{"id":89957,"date":"2025-10-19T13:30:43","date_gmt":"2025-10-19T11:30:43","guid":{"rendered":"https:\/\/port.lukasiewicz.gov.pl\/?post_type=projects&#038;p=89957"},"modified":"2026-03-16T12:37:47","modified_gmt":"2026-03-16T11:37:47","slug":"fast-and-bright-perovskite-scintillator-enhanced-by-the-purcell-effect-fapurite","status":"publish","type":"projects","link":"https:\/\/port.lukasiewicz.gov.pl\/en\/projekty-badawcze\/fast-and-bright-perovskite-scintillator-enhanced-by-the-purcell-effect-fapurite\/","title":{"rendered":"Fast and Bright Perovskite Scintillator Enhanced by the Purcell Effect &#8211; Fapurite"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-post\" data-elementor-id=\"89957\" class=\"elementor elementor-89957 elementor-67577\" data-elementor-post-type=\"projects\">\n\t\t\t\t<div class=\"elementor-element elementor-element-49af498 e-flex e-con-boxed e-con e-parent\" data-id=\"49af498\" data-element_type=\"container\" data-e-type=\"container\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t\t\t<div class=\"elementor-element elementor-element-ca6200a elementor-widget elementor-widget-text-editor\" data-id=\"ca6200a\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p data-start=\"110\" data-end=\"201\">Project funded by the <strong data-start=\"132\" data-end=\"165\">National Science Centre (NCN)<\/strong> under the <strong data-start=\"176\" data-end=\"187\">OPUS 24<\/strong> competition<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-7cdc54d elementor-widget elementor-widget-image\" data-id=\"7cdc54d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"2560\" height=\"216\" src=\"https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-scaled.webp\" class=\"attachment-full size-full wp-image-86250\" alt=\"Logo Narodowego Centrum Nauki NCN\" srcset=\"https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-scaled.webp 2560w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-300x25.webp 300w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-1024x86.webp 1024w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-768x65.webp 768w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-1536x130.webp 1536w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-2048x173.webp 2048w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-1200x101.webp 1200w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-1980x167.webp 1980w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-24x2.webp 24w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-36x3.webp 36w, https:\/\/port.lukasiewicz.gov.pl\/wp-content\/uploads\/sites\/35\/2025\/08\/ncn-logo-poziom-48x4.webp 48w\" sizes=\"(max-width: 2560px) 100vw, 2560px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-f66a5c7 cut-off-wrapper-90 elementor-widget__width-initial elementor-widget-tablet__width-initial elementor-widget-mobile__width-inherit elementor-widget elementor-widget-text-editor\" data-id=\"f66a5c7\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Project number: <strong data-start=\"219\" data-end=\"242\">2022\/47\/B\/ST5\/01966<\/strong><br data-start=\"242\" data-end=\"245\" \/>Project value: <strong data-start=\"260\" data-end=\"280\">1,520,820.00 PLN<\/strong><br data-start=\"280\" data-end=\"283\" \/>Funding amount: <strong data-start=\"299\" data-end=\"319\">1,520,820.00 PLN<\/strong><br data-start=\"319\" data-end=\"322\" \/>Project duration: <strong data-start=\"340\" data-end=\"367\">02\/10\/2023 \u2013 01\/10\/2026<\/strong><br data-start=\"367\" data-end=\"370\" \/>Project manager: <strong data-start=\"387\" data-end=\"422\">Muhammad Danang Birowosuto, PhD<\/strong><\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-6a2659d elementor-align-left elementor-widget elementor-widget-button\" data-id=\"6a2659d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"button.