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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mol. Biosci.</journal-id>
<journal-title>Frontiers in Molecular Biosciences</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mol. Biosci.</abbrev-journal-title>
<issn pub-type="epub">2296-889X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">917725</article-id>
<article-id pub-id-type="doi">10.3389/fmolb.2022.917725</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Molecular Biosciences</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Cryo-EM Structure of an Atypical Proton-Coupled Peptide Transporter: Di- and Tripeptide Permease C</article-title>
<alt-title alt-title-type="left-running-head">Killer et al.</alt-title>
<alt-title alt-title-type="right-running-head">Cryo-EM Structure of DtpC</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Killer</surname>
<given-names>Maxime</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>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Finocchio</surname>
<given-names>Giada</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1809503/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Mertens</surname>
<given-names>Haydyn D. T.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1384200/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Svergun</surname>
<given-names>Dmitri I.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/137531/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Pardon</surname>
<given-names>Els</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Steyaert</surname>
<given-names>Jan</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/230795/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>L&#xf6;w</surname>
<given-names>Christian</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="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1545961/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Centre for Structural Systems Biology (CSSB)</institution>, <addr-line>Hamburg</addr-line>, <country>Germany</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Molecular Biology Laboratory (EMBL)</institution>, <institution>Hamburg Unit C/o Deutsches Elektronen Synchrotron (DESY)</institution>, <addr-line>Hamburg</addr-line>, <country>Germany</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Collaboration for Joint PhD Degree Between EMBL and Heidelberg University</institution>, <institution>Faculty of Biosciences</institution>, <addr-line>Heidelberg</addr-line>, <country>Germany</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Structural Biology Brussels</institution>, <institution>Vrije Universiteit Brussel (VUB)</institution>, <addr-line>Brussels</addr-line>, <country>Belgium</country>
</aff>
<aff id="aff5">
<sup>5</sup>
<institution>VIB-VUB Center for Structural Biology</institution>, <institution>VIB</institution>, <addr-line>Brussels</addr-line>, <country>Belgium</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/512979/overview">Arjen J. Jakobi</ext-link>, Delft University of Technology, Netherlands</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/1238383/overview">Ekaitz Errasti Murugarren</ext-link>, University of Barcelona. Spain</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1316843/overview">Giorgos Gouridis</ext-link>, Foundation for Research and Technology Hellas (FORTH), Greece</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Christian L&#xf6;w, <email>christian.loew@embl-hamburg.de</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Structural Biology, a section of the journal Frontiers in Molecular Biosciences</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>11</day>
<month>07</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>9</volume>
<elocation-id>917725</elocation-id>
<history>
<date date-type="received">
<day>11</day>
<month>04</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>16</day>
<month>06</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Killer, Finocchio, Mertens, Svergun, Pardon, Steyaert and L&#xf6;w.