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<article article-type="research-article" dtd-version="2.3" xml:lang="EN" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mater.</journal-id>
<journal-title>Frontiers in Materials</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mater.</abbrev-journal-title>
<issn pub-type="epub">2296-8016</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">630046</article-id>
<article-id pub-id-type="doi">10.3389/fmats.2021.630046</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Materials</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Switchable Coumarins for Ratiometric pH Sensing</article-title>
<alt-title alt-title-type="left-running-head">Mazza et al.</alt-title>
<alt-title alt-title-type="right-running-head">Ratiometric Sensors</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Mazza</surname>
<given-names>Mercedes M. A.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Cardano</surname>
<given-names>Francesca</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<uri xlink:href="http://loop.frontiersin.org/people/1177819/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Baker</surname>
<given-names>James D.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Giordani</surname>
<given-names>Silvia</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<uri xlink:href="http://loop.frontiersin.org/people/304855/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Raymo</surname>
<given-names>Fran&#xe7;isco M.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="http://loop.frontiersin.org/people/2693/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<label>
<sup>1</sup>
</label>Departments of Chemistry and Biology, Laboratory for Molecular Photonics, University of Miami, <addr-line>Coral Gables</addr-line>, <addr-line>FL</addr-line>, <country>United States</country>
</aff>
<aff id="aff2">
<label>
<sup>2</sup>
</label>Nano Carbon Materials, Istituto Italiano di Tecnologia, <addr-line>Genoa</addr-line>, <country>Italy</country>
</aff>
<aff id="aff3">
<label>
<sup>3</sup>
</label>Department of Chemistry and Industrial Chemistry, University of Genoa, <addr-line>Genoa</addr-line>, <country>Italy</country>
</aff>
<aff id="aff4">
<label>
<sup>4</sup>
</label>School of Chemical Sciences, Dublin City University, <addr-line>Glasnevin</addr-line>, <country>Ireland</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/114400">Xun Yu</ext-link>, New York Institute of Technology, United States</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/472552">Lin Yuan</ext-link>, Hunan University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/227383">Maya Thanou</ext-link>, King&#x2019;s College London, United Kingdom</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Fran&#xe7;isco M. Raymo, <email>fraymo@miami.edu</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Smart Materials, a section of the journal Frontiers in Materials</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>15</day>
<month>02</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>8</volume>
<elocation-id>630046</elocation-id>
<history>
<date date-type="received">
<day>16</day>
<month>11</month>
<year>2020</year>
</date>
<date date-type="accepted">
<day>07</day>
<month>01</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2021 Mazza, Cardano, Baker, Giordani and Raymo.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Mazza, Cardano, Baker, Giordani and Raymo</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>A fluorescent chromophore and a pH-sensitive heterocycle were integrated within a single covalent skeleton to generate four molecular switches with ratiometric fluorescence response. Upon acidification, the pH-sensitive heterocycle opens to shift bathochromically the absorption and emission bands of the fluorescent chromophore. As a result, an equilibrium between two species with resolved fluorescence is established with fast kinetics in aqueous environments. The relative amounts of the two interconverting forms and their relative emission intensities change with pH, providing the opportunity to probe this parameter ratiometrically with fluorescence measurements. Specifically, the resolved emissions of the two species can be collected in separate detection channels of the same microscope to map their ratio across a labeled sample and reconstruct its pH distribution ratiometrically with spatial resolution at the micrometer level. Additionally, the sensitivity of these molecular switches varies with the nature of the heterocyclic ring and with its substituents, allowing the possibility of regulating their response to a given pH range of interest with the aid of chemical synthesis. Thus, a family of valuable fluorescent probes for ratiometric pH sensing in a diversity of samples can emerge from the unique combination of structural and photophysical properties designed into our innovative molecular switches.</p>
</abstract>
<kwd-group>
<kwd>coumarins</kwd>
<kwd>fluorescence imaging</kwd>
