{"version":"1.0","provider_name":"Bridging Laboratory Astrophysics, fuSion and phoTonics at Technion","provider_url":"https:\/\/phsites.technion.ac.il\/blastt","author_name":"Adi","author_url":"https:\/\/phsites.technion.ac.il\/blastt\/author\/adile\/","title":"Nuclear photonics - Bridging Laboratory Astrophysics, fuSion and phoTonics at Technion","type":"rich","width":600,"height":338,"html":"<blockquote class=\"wp-embedded-content\" data-secret=\"baH5xyE6Yj\"><a href=\"https:\/\/phsites.technion.ac.il\/blastt\/research\/nuclear-photonics\/\">Nuclear photonics<\/a><\/blockquote><iframe sandbox=\"allow-scripts\" security=\"restricted\" src=\"https:\/\/phsites.technion.ac.il\/blastt\/research\/nuclear-photonics\/embed\/#?secret=baH5xyE6Yj\" width=\"600\" height=\"338\" title=\"&#8220;Nuclear photonics&#8221; &#8212; Bridging Laboratory Astrophysics, fuSion and phoTonics at Technion\" data-secret=\"baH5xyE6Yj\" 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\/blastt\/wp-includes\/js\/wp-embed.min.js\n\/* ]]> *\/\n<\/script>\n","thumbnail_url":"http:\/\/phsites.technion.ac.il\/blastt\/wp-content\/uploads\/sites\/79\/2025\/11\/a-photo-for-the-photonics-theme.png","thumbnail_width":1062,"thumbnail_height":1020,"description":"Laser-driven high-brilliance sources offer new perspectives in terms of compact material probing, even of dense objects, or in imaging of high speed events, with better than picosecond resolution. We are currently working on pushing the capabilities of a dual (neutron and x-ray) interrogation method, based on ultra-intense lasers irradiating solid targets. The \u201cwhite\u201d (i.e. broadband) &hellip;"}