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<div class=\"elementor-button-wrapper\">\n\t\t\t\t\t<a class=\"elementor-button elementor-button-link elementor-size-sm\" href=\"https:\/\/bazawiedzy.port.lukasiewicz.gov.pl\/info\/projectmain\/PORTcd112e50059d45c69c5da93b27260f4d?r=projectmain&#038;ps=20&#038;tab=&#038;title=Projekty%2B%25E2%2580%2593%2BSzybki%2Bi%2Bjasny%2Bscyntylator%2Bperowskitowy%2Bwzmocniony%2BPurcellem%2B%25E2%2580%2593%2BSie%25C4%2587%2BBadawcza%2B%25C5%2581ukasiewicz%2B-%2BPORT%2BPolski%2BO%25C5%259Brodek%2BRozwoju%2BTechnologii&#038;lang=pl\">\n\t\t\t\t\t\t<span class=\"elementor-button-content-wrapper\">\n\t\t\t\t\t\t<span class=\"elementor-button-icon\">\n\t\t\t\t<svg aria-hidden=\"true\" class=\"e-font-icon-svg e-fas-arrow-right\" viewBox=\"0 0 448 512\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\"><path d=\"M190.5 66.9l22.2-22.2c9.4-9.4 24.6-9.4 33.9 0L441 239c9.4 9.4 9.4 24.6 0 33.9L246.6 467.3c-9.4 9.4-24.6 9.4-33.9 0l-22.2-22.2c-9.5-9.5-9.3-25 .4-34.3L311.4 296H24c-13.3 0-24-10.7-24-24v-32c0-13.3 10.7-24 24-24h287.4L190.9 101.2c-9.8-9.3-10-24.8-.4-34.3z\"><\/path><\/svg>\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t<span class=\"elementor-button-text\">VIEW PROJECT<\/span>\n\t\t\t\t\t<\/span>\n\t\t\t\t\t<\/a>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-e0f2b15 elementor-widget elementor-widget-text-editor\" data-id=\"e0f2b15\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p data-start=\"451\" data-end=\"763\">Scintillation materials are sensitive to <strong data-start=\"492\" data-end=\"514\">ionizing radiation<\/strong> and are widely used in various <strong data-start=\"546\" data-end=\"567\">detection systems<\/strong>, including <strong data-start=\"579\" data-end=\"598\">medical imaging<\/strong>, <strong data-start=\"600\" data-end=\"621\">homeland security<\/strong>, <strong data-start=\"623\" data-end=\"664\">high-energy physics (HEP) calorimetry<\/strong>, <strong data-start=\"666\" data-end=\"689\">energy applications<\/strong>, <strong data-start=\"691\" data-end=\"713\">industrial control<\/strong>, <strong data-start=\"715\" data-end=\"735\">oil-well logging<\/strong>, and <strong data-start=\"741\" data-end=\"760\">quantum sensors<\/strong>.<\/p><p data-start=\"765\" data-end=\"1195\">Some scintillators exhibit properties enabling applications beyond static radiation imaging \u2014 such as <strong data-start=\"867\" data-end=\"903\">time-of-flight (TOF) measurement<\/strong>, <strong data-start=\"905\" data-end=\"921\">spectroscopy<\/strong>, and <strong data-start=\"927\" data-end=\"970\">ultrafast multi-frame radiation imaging<\/strong>. Two key properties determine their performance: <strong data-start=\"1020\" data-end=\"1035\">light yield<\/strong> (the number of visible photons produced per unit of deposited radiation energy) and <strong data-start=\"1120\" data-end=\"1134\">decay time<\/strong> (the speed at which photons are emitted after excitation).<\/p><p data-start=\"1197\" data-end=\"1658\">Both parameters influence <strong data-start=\"1223\" data-end=\"1260\">coincidence time resolution (CTR)<\/strong> in <strong data-start=\"1264\" data-end=\"1302\">positron emission tomography (PET)<\/strong> and <strong data-start=\"1307\" data-end=\"1334\">output count rate (OCR)<\/strong> in <strong data-start=\"1338\" data-end=\"1384\">photon-counting computed tomography (PCCT)<\/strong> and <strong data-start=\"1389\" data-end=\"1420\">fast spectral X-ray imaging<\/strong>. CTR values below <strong data-start=\"1439\" data-end=\"1448\">30 ps<\/strong> significantly enhance TOF-PET image quality by improving the <strong data-start=\"1510\" data-end=\"1535\">signal-to-noise ratio<\/strong>, while <strong data-start=\"1543\" data-end=\"1566\">OCR &gt; 20 Mcps\/pixel<\/strong> in PCCT would surpass the performance of current <strong data-start=\"1616\" data-end=\"1655\">CdTe\/CZT semiconductor technologies<\/strong>.