<kwd>molecular switches</kwd>
<kwd>oxazines</kwd>
<kwd>oxazolidines</kwd>
<kwd>pH sensors</kwd>
<kwd>ratiometric sensors</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>The quantitative determination of pH in the intracellular space can provide invaluable information on the many processes responsible for regulating cell functions (<xref ref-type="bibr" rid="B30">Weisz, 2003</xref>; <xref ref-type="bibr" rid="B2">Boron 2004</xref>; <xref ref-type="bibr" rid="B3">Casey et al., 2010</xref>). However, the microscaled dimensions of cells in conjunction with the need to ensure minimal structural perturbations restrict the number of analytical methods compatible with these measurements significantly (<xref ref-type="bibr" rid="B16">Loiselle and Casey, 2010</xref>; <xref ref-type="bibr" rid="B6">Demuth et al., 2016</xref>). In this context, the noninvasive character, micrometer resolution, fast response, and inherent sensitivity of fluorescence measurements (<xref ref-type="bibr" rid="B14">Lakowicz, 2006</xref>) and optical microscopy (<xref ref-type="bibr" rid="B18">Murphy, 2001</xref>) are particularly convenient. Indeed, membrane-permeable dyes with pH-sensitive emission can be exploited to probe pH in the cytosol and in specific organelles of live cells (<xref ref-type="bibr" rid="B10">Han and Burgess, 2010</xref>; <xref ref-type="bibr" rid="B28">Wang et al., 2010</xref>; <xref ref-type="bibr" rid="B15">Li et al., 2014</xref>; <xref ref-type="bibr" rid="B19">Ni and Wu, 2014</xref>; <xref ref-type="bibr" rid="B11">Hou et al., 2017</xref>; <xref ref-type="bibr" rid="B23">Specht et al., 2017</xref>). Generally, the fluorescence quantum yield of the sensitive molecular probe is designed to change with pH; therefore, the emission intensity measured in a given intracellular region of interest can be correlated quantitatively with pH. Nonetheless, concentration and optical effects can also influence the magnitude of the detected emission intensity, complicating the quantitative determination of pH. These limitations can be overcome with ratiometric measurements, if the sensitive dye is engineered to produce dual emission in resolved spectral windows (<xref ref-type="bibr" rid="B12">Huang et al., 2018</xref>; <xref ref-type="bibr" rid="B1">Bigdeli et al., 2019</xref>). Under these conditions, the intensity of one emission can be measured relative to the other in order to eliminate any concentration or optical artifact. In addition to the inherent challenge in designing molecular constructs with dual emission, a further complication in the development of such ratiometric probes arises from the need to adjust their sensitivity to a relatively wide range of pH values. In fact, the pH in the intracellular environment can vary from <italic>ca.</italic> 4 in the acidic lysosomal compartments to as much as <italic>ca.</italic> 8 in the basic mitochondria (<xref ref-type="bibr" rid="B30">Weisz, 2003</xref>; <xref ref-type="bibr" rid="B2">Boron 2004</xref>; <xref ref-type="bibr" rid="B3">Casey et al., 2010</xref>). Thus, modular structural designs that can easily be modified with the aid of chemical synthesis to ensure ratiometric fluorescence response and tunable pH sensitivity would be especially valuable.</p>
<p>Our laboratories identified a mechanism to activate the fluorescence of a coumarin fluorophore in response to pH (<xref ref-type="bibr" rid="B8">Deniz et al., 2012</xref>; <xref ref-type="bibr" rid="B24">Swaminathan et al., 2012</xref>). It is based on the opening of a 2<italic>H</italic>,4<italic>H</italic>-benzo [1,3]oxazine (oxazine) ring upon acidification with the concomitant bathochromic shift in the coumarin absorption. Selective excitation of the protonated species then results in intense fluorescence at <italic>ca.</italic> 660&#xa0;nm. Furthermore, the covalent connection of such a pH-activatable probe to folate ligands allows the activation of fluorescence in acidic endosomal compartments of cancer cells and their discrimination from normal cells (<xref ref-type="bibr" rid="B26">Tang et al., 2017</xref>). However, a significant increase in emission intensity is observed only at pH values lower than <italic>ca.</italic> 5. The need to tune the pH sensitivity of this molecular probe and impose ratiometric response on it suggested the possibility of exploring structural modifications of the original oxazine heterocycle and extending these operating principles to 2<italic>H</italic>,3<italic>H</italic>,4<italic>H</italic>,5<italic>H</italic>-[1,3]oxazole (oxazolidine) rings, which are also known to open in response to acidification (<xref ref-type="bibr" rid="B25">Szal&#xf3;ki et al., 2015</xref>; <xref ref-type="bibr" rid="B9">Fujioka et al., 2020</xref>). This article reports a detailed spectroscopic analysis of four members of this family of molecular switches together with representative imaging experiments in model preparations.</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<title>Materials and Methods</title>
<sec id="s2-1">
