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        <identifier>oai:figshare.com:article/34009122</identifier>
        <datestamp>2026-09-28T05:36:04Z</datestamp>
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          <dc:title>Supplementary file 1_Seamless triple-mode luminescence thermometry in Lu3(Al4Ga1)O12:Pr: high sensitivity from 11 to 700 K.docx</dc:title>
          <dc:creator>Justyna Zeler (9204949)</dc:creator>
          <dc:creator>Joanna Trojan-Piegza (25119738)</dc:creator>
          <dc:creator>Eugeniusz Zych (17632888)</dc:creator>
          <dc:subject>Organic Chemistry</dc:subject>
          <dc:subject>LuAGG:Pr</dc:subject>
          <dc:subject>luminescence thermometry</dc:subject>
          <dc:subject>multimodal thermometry</dc:subject>
          <dc:subject>Pr3+ spectroscopy</dc:subject>
          <dc:subject>wide range luminescence thermometry</dc:subject>
          <dc:description>&lt;p&gt;This study reports on the high-performance luminescence thermometry of a Lu&lt;sub&gt;3&lt;/sub&gt;(Al&lt;sub&gt;4&lt;/sub&gt;Ga&lt;sub&gt;1&lt;/sub&gt;)O&lt;sub&gt;12&lt;/sub&gt;:Pr (LuAGG:Pr) phosphor, demonstrating a remarkable operational range spanning from deep-cryogenic to high-temperature regimes (11–700 K). Its relative thermal sensitivity, S&lt;sub&gt;r&lt;/sub&gt;, remains between 0.7% and 6.5% K&lt;sup&gt;−1&lt;/sup&gt;, exceeding 1% K&lt;sup&gt;−1&lt;/sup&gt; over the vast majority of this interval. To overcome the sensitivity bottlenecks inherent to single-parameter thermometers, we propose a multi-mode thermometric strategy that leverages three distinct physical mechanisms. At cryogenic temperatures (11–120 K), the population redistribution among the Stark levels of the &lt;sup&gt;1&lt;/sup&gt;D&lt;sub&gt;2&lt;/sub&gt; state yields a maximum S&lt;sub&gt;r&lt;/sub&gt; of 6.5% K&lt;sup&gt;−1&lt;/sup&gt;. In the intermediate range (120–320 K), sensing is governed by the Boltzmann-coupled &lt;sup&gt;3&lt;/sup&gt;P&lt;sub&gt;1&lt;/sub&gt; and &lt;sup&gt;3&lt;/sup&gt;P&lt;sub&gt;0&lt;/sub&gt; states, yielding a maximum S&lt;sub&gt;r&lt;/sub&gt; of 5.5% K&lt;sup&gt;−1&lt;/sup&gt; when using the two-level emission ratio. Crucially, we demonstrate that the integration of the intensity ratio between the interconfigurational 5d→4f and &lt;sup&gt;1&lt;/sup&gt;D&lt;sub&gt;2&lt;/sub&gt;→&lt;sup&gt;3&lt;/sup&gt;H&lt;sub&gt;4&lt;/sub&gt; emissions - primarily driven by multiphonon relaxation - significantly enhances performance at elevated temperatures. While Boltzmann-type distributions show declining sensitivity above room temperature, this multiphonon-driven 5d/4f ratio revitalizes the sensor, maintaining S&lt;sub&gt;r&lt;/sub&gt; &gt; 1% K&lt;sup&gt;−1&lt;/sup&gt; up to 700 K, with S&lt;sub&gt;r&lt;/sub&gt; peak of 2.2% K&lt;sup&gt;−1&lt;/sup&gt; at 465 K. By strategically combining these three parameters, we achieve a continuous, high-sensitivity profile across the entire 11–700 K window, establishing LuAGG:Pr as one of the most versatile Pr&lt;sup&gt;3+&lt;/sup&gt; singly activated materials for advanced thermal sensing reported to date.&lt;/p&gt;</dc:description>
          <dc:date>2026-09-28T05:36:04Z</dc:date>
          <dc:type>Dataset</dc:type>
          <dc:type>Dataset</dc:type>
          <dc:identifier>10.3389/fchem.2026.1924671.s001</dc:identifier>
          <dc:relation>https://figshare.com/articles/dataset/Supplementary_file_1_Seamless_triple-mode_luminescence_thermometry_in_Lu3_Al4Ga1_O12_Pr_high_sensitivity_from_11_to_700_K_docx/34009122</dc:relation>
          <dc:rights>CC BY 4.0</dc:rights>
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