{"version":"1.0","provider_name":"Dynamics and Transport in Quantum Matter","provider_url":"https:\/\/phsites.technion.ac.il\/dtqm","author_name":"Adi","author_url":"https:\/\/phsites.technion.ac.il\/dtqm\/author\/adile\/","title":"Mott skyrmions: Stabilizing the false vacuum - Dynamics and Transport in Quantum Matter","type":"rich","width":600,"height":338,"html":"<blockquote class=\"wp-embedded-content\" data-secret=\"tpUVWgge7U\"><a href=\"https:\/\/phsites.technion.ac.il\/dtqm\/gergely-zarand-mott-skyrmions-stabilizing-false-vacuum\/\">Mott skyrmions: Stabilizing the false vacuum<\/a><\/blockquote><iframe sandbox=\"allow-scripts\" security=\"restricted\" src=\"https:\/\/phsites.technion.ac.il\/dtqm\/gergely-zarand-mott-skyrmions-stabilizing-false-vacuum\/embed\/#?secret=tpUVWgge7U\" width=\"600\" height=\"338\" title=\"&#8220;Mott skyrmions: Stabilizing the false vacuum&#8221; &#8212; Dynamics and Transport in Quantum Matter\" data-secret=\"tpUVWgge7U\" frameborder=\"0\" marginwidth=\"0\" marginheight=\"0\" scrolling=\"no\" class=\"wp-embedded-content\"><\/iframe><script type=\"text\/javascript\">\n\/* <![CDATA[ *\/\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:\/\/phsites.technion.ac.il\/dtqm\/wp-includes\/js\/wp-embed.min.js\n\/* ]]> *\/\n<\/script>\n","description":"Gergely Zar\u00e1nd Topological excitations keep fascinating physicists since many decades. While individual vortices and solitons emerge and have been observed in many areas of physics, their most intriguing higher dimensional topological relatives, skyrmions \u00a0and magnetic monopoles remained mostly elusive. Here we propose that loading a three-component nematic superfluid such as 23Na into a deep optical &hellip;"}