<title>General Procedures</title>
<p>Chemicals were purchased from commercial sources and used as received. H<sub>2</sub>O (18.2&#xa0;M&#x3a9;&#xa0;cm) was purified with a Barnstead International Nanopure Diamond Analytical system. Compounds <bold>1, 3, 5&#x2013;9, and 11</bold> (<xref ref-type="sec" rid="s9">Supplementary Figures S1,S2</xref>) were prepared according to literature procedures (<xref ref-type="bibr" rid="B31">Wu et al., 2007</xref>; <xref ref-type="bibr" rid="B27">Tomasulo et al., 2008</xref>; <xref ref-type="bibr" rid="B7">Deniz et al., 2010</xref>; <xref ref-type="bibr" rid="B33">Zhang et al., 2015</xref>; <xref ref-type="bibr" rid="B17">Mazza et al., 2019</xref>; <xref ref-type="bibr" rid="B29">Wang et al., 2020</xref>). Electrospray ionization mass spectra (ESIMS) were recorded with a Bruker micrOTOF-Q spectrometer. Nuclear magnetic resonance (NMR) spectra were recorded with a Bruker Avance 400 spectrometer. Absorption spectra were recorded in aerated quartz cells (path length &#x3d; 1.0&#xa0;cm) with a Varian Cary 100 Bio spectrometer, equipped with an Agilent Technology Cary Dual Cell Peltier accessory. Emission spectra were recorded in aerated quartz cells (path length &#x3d; 1.0&#xa0;cm) with a Varian Cary Eclipse spectrometer, equipped with a Varian Cary Single Cell Peltier accessory. Fluorescence quantum yields were determined against 9,10-diphenylanthracene (<bold>2Cl</bold> and <bold>4Cl</bold>) and cresyl violet (<bold>2OpH</bold> and <bold>4OpH</bold>), following a literature protocol (<xref ref-type="bibr" rid="B32">W&#xfc;rth et al., 2013</xref>). Fluorescence images were recorded with a Leica SP5 laser-scanning confocal microscope. Dynamic light scattering (DLS) measurements were performed with a Malvern Zen1600 apparatus.</p>
</sec>
<sec id="s2-2">
<title>Synthesis of 2</title>
<p>Trifluoroacetic acid (TFA, 160&#xa0;&#x3bc;L, 2.09&#xa0;mmol) was added dropwise to a solution of <bold>6</bold> (100&#xa0;mg, 0.32&#xa0;mmol) and <bold>7</bold> (79&#xa0;mg, 0.32&#xa0;mmol) in EtOH (10&#xa0;ml). The mixture was heated under reflux for 24&#xa0;h. After cooling down to ambient temperature, the solvent was distilled under reduced pressure and the residue was dissolved in CH<sub>2</sub>Cl<sub>2</sub> (50&#xa0;ml) and washed with NaHCO<sub>3</sub> (5% w/v, 20&#xa0;ml) and H<sub>2</sub>O (20&#xa0;ml). The organic phase was dried over anhydrous Na<sub>2</sub>SO<sub>4</sub> and filtered and the solvent was distilled under reduced pressure. The residue was purified by column chromatography [SiO<sub>2</sub>, CH<sub>2</sub>Cl<sub>2</sub>/MeOH (98:2, v/v)] to give <bold>2</bold> (9%, 15&#xa0;mg) as a green solid. ESIMS: <italic>m/z</italic> &#x3d; 538.2359 [M &#x2b; H]<sup>&#x2b;</sup> (<italic>m/z</italic> calcd. for C<sub>32</sub>H<sub>32</sub>N<sub>3</sub>O<sub>5</sub> &#x3d; 538.2342); <sup>1</sup>H NMR (400&#xa0;MHz, CD<sub>3</sub>CN): &#x3b4; (ppm) &#x3d; 7.81 (s, 1H), 7.64&#x2013;7.66 (d, 8&#xa0;Hz, 1H), 7.28&#x2013;7.35 (m, 2H), 7.17&#x2013;7.19 (d, 5&#xa0;Hz, 2H), 6.98&#x2013;7.09 (m, 2H), 6.82&#x2013;6.89 (m, 1H), 6.77&#x2013;6.79 (m, 1H), 6.67&#x2013;6.72 (m, 2H), 6.51 (s, 1H), 5.02 (d, 19Hz, 1H), 4.78 (d, 19Hz, 1H), 3.41&#x2013;3.46 (m 4H), 1.52 (s, 3H), 1.16&#x2013;1.19 (m, 9H); <sup>13</sup>C NMR (100&#xa0;MHz, CD<sub>3</sub>CN): &#x3b4; (ppm) &#x3d; 183.5, 174.3, 137.5, 131.6, 130.5, 129.4, 128.1, 127.5, 126.5, 125.0, 123.1, 122.4, 122.2, 120.4, 109.3, 108.9, 100.1, 80.1, 55.0, 44.6, 38.7, 25.2, 17.8, 11.9.</p>
</sec>
<sec id="s2-3">
<title>Synthesis of 4</title>
<p>Palladium(II) acetate (18&#xa0;mg, 0.07&#xa0;mmol) was added to a solution of <bold>10</bold> (40&#xa0;mg, 0.07&#xa0;mmol) and <bold>11</bold> (20&#xa0;mg, 0.14&#xa0;mmol) in Et<sub>3</sub>N (20&#xa0;ml). The mixture was heated under reflux and Ar for 24&#xa0;h. After cooling down to ambient temperature, the reaction mixture was diluted with CH<sub>2</sub>Cl<sub>2</sub> (20&#xa0;ml) and washed with H<sub>2</sub>O (2 &#xd7; 20&#xa0;ml). The organic phase was dried over anhydrous Na<sub>2</sub>SO<sub>4</sub> and filtered and the solvent was distilled under reduced pressure. The residue was purified by column chromatography [SiO<sub>2</sub>, CH<sub>2</sub>Cl<sub>2</sub>/MeOH (93:7, v/v) and Et<sub>3</sub>N (1% v/v)] to give <bold>4</bold> (25%, 10&#xa0;mg) as a green solid. ESIMS: <italic>m/z</italic> &#x3d; 563.2888 [M &#x2b; H]<sup>&#x2b;</sup> (<italic>m/z</italic> calcd. for C<sub>36</sub>H<sub>39</sub>N<sub>2</sub>O<sub>4</sub> &#x3d; 563.2910); <sup>1</sup>H NMR (400&#xa0;MHz, CDCl<sub>3</sub>): &#x3b4; (ppm) &#x3d; 7.60 (s, 1H), 7.44 (d, 8&#xa0;Hz, 2H), 7.24&#x2013;7.31 (m, 4H), 6.96 (s, 1H), 6.87&#x2013;6.92 (m, 2H), 6.75&#x2013;6.81 (m, 2H), 6.65&#x2013;6.72 (m, 1H), 6.59 (d, Hz, 1H), 6.51 (s, 1H), 4.30 (m, 1H), 3.81&#x2013;3.85 (m, 4H), 3.66&#x2013;3.67 (m, 2H), 3.41&#x2013;3.49 (m, 4H), 1.49 (s, 3H), 1.25&#x2013;1.23 (t, 6H), 1.19 (s, 3H); <sup>13</sup>C NMR (100&#xa0;MHz, CDCl<sub>3</sub>): &#x3b4; (ppm) &#x3d; 161.1, 158.8, 155.8, 150.6, 150.5, 140.4, 139.5, 131.6, 130.8, 128.8, 127.8, 127.3, 127.1, 126.8, 126.5, 125.5, 120.2, 117.1, 114.2, 112.1, 110.5, 109.1, 108.9, 97.2, 63.5, 55.3, 50.1, 47.9, 44.8, 28.6, 20.4, 12.5.</p>
