{"id":195,"date":"2024-10-16T18:10:53","date_gmt":"2024-10-16T18:10:53","guid":{"rendered":"https:\/\/seegroup.mit.edu\/?page_id=195"},"modified":"2025-06-07T20:13:05","modified_gmt":"2025-06-07T20:13:05","slug":"solar-cells","status":"publish","type":"page","link":"https:\/\/seegroup.mit.edu\/index.php\/solar-cells\/","title":{"rendered":"Solar Cells"},"content":{"rendered":"<p>[et_pb_section fb_built=&#8221;1&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row column_structure=&#8221;2_3,1_3&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;2_3&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; header_font=&#8221;||||||||&#8221; header_2_font=&#8221;ABeeZee||||||||&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h2><strong>Research: Solar Cells<\/strong><\/h2>\n<p>[\/et_pb_text][et_pb_text _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; text_font_size=&#8221;18px&#8221; text_line_height=&#8221;1.8em&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p>We believe that the best way to reduce the cost of photovoltaic (PV) energy is to improve efficiencies. This reduces both the cost of the solar cell per Watt generated, as well as reducing the installation cost, since fewer cells are required.<\/p>\n<p>We seek to complement traditional silicon solar cells with new technology that uses excitons to mediate the flow of energy. Mastering the properties of excitons offers the ability to guide energy at the nanoscale, and transform it with a flexibility that is impossible in conventional systems. For example, excitons have no net charge and can be split or combined. As an example, we have exploited this flexibility by using singlet exciton fission to generate multiple carriers in an organic solar cell at an efficiency of &gt; 1.26 electrons per photon, exceeding the unity limit in conventional electronic materials. The spintronics of excitons is key to our work. Indeed, the high efficiencies of singlet exciton fission arise because competing thermalization losses are spin disallowed.<\/p>\n<p>[\/et_pb_text][\/et_pb_column][et_pb_column type=&#8221;1_3&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_text][et_pb_text _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; text_font=&#8221;ABeeZee||||||||&#8221; text_font_size=&#8221;18px&#8221; custom_padding=&#8221;||||false|false&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p style=\"text-align: left;\">Main Research Areas<\/p>\n<p>[\/et_pb_text][et_pb_text _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; text_text_color=&#8221;#C5310D&#8221; text_font_size=&#8221;16px&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<div id=\"interiorcontentresearch\">\n<div id=\"interiorrightresearch\">\n<div id=\"interiorcontentresearch\">\n<div id=\"interiorrightresearch\">\n<div id=\"interiorcontentresearch\">\n<div id=\"interiorrightresearch\">\n<div id=\"interiorcontentresearch\">\n<div id=\"interiorrightresearch\">\n<p><a href=\"https:\/\/seegroup.mit.edu\/index.php\/solar-cells\/\" style=\"color: #c5310d !important; text-decoration: none;\" onmouseover=\"this.style.textDecoration='underline'\" onmouseout=\"this.style.textDecoration='none'\">Solar Cells<\/a><\/p>\n<p><a href=\"https:\/\/seegroup.mit.edu\/index.php\/light-emitting-devices\/\" style=\"color: #c5310d !important; text-decoration: none;\" onmouseover=\"this.style.textDecoration='underline'\" onmouseout=\"this.style.textDecoration='none'\">Light Emitting Devices<\/a><\/p>\n<p><a href=\"https:\/\/seegroup.mit.edu\/index.php\/gas-sensing\/\" style=\"color: #c5310d !important; text-decoration: none;\" onmouseover=\"this.style.textDecoration='underline'\" onmouseout=\"this.style.textDecoration='none'\">Gas Sensing<\/a><a href=\"https:\/\/seegroup.mit.edu\/index.php\/magnetic-domain-wall-devices\/\" style=\"text-decoration: none; color: #c5310d !important;\" onmouseover=\"this.style.textDecoration='underline'\" onmouseout=\"this.style.textDecoration='none'\"><\/a><\/p>\n<p><a style=\"color: #c5310d !important;\" href=\"https:\/\/seegroup.mit.edu\/index.php\/spintronics\/\">Spintronics for Computation<\/a><\/p>\n<p><a style=\"color: #c5310d !important;\" href=\"https:\/\/seegroup.mit.edu\/index.php\/research\/photon-upconversion-and-downconversion\/\">Photon Upconversion and Downconversion<\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h2><span style=\"font-size: large;\">Coupling excitonic materials to silicon, however, presents two important challenges. First, how can energy be communicated from excitons to silicon? Second, can silicon technologies efficiently collect that energy and convert it into charge?<\/span><\/h2>\n<h2><span style=\"font-size: large;\">Our approach is to directly couple materials that perform singlet exciton fission with silicon. The excitonic materials absorb light in the visible spectrum and split the energy into two spin 1, or triplet, excited states. In 2019, we observed evidence that these triplet excited states could be coupled to silicon surfaces across a thin (~ 1nm) interfacial layer of hafnium oxynitride (<a href=\"https:\/\/doi.org\/10.1038\/s41586-019-1339-4\">link<\/a>). More recently, we determined that the coupling was caused by separation of the triplet excited states into charge at defect states in the hafnium oxynitride (<a href=\"https:\/\/doi.org\/10.1002\/adma.202415110\">link<\/a>).