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Killer, Finocchio, Mertens, Svergun, Pardon, Steyaert and L&#xf6;w</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>Proton-coupled Oligopeptide Transporters (POTs) of the Major Facilitator Superfamily (MFS) mediate the uptake of short di- and tripeptides in all phyla of life. POTs are thought to constitute the most promiscuous class of MFS transporters, with the potential to transport more than 8400 unique substrates. Over the past two&#xa0;decades, transport assays and biophysical studies have shown that various orthologues and paralogues display differences in substrate selectivity. The <italic>E. coli</italic> genome codes for four different POTs, known as Di- and tripeptide permeases A-D (DtpA-D). DtpC was shown previously to favor positively charged peptides as substrates. In this study, we describe, how we determined the structure of the 53&#xa0;kDa DtpC by cryogenic electron microscopy (cryo-EM), and provide structural insights into the ligand specificity of this atypical POT. We collected and analyzed data on the transporter fused to split superfolder GFP (split sfGFP), in complex with a 52&#xa0;kDa Pro-macrobody and with a 13&#xa0;kDa nanobody. The latter sample was more stable, rigid and a significant fraction dimeric, allowing us to reconstruct a 3D volume of DtpC at a resolution of 2.7&#xa0;&#xc5;. This work provides a molecular explanation for the selectivity of DtpC, and highlights the value of small and rigid fiducial markers such as nanobodies for structure determination of low molecular weight integral membrane proteins lacking soluble domains.</p>
</abstract>
<kwd-group>
<kwd>peptide transporter</kwd>
<kwd>SLC15</kwd>
<kwd>nanobody</kwd>
<kwd>Pro-macrobody</kwd>
<kwd>single particle cryo-EM</kwd>
<kwd>DtpC</kwd>
<kwd>YjdL</kwd>
<kwd>proton-dependent oligopeptide transporter</kwd>
</kwd-group>
<contract-num rid="cn001">05K18YEA</contract-num>
<contract-sponsor id="cn001">Bundesministerium f&#xfc;r Bildung und Forschung<named-content content-type="fundref-id">10.13039/501100002347</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Membranes of cells compartmentalize metabolic processes and present a selective barrier for permeation. To preserve the characteristic intracellular milieu, membrane transporters with specialized functions have evolved to maintain the nutrient homeostasis of cells (<xref ref-type="bibr" rid="B25">Hediger et al., 2013</xref>; <xref ref-type="bibr" rid="B75">Zhang et al., 2019</xref>). Many of those are energized by an electrochemical proton gradient, providing a powerful driving force for transport and accumulation of nutrients above extracellular concentrations. Proton-dependent oligopeptide transporters (POTs) of the Solute Carrier 15 family (SLC15) are representatives of such secondary active transport systems and occur in all living organisms except in Archaea. They allow an efficient uptake of peptides and amino acids in bulk quantities (<xref ref-type="bibr" rid="B14">Daniel et al., 2006</xref>; <xref ref-type="bibr" rid="B70">Thwaites and Anderson, 2007</xref>). The best characterized members are the two mammalian PepT1 and PepT2 transporters which are known to play crucial roles in human health, being responsible for the uptake and distribution of nutrients such as di- and tripeptides (<xref ref-type="bibr" rid="B7">Brandsch et al., 2004</xref>; <xref ref-type="bibr" rid="B65">Smith et al., 2013</xref>; <xref ref-type="bibr" rid="B67">Spanier and Rohm, 2018</xref>; <xref ref-type="bibr" rid="B72">Viennois et al., 2018</xref>). They also play key roles in human diseases, and impact the pharmacokinetic profiles of orally administered drug molecules (<xref ref-type="bibr" rid="B13">Daniel, 2004</xref>; <xref ref-type="bibr" rid="B8">Brandsch, 2009</xref>; <xref ref-type="bibr" rid="B28">Ingersoll et al., 2012</xref>; <xref ref-type="bibr" rid="B27">Hillgren et al., 2013</xref>; <xref ref-type="bibr" rid="B11">Colas et al., 2017</xref>; <xref ref-type="bibr" rid="B26">Heinz et al., 2020</xref>). SLC15 transporters belong to the Major Facilitator superfamily (MFS). MFS transporters share a well-characterized fold, consisting of twelve transmembrane helices organized in two six-helix bundles, expected to function according to the alternate access mechanisms (<xref ref-type="bibr" rid="B29">Jardetzky, 1966</xref>) where either side of the transporter is alternately exposed to one side of the membrane. Therefore, substantial conformational changes are required to complete an entire transport cycle with at least three postulated states: (i) inward-open, (ii) occluded, and (iii) outward-open (<xref ref-type="bibr" rid="B74">Yan, 2015</xref>; <xref ref-type="bibr" rid="B16">Drew and Boudker, 2016</xref>; <xref ref-type="bibr" rid="B58">Quistgaard et al., 2016</xref>; <xref ref-type="bibr" rid="B3">Bartels et al., 2021</xref>; <xref ref-type="bibr" rid="B17">Drew et al., 2021</xref>). POTs have been intensively studied on a structural and biochemical level over the last 30 years. More than 50 entries for this transporter class can be found in the protein data bank, representing ten different bacterial homologues and the mammalian PepT1 and PepT2 transporters, bound to a limited set of substrates and drugs (<xref ref-type="bibr" rid="B46">Newstead et al., 2011</xref>; <xref ref-type="bibr" rid="B66">Solcan et al., 2012</xref>; <xref ref-type="bibr" rid="B15">Doki et