</sec>
<sec id="s2-4">
<title>Synthesis of 9</title>
<p>2-Bromoethanol (298&#xa0;&#x3bc;L, 4.21&#xa0;mmol) was added dropwise to a solution of <bold>8</bold> (1&#xa0;g, 3.51&#xa0;mmol) in MeCN (10&#xa0;ml). The mixture was heated under reflux and Ar for 24&#xa0;h. After cooling down to ambient temperature, the solvent was distilled under reduced pressure and the residue was dissolved in hexane (10&#xa0;ml), sonicated for 30&#xa0;min, and filtered. The residue was dissolved in CH<sub>2</sub>Cl<sub>2</sub> (50&#xa0;ml) and stored in a fridge for 2&#xa0;h. The resulting precipitate was filtered off, washed with CH<sub>2</sub>Cl<sub>2</sub> (20&#xa0;ml), and dried to give <bold>9</bold> (63%, 910&#xa0;mg) as a pink solid. ESIMS: <italic>m/z</italic> &#x3d; 330.0349 [M&#x2013;Br]<sup>&#x2b;</sup> (<italic>m/z</italic> calcd. for C<sub>13</sub>H<sub>17</sub>INO &#x3d; 330.0355); <sup>1</sup>H NMR (400&#xa0;MHz, CD<sub>3</sub>CN): &#x3b4; (ppm) &#x3d; 8.13 (s, 1H), 7.99 (d, 8&#xa0;Hz, 1H), 7.59 (d, 8&#xa0;Hz, 1H), 4.52 (t, 5&#xa0;Hz, 2H), 3.99 (t, 5&#xa0;Hz, 2H), 2.79 (s, 3H), 1.58 (s, 6H).</p>
</sec>
<sec id="s2-5">
<title>Synthesis of 10</title>
<p>TFA (209&#xa0;&#x3bc;L, 2.65&#xa0;mmol) was added dropwise to a solution of <bold>7</bold> (100&#xa0;mg, 0.41&#xa0;mmol) and <bold>9</bold> (167&#xa0;mg, 0.41&#xa0;mmol) in EtOH (8&#xa0;ml). The mixture was heated under reflux for 24&#xa0;h. After cooling down to ambient temperature, the solvent was distilled under reduced pressure and the residue was dissolved in CH<sub>2</sub>Cl<sub>2</sub> (5&#xa0;ml). The addition of Et<sub>2</sub>O (200&#xa0;ml) and refrigeration for 12&#xa0;h resulted in the formation of a precipitate. After filtration, the solid residue was dissolved in aqueous NaHCO<sub>3</sub> (5% w/v, 20&#xa0;ml) and stirred for 1&#xa0;h at ambient temperature. The aqueous mixture was extracted with EtOAc (3 &#xd7; 40&#xa0;ml). The organic phase was dried over anhydrous Na<sub>2</sub>SO<sub>4</sub> and filtered and the solvent was distilled off under reduced pressure to give <bold>10</bold> as a green solid (22%, 50&#xa0;mg). ESIMS: <italic>m/z</italic> &#x3d; 557.1293 [M &#x2b; H]&#x2b;(<italic>m/z</italic> calcd. for C<sub>27</sub>H<sub>30</sub>IN<sub>2</sub>O<sub>3</sub> &#x3d; 557.1301); <sup>1</sup>H NMR (400&#xa0;MHz, CDCl<sub>3</sub>): &#x3b4; (ppm) &#x3d; 7.59 (s, 1H), 7.45 (d, 8&#xa0;Hz, 1H), 7.34 (s, 1H), 7.25&#x2013;7.30 (m, 1H), 6.79 (d, 8&#xa0;Hz, 1H), 6.64 (d, 17&#xa0;Hz, 1H), 6.56&#x2013;6.63 (m, 2H), 6.51 (s, 1H), 4.13 (q, 7&#xa0;Hz, 1H), 3.76&#x2013;3.82 (m, 1H), 3.54&#x2013;3.67 (m, 2H), 3.41&#x2013;3.46 (m, 4H), 1.42 (s, 3H), 1.27&#x2013;1.21 (m, 6H), 1.17 (s, 3H).</p>
</sec>
<sec id="s2-6">
<title>Preparation of Doped Nanoparticles and Beads</title>
<p>CH<sub>2</sub>Cl<sub>2</sub> solutions of <bold>1&#x2013;4</bold> (0.4&#x2013;3.1 mM, 10&#xa0;&#xb5;L) were individually mixed with a CH<sub>2</sub>Cl<sub>2</sub> solution of Pluronic 123 (2.5&#xa0;mg&#xa0;ml<sup>&#x2212;1</sup>, 600&#xa0;&#xb5;L) and stirred for 15&#xa0;min at ambient temperature. The solvent was distilled off under reduced pressure. The residue was dissolved in H<sub>2</sub>O (1&#xa0;ml) for spectroscopic measurements or in an aqueous solution of sodium alginate (4% w/v, 2&#xa0;ml) for imaging experiments. DLS measurements revealed the hydrodynamic diameter of the doped polymer nanoparticles to be <italic>ca.</italic> 80&#xa0;nm. Droplets of the resulting mixture of sodium alginate and polymer nanoparticles were added to an aqueous solution of CaCl<sub>2</sub> (0.24 M, 750&#xa0;&#xb5;L) with a syringe through a 25-gauge needle. Beads with diameters of a few millimeters formed upon contact of the droplets with the CaCl<sub>2</sub> solution. After 2&#xa0;min, individual beads were suspended in H<sub>2</sub>O (500&#xa0;&#xb5;L) at different pH, ranging from 7.4 to 4.0, and then transferred to a glass Petri dish.</p>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>Results</title>
<p>Compounds <bold>1Cl</bold> and <bold>2Cl</bold> incorporate an oxazine heterocycle and differ in the position of a nitro substituent (<xref ref-type="fig" rid="F1">Figure 1</xref>). Compounds <bold>3Cl</bold> and <bold>4Cl</bold> have an oxazolidine heterocycle in place of the oxazine ring and differ in the substituent on 2<italic>H</italic>,3<italic>H</italic>-indole (indole) heterocycle. Compounds <bold>1Cl</bold> and <bold>3Cl</bold> were prepared according to literature protocols (<xref ref-type="bibr" rid="B7">Deniz et al., 2010</xref>; <xref ref-type="bibr" rid="B17">Mazza et al., 2019</xref>). Compounds <bold>2Cl</bold> and <bold>4Cl</bold> were synthesized in one and three steps, respectively (<xref ref-type="sec" rid="s9">Supplementary Figures S1,S2</xref>), and their structural identities were confirmed by high-resolution ESIMS and <sup>1</sup>H NMR spectroscopy.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Interconversion of the ring-closed (Cl) and protonated ring-open (OpH) forms of <bold>1&#x2013;4</bold>.</p>