<\/p><p data-start=\"1660\" data-end=\"2003\">The best commercial PET scintillator, <strong data-start=\"1698\" data-end=\"1721\">Lu\u2082SiO\u2085:Ce (LSO:Ce)<\/strong>, achieves a CTR of <strong data-start=\"1741\" data-end=\"1750\">60 ps<\/strong>, but its cost (~426 EUR for a 20\u00d720\u00d720 mm\u00b3 crystal) makes complete TOF-PET systems <strong data-start=\"1834\" data-end=\"1857\">extremely expensive<\/strong>. Furthermore, progress in PCCT using existing semiconductor technologies is limited due to the need for more <strong data-start=\"1967\" data-end=\"2000\">stable and reliable detectors<\/strong>.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-ad6a88f elementor-widget elementor-widget-heading\" data-id=\"ad6a88f\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Project concept<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-f6d69da elementor-widget elementor-widget-text-editor\" data-id=\"f6d69da\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p data-start=\"2035\" data-end=\"2285\">Inspired by advances in <strong data-start=\"2059\" data-end=\"2076\">photovoltaics<\/strong>, this project proposes <strong data-start=\"2100\" data-end=\"2149\">solution-processable perovskite scintillators<\/strong> as a <strong data-start=\"2155\" data-end=\"2185\">cost-effective alternative<\/strong> to LSO:Ce \u2014 potentially reducing costs <strong data-start=\"2225\" data-end=\"2252\">by a factor of up to 50<\/strong>. Two promising candidates are:<\/p><ul data-start=\"2287\" data-end=\"2410\"><li data-start=\"2287\" data-end=\"2352\"><p data-start=\"2289\" data-end=\"2352\"><strong data-start=\"2289\" data-end=\"2350\">2D hybrid organic\u2013inorganic perovskite crystals (2D HOIP)<\/strong><\/p><\/li><li data-start=\"2353\" data-end=\"2410\"><p data-start=\"2355\" data-end=\"2410\"><strong data-start=\"2355\" data-end=\"2408\">Lead-free all-inorganic perovskite crystals (AIP)<\/strong><\/p><\/li><\/ul><p data-start=\"2412\" data-end=\"2820\">Current 2D HOIP scintillators exhibit a <strong data-start=\"2452\" data-end=\"2483\">light yield &gt;20 photons\/keV<\/strong> and <strong data-start=\"2488\" data-end=\"2509\">decay times &lt;5 ns<\/strong>, resulting in a CTR of about <strong data-start=\"2539\" data-end=\"2548\">80 ps<\/strong> \u2014 slightly inferior to LSO:Ce but with an <strong data-start=\"2591\" data-end=\"2636\">absorption length only four times greater<\/strong>. Lead-free AIP crystals, with an absorption length comparable to LSO:Ce, achieve up to <strong data-start=\"2724\" data-end=\"2743\">100 photons\/keV<\/strong>, yet their <strong data-start=\"2755\" data-end=\"2779\">decay times (~50 ns)<\/strong> yield CTR values exceeding <strong data-start=\"2807\" data-end=\"2817\">150 ps<\/strong>.<\/p><p data-start=\"2822\" data-end=\"3091\">To achieve the target <strong data-start=\"2844\" data-end=\"2857\">30 ps CTR<\/strong>, the <strong data-start=\"2863\" data-end=\"2878\">light yield<\/strong> of 2D HOIP and AIP scintillators must be <strong data-start=\"2920\" data-end=\"2951\">enhanced three- to fivefold<\/strong>. For PCCT, current 2D HOIP crystals already reach <strong data-start=\"3002\" data-end=\"3019\">10 Mcps\/pixel<\/strong>, only two times lower than state-of-the-art semiconductor technology.