al., 2013</xref>; <xref ref-type="bibr" rid="B23">Guettou et al., 2013</xref>; <xref ref-type="bibr" rid="B22">Guettou et al., 2014</xref>; <xref ref-type="bibr" rid="B41">Lyons et al., 2014</xref>; <xref ref-type="bibr" rid="B76">Zhao et al., 2014</xref>; <xref ref-type="bibr" rid="B59">Quistgaard et al., 2017</xref>; <xref ref-type="bibr" rid="B42">Martinez Molledo et al., 2018a</xref>; <xref ref-type="bibr" rid="B43">Martinez Molledo et al., 2018b</xref>; <xref ref-type="bibr" rid="B44">Minhas et al., 2018</xref>; <xref ref-type="bibr" rid="B45">Nagamura et al., 2019</xref>; <xref ref-type="bibr" rid="B71">Ural-Blimke et al., 2019</xref>; <xref ref-type="bibr" rid="B35">Killer et al., 2021</xref>; <xref ref-type="bibr" rid="B49">Parker et al., 2021</xref>; <xref ref-type="bibr" rid="B64">Shen et al., 2022</xref>; <xref ref-type="bibr" rid="B68">Stauffer et al., 2022</xref>). Although bacterial and eukaryotic POTs share an overall conserved binding site, individual amino acids changes in or in close vicinity of the binding site are likely responsible for observed differences in affinities and selectivity for particular peptides and drugs among the studied POT homologues. Here, structural biology studies are particularly crucial to understand substrate promiscuity and drug coordination on a molecular level. While bacterial POT structures, determined by mainly X-ray crystallography, represent exclusively the inward-open or inward-open-partially occluded state, the mammalian PepT1 and PepT2 transporters were recently captured in various conformations by single particle cryo-EM, advancing the mechanistic understanding of the entire transport cycle (<xref ref-type="bibr" rid="B35">Killer et al., 2021</xref>; <xref ref-type="bibr" rid="B49">Parker et al., 2021</xref>). Despite their small size of typically only 50&#xa0;kDa for an individual transporter unit, these systems become more and more accessible for single-particle cryo-EM approaches. Indeed, in 2021, more MFS transporter structures were determined by single-particle Cryo-EM (17 pdb entries; resolution range 3.0&#x2014;4.2&#xa0;&#xc5;) than X-ray crystallography (14 pdb entries; resolution range 1.8&#x2014;3.6&#xa0;&#xc5;).</p>
<p>Although known POT structures show a high level of similarity, various works have indicated that homologues can differ in their range of transported substrate and drug molecules (<xref ref-type="bibr" rid="B41">Lyons et al., 2014</xref>; <xref ref-type="bibr" rid="B53">Prabhala et al., 2014</xref>; <xref ref-type="bibr" rid="B5">Boggavarapu et al., 2015</xref>; <xref ref-type="bibr" rid="B63">Sharma et al., 2016</xref>; <xref ref-type="bibr" rid="B42">Martinez Molledo et al., 2018a</xref>). The <italic>E. coli</italic> genome codes for four different POTs named Di- and tripeptide permease A-D (DtpA-D), also known as YdgR (&#x3d;DtpA), YhiP (&#x3d;DtpB), YjdL (&#x3d;DtpC) and YbgH (&#x3d;DtpD). They cluster in pairs, DtpA and B (sequence identity 51%), and DtpC and D (sequence identity 56%) with around 25% identity between them. DtpA and B exhibit a prototypical substrate preference similar to the human PepT1 transporter (<xref ref-type="bibr" rid="B10">Chen et al., 2000</xref>; <xref ref-type="bibr" rid="B24">Harder et al., 2008</xref>; <xref ref-type="bibr" rid="B19">Foley et al., 2010</xref>; <xref ref-type="bibr" rid="B52">Prabhala et al., 2017</xref>; <xref ref-type="bibr" rid="B54">Prabhala et al., 2018</xref>), while DtpC and D have been classified as atypical POTs, because DtpC prefers dipeptides in particular those with a lysine residue in the second position. Although DtpC has been well characterized in terms of function over the last years (<xref ref-type="bibr" rid="B18">Ernst et al., 2009</xref>; <xref ref-type="bibr" rid="B31">Jensen et al., 2012a</xref>; <xref ref-type="bibr" rid="B32">Jensen et al., 2012b</xref>; <xref ref-type="bibr" rid="B33">Jensen et al., 2012c</xref>; <xref ref-type="bibr" rid="B30">Jensen et al., 2014</xref>; <xref ref-type="bibr" rid="B53">Prabhala et al., 2014</xref>; <xref ref-type="bibr" rid="B1">Aduri et al., 2015</xref>), it has resisted structure determination by X-ray crystallography so far (<xref ref-type="bibr" rid="B21">Gabrielsen et al., 2011</xref>).</p>