</caption>
<graphic xlink:href="fmats-08-630046-g001.tif"/>
</fig>
<p>The absorption spectra (<xref ref-type="fig" rid="F2">Figures 2</xref>, <xref ref-type="fig" rid="F3">3</xref>) of acetonitrile solutions of <bold>1Cl&#x2013;4Cl</bold> show an intense band at 399&#x2013;412&#xa0;nm (<sup>Cl</sup>&#x3bb;<sub>Ab</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) associated with the coumarin chromophore in all instances. Upon addition of increasing amounts of trifluoroacetic acid (TFA), this absorption decreases in intensity with the concomitant appearance and growth of a new band at 576&#x2013;594&#xa0;nm (<sup>OpH</sup>&#x3bb;<sub>Ab</sub> in <xref ref-type="table" rid="T1">Table 1</xref>). This additional absorption resembles that of model compound <bold>5</bold> (<xref ref-type="sec" rid="s9">Supplementary Figure S3</xref>) and is indicative of the opening and protonation of the oxazine or oxazolidine heterocycle to form <bold>1OpH</bold>&#x2013;<bold>4OpH</bold>. Indeed, this structural transformation converts the carbon atom at the junction of the indole and either the oxazine or the oxazolidine heterocycle from sp<sup>3</sup> to sp<sup>2</sup> and brings the coumarin component in conjugation with the resulting 3<italic>H</italic>-indolium cation. As a result of the extended electronic delocalization, the main absorption of the coumarin chromophore shifts bathochromically, in agreement with literature on related compounds (<xref ref-type="bibr" rid="B8">Deniz et al., 2012</xref>; <xref ref-type="bibr" rid="B24">Swaminathan et al., 2012</xref>; <xref ref-type="bibr" rid="B26">Tang et al., 2017</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Absorption <bold>(<italic>a</italic>)</bold> and emission (<bold>
<italic>b</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 405&#xa0;nm; <bold>
<italic>c</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 575&#xa0;nm) spectra of a MeCN solution of <bold>1</bold> (22&#xa0;&#xb5;M) recorded before (black) and after (red) the addition of increasing amounts of TFA (0.1&#x2013;1.8 eq.). Absorption <bold>(<italic>d</italic>)</bold> and emission (<bold>
<italic>e</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 405&#xa0;nm; <bold>
<italic>f</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 575&#xa0;nm) spectra of a MeCN solution of <bold>2</bold> (7&#xa0;&#xb5;M) recorded before (black) and after (red) the addition of increasing amounts of TFA (0.1&#x2013;1.8 eq.).</p>
</caption>
<graphic xlink:href="fmats-08-630046-g002.tif"/>
</fig>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Absorption <bold>(<italic>a</italic>)</bold> and emission (<bold>
<italic>b</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 405&#xa0;nm; <bold>
<italic>c</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 575&#xa0;nm) spectra of a MeCN solution of <bold>3</bold> (6&#xa0;&#xb5;M) recorded before (black) and after (red) the addition of increasing amounts of TFA (0.1&#x2013;1.1 eq.). Absorption <bold>(<italic>d</italic>)</bold> and emission (<bold>
<italic>e</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 405&#xa0;nm; <bold>
<italic>f</italic>
</bold>, &#x3bb;<sub>Ex</sub> &#x3d; 575&#xa0;nm) spectra of a MeCN solution of <bold>4</bold> (11&#xa0;&#xb5;M) recorded before (black) and after (red) the addition of increasing amounts of TFA (0.1&#x2013;1.1 eq.).</p>
</caption>
<graphic xlink:href="fmats-08-630046-g003.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Photophysical parameters for 1&#x2013;4 [a].</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left"/>
<th align="center">
<italic>Solvent</italic>
</th>
<th align="center">
<sup>Cl</sup>&#x3bb;<sub>Ab</sub> (nm)</th>
<th align="center">
<sup>Cl</sup>&#x3bb;<sub>Em</sub> (nm)</th>
<th align="center">
<sup>Cl</sup>&#x3d5;</th>
<th align="center">
<sup>OpH</sup>&#x3bb;<sub>Ab</sub> (nm)</th>
<th align="center">
<sup>OpH</sup>&#x3bb;<sub>Em</sub> (nm)</th>
<th align="center">
<sup>OpH</sup>&#x3d5;</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">
<bold>1</bold>
</td>
<td align="center">MeCN</td>
<td align="center">412</td>
<td align="center">480</td>
<td align="center">0.01</td>
<td align="center">594</td>
<td align="center">661</td>
<td align="center">0.02</td>
</tr>
<tr>
<td align="left"/>
<td align="center">H<sub>2</sub>O</td>
<td align="center">412</td>
<td align="center">472</td>
<td align="center">0.12</td>
<td align="center">593</td>
<td align="center">649</td>
<td align="center">0.53</td>
</tr>
<tr>
<td align="left">
<bold>2</bold>
</td>
<td align="center">MeCN</td>
<td align="center">399</td>
<td align="center">454</td>
<td align="center">0.02</td>
<td align="center">588</td>
<td align="center">654</td>
<td align="center">0.20</td>
</tr>
<tr>
<td align="left"/>
<td align="center">H<sub>2</sub>O</td>
