closer look at how symmetry constraints and the spin\u2013orbit coupling shape the electronic structure of Bi (111) - Professor Talat S. Rahman","type":"rich","width":600,"height":338,"html":"<blockquote class=\"wp-embedded-content\" data-secret=\"hKbqmNXgXj\"><a href=\"https:\/\/sciences.ucf.edu\/physics\/rahman-group\/ortigoza-et-al-2023\/\">A closer look at how symmetry constraints and the spin\u2013orbit coupling shape the electronic structure of Bi (111)<\/a><\/blockquote><iframe sandbox=\"allow-scripts\" security=\"restricted\" src=\"https:\/\/sciences.ucf.edu\/physics\/rahman-group\/ortigoza-et-al-2023\/embed\/#?secret=hKbqmNXgXj\" width=\"600\" height=\"338\" title=\"&#8220;A closer look at how symmetry constraints and the spin\u2013orbit coupling shape the electronic structure of Bi (111)&#8221; &#8212; Professor Talat S. Rahman\" data-secret=\"hKbqmNXgXj\" frameborder=\"0\" marginwidth=\"0\" marginheight=\"0\" scrolling=\"no\" class=\"wp-embedded-content\"><\/iframe><script>\n\/*! This file is auto-generated *\/\n!function(d,l){\"use strict\";l.querySelector&&d.addEventListener&&\"undefined\"!=typeof URL&&(d.wp=d.wp||{},d.wp.receiveEmbedMessage||(d.wp.receiveEmbedMessage=function(e){var t=e.data;if((t||t.secret||t.message||t.value)&&!\/[^a-zA-Z0-9]\/.test(t.secret)){for(var s,r,n,a=l.querySelectorAll('iframe[data-secret=\"'+t.secret+'\"]'),o=l.querySelectorAll('blockquote[data-secret=\"'+t.secret+'\"]'),c=new RegExp(\"^https?:$\",\"i\"),i=0;i<o.length;i++)o[i].style.display=\"none\";for(i=0;i<a.length;i++)s=a[i],e.source===s.contentWindow&&(s.removeAttribute(\"style\"),\"height\"===t.message?(1e3<(r=parseInt(t.value,10))?r=1e3:~~r<200&&(r=200),s.height=r):\"link\"===t.message&&(r=new URL(s.getAttribute(\"src\")),n=new URL(t.value),c.test(n.protocol))&&n.host===r.host&&l.activeElement===s&&(d.top.location.href=t.value))}},d.addEventListener(\"message\",d.wp.receiveEmbedMessage,!1),l.addEventListener(\"DOMContentLoaded\",function(){for(var e,t,s=l.querySelectorAll(\"iframe.wp-embedded-content\"),r=0;r<s.length;r++)(t=(e=s[r]).getAttribute(\"data-secret\"))||(t=Math.random().toString(36).substring(2,12),e.src+=\"#?secret=\"+t,e.setAttribute(\"data-secret\",t)),e.contentWindow.postMessage({message:\"ready\",secret:t},\"*\")},!1)))}(window,document);\n\/\/# sourceURL=https:\/\/sciences.ucf.edu\/physics\/rahman-group\/wp-includes\/js\/wp-embed.min.js\n<\/script>\n","description":"Fully relativistic density-functional-theory calculations of Bi(111) thin films are analyzed to revisit their two metallic surface-states branches. We first contrast these metallic branches with surface states arising at gaps in the valence band opened by the spin\u2013orbit coupling (SOC). We find that the two metallic branches along\u00a0\u0393\ud835\udc40\u2015\u00a0do not overlap with the bulk band at the ... Read more","thumbnail_url":"https:\/\/sciences.ucf.edu\/physics\/rahman-group\/wp-content\/uploads\/sites\/40\/2024\/05\/cmacfb67f1_hr-789x1024.jpg"}