<p>Here we describe the structure determination of the bacterial POT transporter DtpC by single particle cryo-EM. Considering that the transporter displays no characteristic cytoplasmic or periplasmic features which are helpful to drive the particle alignment, we applied different strategies previously described in the literature to increase the overall size of the transporter to overcome these limitations. We i) fused the transporter to split-sfGFP (<xref ref-type="bibr" rid="B38">Liu et al., 2020</xref>; <xref ref-type="bibr" rid="B37">Liu et al., 2022</xref>), ii) raised different nanobodies against DtpC (<xref ref-type="bibr" rid="B48">Pardon et al., 2014</xref>) and iii) extended the nanobody to a Pro-macrobody (<xref ref-type="bibr" rid="B9">Brunner et al., 2020</xref>; <xref ref-type="bibr" rid="B6">Botte et al., 2022</xref>). The various samples were subsequently imaged by cryo-EM and analysed. DtpC in complex with the conformation specific nanobody 26 turned out to be more rigid and a significant fraction of the sample dimeric, allowing us to reconstruct DtpC to 2.7&#xa0;&#xc5; resolution. The DtpC structure now provides molecular insights into how selectivity within this transporter family is achieved.</p>
</sec>
<sec sec-type="results|discussion" id="s2">
<title>2 Results and Discussion</title>
<sec id="s2-1">
<title>2.1 Different Fiducial Marker Strategies for Structure Determination</title>
<p>Since MFS transporters typically lack additional domains outside their transport unit, which is a major impediment for accurate particle alignment in single particle cryo-EM approaches, we assessed three fiducial marker strategies introducing additional density outside of detergent micelles containing DtpC, by analyzing the quality of 2D class averages (<xref ref-type="fig" rid="F1">Figure 1</xref>). To obtain conformation specific binders against DtpC, we first immunized llamas with recombinant DtpC and selected nanobodies (Nbs) following standard procedures (<xref ref-type="bibr" rid="B48">Pardon et al., 2014</xref>). Three out of five selected binders (Nb17, Nb26, and Nb38) co-eluted with DtpC on gel filtration (<xref ref-type="sec" rid="s9">Supplementary Figure S1</xref>) and increased the melting temperature of the respective DtpC-Nb complex by 20&#xb0;C, 16&#xb0;C, and 12&#xb0;C. (<xref ref-type="fig" rid="F2">Figures 2A,B</xref>). DtpC in complex with Nb17 and Nb26 yielded crystals in various conditions, but despite extensive optimization efforts, the crystals of the DtpC-Nb26 complex did not diffract X-rays better than 5&#xa0;&#xc5; resolution. In a second step, we decided to increase the size of Nb26, which formed a tight complex with DtpC, by fusing one copy of the maltose binding protein (MBP) to its C-terminus as described previously (<xref ref-type="bibr" rid="B6">Botte et al., 2022</xref>)<bold>.</bold> This resulted in a 52&#xa0;kDa Pro-macrobody (short Mb26), and we expected it to bind to the periplasmic side of the transporter as seen in other MFS transporter-Nb complexes (<xref ref-type="fig" rid="F1">Figure 1</xref>). In a third approach, we fused the two self-assembling parts of split-sfGFP; with &#x3b2;1-6 on the N-terminus of DtpC, and &#x3b2;7-11 on the C-terminus. We named this construct split sfGFP-DtpC<sub>FL</sub>. In order to minimize the mobility between the membrane protein and the split sfGFP fiducial, we also generated two additional constructs where the last five (split sfGFP-DtpC<sub>1-475</sub>), or ten residues (split sfGFP-DtpC<sub>1-470</sub>) of the transporter were deleted. We then assessed proper folding and complementation by monitoring the fluorescence of the chromophore on an HPLC system (<xref ref-type="fig" rid="F2">Figure 2C</xref>). All constructs eluted at similar retention times and the fluorescence was highest in the non-truncated construct (split sfGFP-DtpC<sub>FL</sub>) and lowest in the most truncated version (split sfGFP-DtpC<sub>1-470</sub>). In order to extend this observation to other MFS transporters, we repeated this experiment with the human POT homologue PepT1, and noticed a similar trend upon shortening of the termini. Yet, since the decrease of fluorescence was only minor in split sfGFP-DtpC<sub>1-475</sub> in comparison to split sfGFP-DtpC<sub>FL</sub>, we proceeded to imaging with the shorter construct in the presence of Nb26.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Utilization of different fiducial markers to improve particle alignment and 2D averaging from cryo-EM images. From left to right: DtpC-Mb26, split-sfGFP-DtpC<sub>1-475</sub>-Nb26, and DtpC-Nb26 were purified, vitrified on grids and imaged. Single particles were identified, clustered and averaged. The best average from each sample is shown under a representative raw micrograph.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g001.tif"/>