<td align="center">401</td>
<td align="center">478</td>
<td align="center">0.02</td>
<td align="center">565</td>
<td align="center">647</td>
<td align="center">0.20</td>
</tr>
<tr>
<td align="left">
<bold>3</bold>
</td>
<td align="center">MeCN</td>
<td align="center">402</td>
<td align="center">476</td>
<td align="center">0.98</td>
<td align="center">576</td>
<td align="center">647</td>
<td align="center">0.21</td>
</tr>
<tr>
<td align="left"/>
<td align="center">H<sub>2</sub>O</td>
<td align="center">398</td>
<td align="center">465</td>
<td align="center">0.98</td>
<td align="center">576</td>
<td align="center">644</td>
<td align="center">0.13</td>
</tr>
<tr>
<td align="left">
<bold>4</bold>
</td>
<td align="center">MeCN</td>
<td align="center">400</td>
<td align="center">476</td>
<td align="center">0.30</td>
<td align="center">594</td>
<td align="center">666</td>
<td align="center">0.13</td>
</tr>
<tr>
<td align="left"/>
<td align="center">H<sub>2</sub>O</td>
<td align="center">398</td>
<td align="center">466</td>
<td align="center">0.55</td>
<td align="center">608</td>
<td align="center">671</td>
<td align="center">0.08</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>[a] Wavelengths at the absorption (<sup>Cl</sup>&#x3bb;<sub>Ab</sub> and <sup>OpH</sup>&#x3bb;<sub>Ab</sub>) and emission (<sup>Cl</sup>&#x3bb;<sub>Em</sub> and <sup>OpH</sup>&#x3bb;<sub>Em</sub>) maxima and fluorescence quantum yield (<sup>Cl</sup>&#x3d5; and <sup>OpH</sup>&#x3d5;) of the ring-closed (<bold>Cl</bold>) and protonated ring-open (<bold>OpH</bold>) forms of <bold>1</bold>&#x2013;<bold>4</bold>. The data listed for OpH in MeCN were measured after the addition of TFA (0.75 eq.) to a solution of the corresponding ring-closed form. The data listed for <bold>Cl</bold> and <bold>OpH</bold> in H<sub>2</sub>O were measured in the presence of Pluronic 123 (1.5&#xa0;mg&#xa0;mL<sup>&#x2212;1</sup>) at a pH of 7.5 and 3.0, respectively.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<p>The emission spectra (<xref ref-type="fig" rid="F2">Figures 2</xref>, <xref ref-type="fig" rid="F3">3</xref>) of acetonitrile solutions of <bold>1Cl</bold>&#x2013;<bold>4Cl</bold> reveal an intense band at 454&#x2013;480&#xa0;nm (<sup>Cl</sup>&#x3bb;<sub>Em</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) for the coumarin chromophore in all instances. However, the fluorescence quantum yields (<sup>Cl</sup>&#x3d5; in <xref ref-type="table" rid="T1">Table 1</xref>) of the oxazine derivatives are significantly lower than those of the oxazolidine counterparts. Upon acidification, this emission band decreases in intensity with the concomitant appearance and growth of a new band at 647&#x2013;666&#xa0;nm (<sup>OpH</sup>&#x3bb;<sub>Em</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) for <bold>1OpH&#x2013;4OpH</bold>. Once again, the fluorescence quantum yields (<sup>OpH</sup>&#x3d5; in <xref ref-type="table" rid="T1">Table 1</xref>) of the oxazine derivatives are significantly lower than those of the oxazolidine counterparts. Presumably, electron transfer from the excited coumarin chromophore to the nitro group is responsible for suppressing the ability of the ring-closed and protonated ring-open forms of <bold>1</bold> and <bold>2</bold> to be emitted.</p>
<p>Compounds <bold>1Cl&#x2013;4Cl</bold> are relatively hydrophobic and essentially insoluble in aqueous environments. However, they readily dissolve in the presence of appropriate amounts (&#x3e;1&#xa0;mg&#xa0;mL<sup>&#x2212;1</sup>) of Pluronic 123 and retain their photophysical properties as long as their concentration is maintained in the micromolar regime (&#x3c;50&#xa0;&#x3bc;M) to avoid aggregation. Indeed, this particular amphiphilic polymer is known to form micelles capable of capturing hydrophobic molecules in their interior and solubilizing them in aqueous environments (<xref ref-type="bibr" rid="B20">Pitto-Barry and Barry, 2015</xref>; <xref ref-type="bibr" rid="B13">Jarak et al., 2020</xref>). Consistently, DLS measurements on the resulting solutions indicate the formation of nanoparticles with an average hydrodynamic diameter of <italic>ca.</italic> 80&#xa0;nm in all instances. Absorption spectra (<xref ref-type="sec" rid="s9">Supplementary Figures S4,S5</xref>), recorded at different pH values, are consistent with the spectral changes observed in acetonitrile upon acidification (<xref ref-type="fig" rid="F2">Figures 2</xref>,<xref ref-type="fig" rid="F3">3</xref>). Specifically, the absorption band of the ring-closed form at 398&#x2013;412&#xa0;nm (<sup>Cl</sup>&#x3bb;<sub>Ab</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) decreases and that of the protonated ring-open form at 565&#x2013;608&#xa0;nm (<sup>OpH</sup>&#x3bb;<sub>Ab</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) increases upon acidification in all instances. Analyses of the pH dependence of the absorbance at <sup>OpH</sup>&#x3bb;<sub>Ab</sub> suggest that p<italic>K</italic>