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-49800c2 elementor-widget elementor-widget-heading\" data-id=\"49800c2\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Project objective<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-6d6fe0f elementor-widget elementor-widget-text-editor\" data-id=\"6d6fe0f\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>The <strong data-start=\"3129\" data-end=\"3149\">Fapurite project<\/strong> aims to overcome these limitations by employing <strong data-start=\"3198\" data-end=\"3215\">nanophotonics<\/strong>, specifically <strong data-start=\"3230\" data-end=\"3257\">resonant nanostructures<\/strong>, to enhance light emission through the <strong data-start=\"3297\" data-end=\"3315\">Purcell effect<\/strong>. This approach will simultaneously improve <strong data-start=\"3359\" data-end=\"3374\">light yield<\/strong> and <strong data-start=\"3379\" data-end=\"3393\">decay time<\/strong>, enabling a <strong data-start=\"3406\" data-end=\"3426\">reduction in CTR<\/strong> and an <strong data-start=\"3434\" data-end=\"3453\">increase in OCR<\/strong>, paving the way for <strong data-start=\"3474\" data-end=\"3534\">faster and more efficient perovskite-based scintillators<\/strong> for advanced imaging technologies.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Project funded by the National Science Centre (NCN) under the OPUS 24 competition Project number: 2022\/47\/B\/ST5\/01966Project value: 1,520,820.00 PLNFunding amount: 1,520,820.00 PLNProject duration: 02\/10\/2023 \u2013 01\/10\/2026Project manager: Muhammad Danang Birowosuto, PhD VIEW PROJECT Scintillation materials are sensitive to ionizing radiation and are widely used in various detection systems, including medical imaging, homeland security, high-energy physics [&hellip;]<\/p>\n","protected":false},"featured_media":80863,"menu_order":0,"template":"","format":"standard","meta":{"_acf_changed":false,"_seopress_robots_primary_cat":"","_seopress_titles_title":"","_seopress_titles_desc":"","_seopress_robots_index":"","inline_featured_image":false,"footnotes":""},"categories":[747],"grupy_badawcze":[622],"pozostale_projekty":[],"class_list":["post-89957","projects","type-projects","status-publish","format-standard","has-post-thumbnail","hentry","category-nsc","grupy_badawcze-grupa-badawcza-materialow-dla-fotoniki"],"acf":{"kierownik_projektu":["Dr. Muhammad Danang Birowosuto"],"dofinansowanie":"Narodowe Centrum Nauki","grupa_badawcza":["Photonic Materials Research Group"],"nazwa_projektu":"","tematyka_projektu":"","opis_projektu":"","dofinanowanie":"National Science Centre"},"publishpress_future_action":{"enabled":true,"date":"2026-09-01 00:00:00","action":"category","newStatus":"draft","terms":[595],"taxonomy":"category","extraData":[]},"publishpress_future_workflow_manual_trigger":{"enabledWorkflows":[]},"_links":{"self":[{"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/projects\/89957","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/projects"}],"about":[{"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/types\/projects"}],"version-history":[{"count":5,"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/projects\/89957\/revisions"}],"predecessor-version":[{"id":95448,"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/projects\/89957\/revisions\/95448"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/media\/80863"}],"wp:attachment":[{"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/media?parent=89957"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/categories?post=89957"},{"taxonomy":"grupy_badawcze","embeddable":true,"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/grupy_badawcze?post=89957"},{"taxonomy":"pozostale_projekty","embeddable":true,"href":"https:\/\/port.lukasiewicz.gov.pl\/en\/wp-json\/wp\/v2\/pozostale_projekty?post=89957"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}