</fig>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Characterization of the different fiducial markers. <bold>(A)</bold> The melting temperature of each fiducial and DtpC-fiducial complex was measured by nano-differential scanning fluorimetry (DSF) in triplicate measurements as shown as open circles. The average of the three values is marked by a line. <bold>(B)</bold> The first derivative of the summarized data in <bold>(A)</bold> is shown for DtpC and the three imaged samples together with the respective fiducial. <bold>(C)</bold> A schematic representation of the split sfGFP-DtpC architecture is shown on the top left panel. Below, structure predictions were generated for split-sfGFP-DtpC<sub>&#x2b;5Gly</sub>, split-sfGFP-DtpC<sub>FL</sub>, sfGFP-DtpC<sub>1-475</sub>, and overlaid with sfGFP (PDB accession number 2B3P). The dark-violet coloring corresponds to the fraction of &#xdf;7 which is properly folded in sfGFP while unfolded in the restrained chimeric construct. The right panel shows HPLC chromatogram profiles monitoring the fluorescence of the chromophore of split sfGFP in the context of the indicated constructs, using 480&#xa0;nm as excitation wavelength and recording at 510&#xa0;nm the emitted light.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g002.tif"/>
</fig>
<p>The particle density and distribution in the vitrified solution was similar in the three imaged samples. However, DtpC-Nb26 produced the best 2D class averages considering the sharpness of secondary structure elements inside the micelle, as judged by visual inspection (<xref ref-type="fig" rid="F1">Figure 1</xref>, <xref ref-type="sec" rid="s9">Supplementary Figure S2</xref>). The Pro-macrobody Mb26 fiducial was clearly visible in 2D class averages, but it adopted various positions in relation to the transporter, therefore making accurate alignment of the particles more difficult than in its shorter but more rigid and stable nanobody version (<xref ref-type="fig" rid="F1">Figure 1</xref>, <xref ref-type="fig" rid="F3">Figure 3A, B</xref>, <xref ref-type="sec" rid="s9">Supplementary Figure S2</xref>). The split sfGFP-DtpC<sub>(1&#x2013;475)</sub>-Nb26 sample allowed clear visualization of the transmembrane helices after clustering a small subset of particles, but the majority of particles clustered in classes with blurry density for the split sfGFP fiducial, or with the two complementary parts &#x3b2;1-6 and &#x3b2;7-11 not assembled (<xref ref-type="sec" rid="s9">Supplementary Figure S2</xref>). AlphaFold2 predictions on the imaged construct, as well as on the full length construct later suggested a destabilization of the beta-barrel upon increasing termini restrains, resulting in partial unfolding of &#x3b2;7 and exposure of the chromophore to solvent quenching. Interestingly, this effect could partially be reverted by adding a linker of five glycine residues between the C-bundle and &#x3b2;7 based on <italic>in silico</italic> data. We conclude that termini restraining using the split-sfGFP approach is a promising fiducial strategy for structural studies of MFS transporters, in addition to the previous demonstrated showcases on small membrane proteins (2, 4 and 6TMs) (<xref ref-type="bibr" rid="B38">Liu et al., 2020</xref>; <xref ref-type="bibr" rid="B37">Liu et al., 2022</xref>). However, the amount of restraining in larger membrane proteins such as MFS transporters where both termini are placed far from each other need to be optimized experimentally or <italic>in silico</italic>, to produce a stable and rigid fiducial; two crucial aspects for high resolution structure determination of MFS transporters by single particle cryo-EM.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Cryo-EM structure of DtpC-Nb26. <bold>(A)</bold> Representative 2D class averages of the dimeric population. <bold>(B)</bold> 3D reconstruction of the DtpC-Nb26 inverted dimer used for local focused refinement on one copy of the transporter, shown in <bold>(C)</bold>. <bold>(D)</bold> Atomic model of DtpC displayed as ribbon diagram. The different structural elements are labelled.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g003.tif"/>
</fig>
<p>As we obtained the best 2D class averages for DtpC with the fiducial marker Nb26, we proceeded to a large data collection (<xref ref-type="table" rid="T1">Table 1</xref>) and could cluster a subset of dimers within this data set (<xref ref-type="fig" rid="F3">Figure 3</xref>). The presence of different oligomeric species was already expected based on the peak shape of the gel filtration run (<xref ref-type="fig" rid="F4">Figure 4A</xref>). The large mass of the dimer, and the stable and rigid signal of the Nb26 fiducial, allowed us to reconstruct the DtpC-Nb26 dimer to 3.0&#xa0;&#xc5; resolution and model this assembly (<xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>, <xref ref-type="sec" rid="s9">Supplementary Figure S3</xref>). The quaternary structure consists of a non-symmetrical inverted dimer mediated by interactions through a large hydrophobic interface between the HA-HB helices of DtpC (<xref ref-type="sec" rid="s9">Supplementary Figure