<sub>a</sub> is 5.15 for 1; 3.51 for 2; 5.97 for <bold>3;</bold> 5.28 for <bold>4</bold>. Comparison of the values estimated for <bold>1</bold> and <bold>2</bold> demonstrates that the relocation of the nitro group from the <italic>para</italic>- to the <italic>meta</italic>-position, relative to the oxygen atom, on the phenylene ring fused to the oxazine heterocycle hinders protonation and ring opening. Comparison of the values determined for <bold>1</bold> and <bold>3</bold> shows that the transition from an ozaxine to an oxazolidine ring has instead the opposite effect.</p>
<p>The pH dependence of the equilibrium between the ring-closed and protonated ring-open forms of <bold>1 to 4</bold>, evident from the absorption spectra, translates into dual emission (<xref ref-type="sec" rid="s9">Supplementary Figures S4,S5</xref>). Specifically, the emission band of one species at 465&#x2013;478&#xa0;nm (<sup>Cl</sup>&#x3bb;<sub>Em</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) decreases and that of the other at 647&#x2013;671&#xa0;nm (<sup>OpH</sup>&#x3bb;<sub>Em</sub> in <xref ref-type="table" rid="T1">Table 1</xref>) increases with acidification in all instances, consistently with the behavior observed in acetonitrile (<xref ref-type="fig" rid="F2">Figures 2</xref>, <xref ref-type="fig" rid="F3">3</xref>). As a result, the ratio between the emission intensities of the ring-closed form (<italic>I</italic>
<sub>Cl</sub>) and that of the protonated ring-open species (<italic>I</italic>OpH) increase monotonically with a rise in pH. The corresponding plots (<xref ref-type="fig" rid="F4">Figure 4</xref>) show that <bold>1, 3</bold>, and <bold>4</bold> respond to pH predominantly between values of <italic>ca.</italic> 4 and <italic>ca.</italic> 8. The largest change in the magnitude of the ratio between the two emission intensities is observed for <bold>4</bold>. Instead, <bold>2</bold> responds to pH predominantly between values of <italic>ca.</italic> 2 and <italic>ca.</italic> 5, demonstrating that the position of the nitro group on the benzoxazine heterocycle has a pronounced influence on the equilibrium between two interconverting species. These observations suggest that the nature and position of the substituents on the pH-sensitive benzoxazine ring can be exploited to tune the response of these molecular switches.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>pH dependence of the ratio between the emission intensities of <bold>Cl</bold> and <bold>OpH</bold> (&#x3bb;<sub>Ex</sub> &#x3d; 405 or 575&#xa0;nm) for aqueous solutions of <bold>1</bold>&#x2013;<bold>4</bold> (2&#x2013;8&#xa0;&#xb5;M) and Pluronic 123 (1.5&#xa0;mg&#xa0;ml<sup>&#x2212;1</sup>).</p>
</caption>
<graphic xlink:href="fmats-08-630046-g004.tif"/>
</fig>
<p>The resolved emission bands of the ring-closed and protonated ring-open forms of <bold>1&#x2010;4</bold> provide, in principle, the opportunity to probe pH ratiometrically with the acquisition of fluorescence images in separate detection channels of the same microscope. Alginate hydrogels are optimal biocompatible model systems (<xref ref-type="bibr" rid="B22">Seliktar 2012</xref>; <xref ref-type="bibr" rid="B21">Rosales and Anseth, 2016</xref>; <xref ref-type="bibr" rid="B34">Zhang and Khademhosseini, 2017</xref>) to explore these possibilities and allow the identification of appropriate imaging conditions to capture and differentiate the fluorescence of the two interconverting species. Specifically, alginate beads of millimeter dimensions can be doped with nanoparticles of Pluronic 123 containing <bold>4</bold>, dispersed in water with a given pH, and imaged. The fluorescence of <bold>4Cl</bold> can be collected between 450 and 600&#xa0;nm (yellow channel in <xref ref-type="fig" rid="F5">Figure 5</xref>) and that of <bold>4OpH</bold> can be recorded between 600 and 770&#xa0;nm (green channel in <xref ref-type="fig" rid="F5">Figure 5</xref>). The resulting images show a fluorescence increase in the yellow channel <bold>(<italic>a&#x2013;d</italic>
</bold> in <xref ref-type="fig" rid="F5">Figure 5</xref>) with a concomitant emission decrease in the green channel (<bold>
<italic>e</italic>
</bold>&#x2013;<bold>
<italic>h</italic>
</bold> in <xref ref-type="fig" rid="F5">Figure 5</xref>) as the pH rises from 4.0 to 7.4. Plots (<bold>
<italic>i</italic>
</bold> in <xref ref-type="fig" rid="F5">Figure 5</xref>) of the emission intensities measured in the two channels further confirm that they are pH-dependent. In fact, the ratio (<bold>
<italic>j</italic>
</bold> in <xref ref-type="fig" rid="F5">Figure 5</xref>) between them increases monotonically with pH, by analogy with the spectroscopic measurements (<xref ref-type="fig" rid="F4">Figure 4</xref>), providing the opportunity to quantify this parameter ratiometrically. Additionally, storage of the sample at a fixed pH does not cause any change in the detected intensities (<xref ref-type="sec" rid="s9">Supplementary Figure S6</xref>), demonstrating that the sensitive probes neither undergo hydrolytic degradation nor photobleaching under these experimental conditions.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Fluorescence images (scale bar &#x3d; 200&#xa0;&#x3bc;m) of four alginate beads doped with Pluronic 123 nanoparticles (1.5&#xa0;mg&#xa0;mL<sup>&#x2212;1</sup>) containing <bold>4</bold> (5&#xa0;&#x3bc;M) and maintained in H<sub>2</sub>O at pH of 4.0 (<bold>