<\/span><\/h2>\n<h2><span style=\"font-size: large;\">We are presently engineering interfaces to control energy transfer by introducing states to mediate interfacial charge separation. This approach has led to the first example of successful coupling of singlet exciton fission to silicon solar cells (<a href=\"https:\/\/doi.org\/10.48550\/arXiv.2407.21093\">link<\/a>).<\/span><\/h2>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=&#8221;1_2,1_2&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; width=&#8221;100%&#8221; max_width=&#8221;750px&#8221; module_alignment=&#8221;center&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;1_2&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_image src=&#8221;https:\/\/seegroup.mit.edu\/wp-content\/uploads\/2025\/03\/PMW09.png&#8221; title_text=&#8221;PMW09&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_image][\/et_pb_column][et_pb_column type=&#8221;1_2&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_image src=&#8221;https:\/\/seegroup.mit.edu\/wp-content\/uploads\/2025\/03\/pyramid13.png&#8221; title_text=&#8221;pyramid13&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; custom_padding=&#8221;|||0px||&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_image][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; min_height=&#8221;58.8px&#8221; custom_margin=&#8221;-35px||||false|false&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; max_width=&#8221;37%&#8221; module_alignment=&#8221;center&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><em>Figure: SEM images of singlet exciton fission coupled silicon solar cells<\/em><\/p>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=&#8221;1_2,1_2&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;1_2&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; text_font_size=&#8221;18px&#8221; text_line_height=&#8221;1.8em&#8221; min_height=&#8221;63.8px&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><a href=\"https:\/\/communities.springernature.com\/posts\/an-old-dream-for-silicon-solar-cells\">An old dream for silicon solar cells | Research Communities by Springer Nature<\/a><\/p>\n<p>[\/et_pb_text][et_pb_text _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; text_font_size=&#8221;18px&#8221; text_line_height=&#8221;1.8em&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p>Outlook<\/p>\n<p>By generating twice the current from the visible spectrum, exciton fission can increase the efficiency of silicon cells beyond their conventional \u2018single junction efficiency limit\u2019. Unlike other approaches, that require coupling a second solar cell to silicon, exciton fission preserves the simplicity of single junction silicon cells, promising a low-cost and readily-manufacturable path for the continued scaling of solar energy.<\/p>\n<p>[\/et_pb_text][et_pb_text _builder_version=&#8221;4.27.3&#8243; _module_preset=&#8221;default&#8221; text_font_size=&#8221;18px&#8221; text_line_height=&#8221;1.8em&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p>See our work on:<\/p>\n<p><a href=\"https:\/\/seegroup.mit.edu\/index.php\/glass-based-solar-concentrators\/\" style=\"font-size: 18px; background-color: #ffffff;\">Organic dye-based Luminescent Solar Concentrators<\/a><\/p>\n<p><a href=\"https:\/\/doi.org\/10.1038\/srep14758\">Solar powered lasers<\/a><\/p>\n<p><a href=\"https:\/\/doi.org\/10.1038\/ncomms7415\">Lowering recombination losses in organic solar cells\u00a0<\/a><\/p>\n<p><a href=\"https:\/\/doi.org\/10.1063\/1.4876600\">Singlet exciton fission in organic photodetectors and solar cells<\/a><\/p>\n<p>[\/et_pb_text][\/et_pb_column][et_pb_column type=&#8221;1_2&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_image src=&#8221;https:\/\/seegroup.mit.edu\/wp-content\/uploads\/2024\/10\/excitons1.png&#8221; title_text=&#8221;excitons1&#8243; _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_image][et_pb_text _builder_version=&#8221;4.21.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><em>Figure:\u00a0Unlike electrons, excitons can be split. In the Center for Excitonics, we have used singlet exciton fission in pentacene to generate at least 1.26 electrons per photon. From Baldo, Van Voorhis, et al. Science (2013) and APL (2013)<\/em><\/p>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section]<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Research: Solar CellsWe believe that the best way to reduce the cost of photovoltaic (PV) energy is to improve efficiencies. This reduces both the cost of the solar cell per Watt generated, as well as reducing the installation cost, since fewer cells are required. We seek to complement traditional silicon solar cells with new technology [&hellip;]<\/p>\n","protected":false},"author":3,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"class_list":["post-195","page","type-page","status-publish","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/pages\/195","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/comments?post=195"}],"version-history":[{"count":35,"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/pages\/195\/revisions"}],"predecessor-version":[{"id":943,"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/pages\/195\/revisions\/943"}],"wp:attachment":[{"href":"https:\/\/seegroup.mit.edu\/index.php\/wp-json\/wp\/v2\/media?parent=195"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}