S3</xref>). Although other inverted dimers were reported in homologous POT structures (<xref ref-type="bibr" rid="B59">Quistgaard et al., 2017</xref>), the source of such arrangements is likely to be artificial. We also investigated the oligomer heterogeneity in solution with small angle X-ray scattering and obtained a good fit at low angles (corresponding to the overall shape of particles in solution) for the cryo-EM volume of the dimer (<xref ref-type="sec" rid="s9">Supplementary Figure S4</xref>). The fit to a monomeric cryo-EM volume was poor, indicating that in detergent solution a significant fraction of DtpC-Nb26 is dimeric. As for the interaction between the membrane protein and the fiducial marker, the CDR3 loop of Nb26 accounts for the strongest interactions with the periplasmic surface of the transporter with two salt bridges, while CDR1 and CDR2 contribute via hydrogen bonding (<xref ref-type="fig" rid="F5">Figure 5</xref>). 3D variability analysis (<xref ref-type="bibr" rid="B55">Punjani and Fleet, 2021</xref>) revealed a small degree of flexibility between the two DtpC-Nb26 copies. Therefore, we performed a local refinement, focused on one copy of the membrane protein, which extended the resolution of the reconstruction to 2.7&#xa0;&#xc5; and improved the accuracy of the atomic model for subsequent structural analysis (<xref ref-type="fig" rid="F4">Figure 4</xref>).</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Data collection and refinement statistics of the deposited DtpC structure.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Protein Reconstructed</th>
<th align="center">Di- and Tripeptide Permease C (DtpC)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">PDB accession code</td>
<td align="left">7ZC2</td>
</tr>
<tr>
<td align="left">EMDB accession code</td>
<td align="left">EMD-14618</td>
</tr>
<tr>
<td align="left">Data acquisition</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Microscope/Detector</td>
<td align="left">Titan Krios/Gatan K3</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Imaging software</td>
<td align="left">EPU</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Magnification</td>
<td align="left">105,000</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Voltage (kV)</td>
<td align="left">300</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Electron exposure (e-/&#xc5;<sup>2</sup>)</td>
<td align="left">75</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Dose rate (e-/pix/s)</td>
<td align="left">19.5</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Frame exposure (e-/&#xc5;<sup>2</sup>)</td>
<td align="left">1.5</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Defocus range (&#xb5;m)</td>
<td align="left">-0.9 to -1.8</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Physical pixel size (&#xc5;)</td>
<td align="left">0.85</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Micrographs</td>
<td align="left">24,333</td>
</tr>
<tr>
<td align="left">Reconstruction</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Picked coordinates (cryolo)</td>
<td align="left">6,464,070</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Particles in 3D classification (RELION)</td>
<td align="left">6,365,235</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Particles in final refinement (CryoSPARC)</td>
<td align="left">878,428</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Symmetry imposed</td>
<td align="left">C1</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Map sharpening method</td>
<td align="left">Phenix Resolve_cryo_em</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Map resolution, FSC<sub>half maps; 0.143</sub> masked/unmasked (&#xc5;)</td>
<td align="left">2.72/3.43</td>
</tr>
<tr>
<td align="left">Refinement</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Initial model used for refinement</td>
<td align="left">AlphaFold2 model, relaxed with Amber</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Model resolution (&#xc5;)</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;FSC 0.143, masked/unmasked</td>
<td align="left">2.64/5.43</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Model composition</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Non-hydrogen atoms</td>
<td align="left">7334</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Protein residues</td>
<td align="left">471</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;ADP B factor (&#xc5;<sup>2</sup>) mean</td>
<td align="left">12.73</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;R.m.s deviations</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Bond lengths (&#xc5;) (&#x23;&#x3e;4&#x3c3;)</td>