<italic>a</italic>
</bold> and <bold>
<italic>e</italic>
</bold>), 5.0 (<bold>
<italic>b</italic>
</bold> and <bold>
<italic>f</italic>
</bold>), 6.0 (<bold>
<italic>c</italic>
</bold> and <bold>
<italic>g</italic>
</bold>), and 7.0 (<bold>
<italic>d</italic>
</bold> and <bold>
<italic>h</italic>
</bold>) together with the corresponding emission intensities (<bold>
<italic>i</italic>
</bold>), integrated across the field of view, and their ratio (<bold>
<italic>j</italic>
</bold>) [yellow channel: &#x3bb;<sub>Ex</sub> &#x3d; 405&#xa0;nm, &#x3bb;<sub>Em</sub> &#x3d; 450&#x2013;600&#xa0;nm; green channel: &#x3bb;<sub>Ex</sub> &#x3d; 561&#xa0;nm, &#x3bb;<sub>Em</sub> &#x3d; 600&#x2013;770&#xa0;nm].</p>
</caption>
<graphic xlink:href="fmats-08-630046-g005.tif"/>
</fig>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>The covalent integration of a coumarin chromophore and either an oxazine or an oxazolidine heterocycle within the same molecular skeleton provides the opportunity of assembling molecular switches with ratiometric fluorescence response to pH. The oxazine or oxazolidine heterocycle opens upon acidification to establish an equilibrium between a ring-closed and a protonated ring-open form. In the latter species only, the coumarin chromophore can extend electronic delocalization over an indolium auxochrome. As a result, the protonated ring-open form is absorbed and emitted at wavelengths that are significantly longer than those where the ring-closed species is absorbed and emitted. This behavior enables the selective excitation of the two interconverting forms at distinct wavelengths and the collection of their emissions in resolved spectral windows. Furthermore, the relative amounts of the two equilibrating species and, hence, their relative emission intensities change with pH. It follows that separate detection channels of the same microscope can be exploited to collect the fluorescence of the two components independently and reconstruct a ratiometric profile of the pH distribution of any sample of interest labeled with these compounds.</p>
<p>A significant advantage of this family of molecular switches over existing compounds with ratiometric fluorescence response to pH is their synthetic accessibility and versatility. Three synthetic steps from readily available precursors are sufficient to assemble the parent molecular scaffold of both oxazine and oxazolidine derivatives, offering the opportunity to prepare relatively large amounts of these compounds. Additional synthetic modifications permit the manipulation of the substituents on the indole heterocycle and on the phenylene ring fused to the oxazine ring. These structural manipulations can be exploited to adjust the pH response and, in principle, to introduce hydrophilic chains for aqueous solubility (<xref ref-type="bibr" rid="B4">Cusido et al., 2012</xref>) or reactive functional groups for the covalent connection of biomolecules (<xref ref-type="bibr" rid="B5">Cusido et al., 2016</xref>; <xref ref-type="bibr" rid="B35">Zhang et al., 2018</xref>) or synthetic polymers (<xref ref-type="bibr" rid="B26">Tang et al., 2017</xref>). In fact, the fascinating prospect of incorporating targeting agents to direct these molecular switches into specific intracellular components and allow local pH probing can definitely be envisaged. Thus, the combination of photophysical and structural properties that can be engineered into these molecular switches can lead to the realization of versatile fluorescent probes for the intracellular visualization of pH distributions at the microscale with ratiometric imaging schemes.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="sec" rid="s9">Supplementary Material</xref>; further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>MA performed spectroscopic measurements. FC synthesized compounds. JB performed imaging experiments. SG supervised synthesis and contributed to manuscript production. FR designed the experiments, analyzed data, and wrote the manuscript.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>The National Science Foundation (CHE-1505885) and the Istituto Italiano di Technologia (IIT) are acknowledged for financial support.</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s9">
<title>Supplementary Material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fmats.2021.630046/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmats.2021.630046/full&#x23;supplementary-material</ext-link>.</p>
<supplementary-material xlink:href="table1.docx" id="SM2" mimetype="application/docx" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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