<td align="left">0.003 (0)</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Bond angles (&#xb0;) (&#x23;&#x3e;4&#x3c3;)</td>
<td align="left">0.616 (0)</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Validation</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;MolProbity score</td>
<td align="left">1.44</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Clashscore</td>
<td align="left">8.04</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Rotamer outliers (%)</td>
<td align="left">0.00</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;Ramachandran plot</td>
<td align="left"/>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Favored (%)</td>
<td align="left">98.29</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Allowed (%)</td>
<td align="left">1.71</td>
</tr>
<tr>
<td align="left">&#xa0;&#xa0;&#xa0;&#xa0;Outliers (%)</td>
<td align="left">0.00</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>High resolution structure determination of DtpC-Nb26. <bold>(A)</bold> Gel filtration was performed on a preparative column (left) before concentrating the sample to 60&#xa0;mg/ml and rerunning it on an analytic column on an HPLC system (right), in order to obtain a highly concentrated sample, free of empty detergent micelles. Peak shape already indicates a mixture of different oligomeric species. <bold>(B)</bold> Representative raw micrograph of the acquired dataset. The applied defocus is -1.5&#xa0;&#xb5;m. <bold>(C)</bold> Summary of the image analysis. The angular assignments from the dimeric reconstruction were used as prior to perform a local focused refinement with reduced angular and translational searches on the masked region illustrated in blue. <bold>(D)</bold> The Fourier transforms over different shells on frequency space, of two independent volumes (half maps) were compared (FSC) and plotted as a function of spatial frequency, to estimate the overall resolution using the 0.143 cutoff threshold. <bold>(E)</bold> The two half maps were used as inputs to assess various post-processing strategies.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g004.tif"/>
</fig>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Interactions between Nb26 and DtpC. <bold>(A)</bold> The sequences of the five nanobodies representing five different families, obtained after selection, with their complementary determining regions (CDR) are shown. Interactions of Nb26 with DtpC are highlighted as green (hydrogen bonds involving the protein backbone), blue (hydrogen bonds involving side chains) and red dashes (salt bridges). <bold>(B)</bold> These interactions are further displayed in 3D. CDR regions are depicted as sticks on the surface of DtpC where the N-terminal bundle is colored in grey, and the C-terminal bundle in dark grey.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g005.tif"/>
</fig>
</sec>
<sec id="s2-2">
<title>2.3 Structural Basis for Ligand Selectivity in DtpC</title>
<p>The DtpC structure revealed the expected and well-known MFS transporter fold, with twelve transmembrane helices (TMs) organized in two helical bundles and additional two&#xa0;TMs specific for the POT family (known as HA and HB domains). It is highly similar compared to the previously determined DtpD structure (<xref ref-type="bibr" rid="B76">Zhao et al., 2014</xref>) with an overall RMSD value of 1.06&#xa0;&#xc5; between the two (for 335 out of 436&#xa0;C<sub>&#x3b1;</sub>-atoms). The peptide binding site of DtpC is exposed to the cytoplasmic side (<xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>). Almost all bacterial POT structures described so far were determined by X-ray methods in a similar inward facing (IF) conformation. The extent to which the central cavity is open to the cytosol is regulated by a mechanism of occlusion mediated by TM4, TM5, TM10, and TM11, as supported by structures in IF occluded, partially occluded, and open states. In the case of the here described DtpC structure, the IF state is open (<xref ref-type="fig" rid="F3">Figure 3</xref>).</p>
<p>Molecules from the periplasmic side, on the contrary, cannot enter the central cavity. Tight closure of both bundles above the binding site is mediated by a salt bridge between D43 (TM2, N-bundle) and R294 (TM7, C-bundle) and hydrogen bonds between H37 (TM1, N-bundle) and D293 (TM7) as well as R28 (TM1) and N421 (TM11, C-bundle) (<xref ref-type="fig" rid="F6">Figure 6A</xref>). We also analyzed previously determined POT structures with clearly resolved side chain densities, to understand how the IF state is generally maintained in this transporter family. Except for human PepT2 and the POT transporter from <italic>Shewanella oneidensis</italic> (PepT<sub>So</sub>), where the inter-bundle periplasmic salt bridge is formed between TM5 and TM7, the IF state is in all other analyzed structures stabilized by a salt bridge on the tip of TM2 and TM7 (<xref ref-type="fig" rid="F6">Figure 6B</xref>). Additional hydrogen bonding networks as described in other studies, can occur, but vary greatly among different homologues. This analysis highlights that the alternate access mechanism in canonical and in so called &#x2018;atypical&#x2019; POTs share similarities such as electrostatic clamping by formation and disruption of salt bridges. The differences in hydrogen bonding patterns however, could account for the various turnover rates seen among POT homologues.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Structural basis for the stabilization of the inward facing state in DtpC and other POT homologues. <bold>(A)</bold> The salt bridge and hydrogen bonds favoring closure of the two bundles on the periplasmic side of DtpC are respectively shown as red and blue dashes. <bold>(B)</bold> The structures of homologous POTs from <italic>Escherichia coli</italic> (DtpD, DtpA), <italic>Shewanella oneidensis</italic> (PepT<sub>So2</sub>, PepT<sub>So</sub>) <italic>Staphylococcus hominis</italic> (PepT<sub>Sh</sub>), <italic>Streptococcus thermophilus</italic> (PepT<sub>St</sub>), <italic>Yersinia enterocolitica</italic> (YePepT) and <italic>Homo sapiens</italic> (HsPepT2), were all previously captured in the IF state. Here they were analyzed to identify the strongest interaction stabilizing their common conformation. The structures are colored from blue to red, from their N- to C-termini, and the respective PDB accession numbers are indicated. Conserved salt bridges are labelled and highlighted by red dashed lines.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g006.tif"/>
</fig>
<p>Canonical POTs are characterized by i) the presence of the E<sub>1</sub>XXE<sub>2</sub>R motif on TM1 involved in proton coupling and ligand binding, and ii) the ability to accommodate dipeptides, tripeptides, and peptidomimetics, which relies on a set of conserved residues located in the central binding cavity. In DtpC, the E<sub>1</sub>XXE<sub>2</sub>R motif, has evolved to Q<sub>1</sub>XXE<sub>2</sub>Y (where Q<sub>1</sub> &#x3d; N17, E<sub>2</sub> &#x3d; E20, Y&#x3d;Y21). In all high resolution X-ray structures of canonical POTs, R is in salt-bridge distance to E<sub>2</sub> and the C-terminus of substrate peptides. Mutation of either E<sub>1</sub> or E<sub>2</sub> in the conventional E<sub>1</sub>XXE<sub>2</sub>R motif to glutamine residues abolishes uptake (<xref ref-type="bibr" rid="B1">Aduri et al., 2015</xref>). A reverse mutation in DtpC, from Q<sub>1</sub>XXE<sub>2</sub>Y to E<sub>1</sub>XXE<sub>2</sub>Y or to E<sub>1</sub>XXQ<sub>2</sub>Y preserves high transport rates, while a Q<sub>1</sub>XXQ<sub>2</sub>Y motif significantly decreases it (<xref ref-type="bibr" rid="B1">Aduri et al., 2015</xref>). In addition, based on previous molecular dynamics experiments, a salt bridge switching mechanism from R-E<sub>2</sub> to R-E<sub>1</sub>, upon protonation of E<sub>2</sub> in the E<sub>1</sub>XXE<sub>2</sub>R motif, was proposed (<xref ref-type="bibr" rid="B1">Aduri et al., 2015</xref>). This biochemical and <italic>in silico</italic> data strongly support a dual role of the E<sub>1</sub>XXE<sub>2</sub>R motif for both proton and peptide transport, where R can form a salt bridge interaction with the C-terminus of peptides or with E<sub>1</sub> when E<sub>2</sub> is protonated, and where the deprotonation event of the latter is required to disrupt the R-peptide interaction.</p>
<p>In DtpC, we now observe that the side chain pocket has a different architecture and characteristic in comparison with the one of canonical POTs. It displays an overall more acidic groove caused by the presence of the aspartate residue 392, conserved among atypical POTs. This residue has been predicted to be involved in substrate coordination and mutation of this residues in DtpC and homologues DtpD (corresponding residue is D395) abolished transport activity (<xref ref-type="bibr" rid="B32">Jensen et al., 2012b</xref>; <xref ref-type="bibr" rid="B76">Zhao et al., 2014</xref>). Canonical POTs have a conserved serine residue instead, yielding a slightly changed hydrophobicity pattern in the binding site (<xref ref-type="fig" rid="F7">Figures 7A&#x2013;D</xref>). A structural overlay of DtpC with a canonical POT structure bound to the dipeptide Ala-Phe allows us to position the peptide in the binding site. By replacing the phenyl group with a lysine side chain (generating the known DtpC dipeptide substrate Ala-Lys instead of Ala-Phe), we postulate a putative salt bridge between the carboxyl group of D392 and the &#x3b5;-amino group of the lysine side chain. This observation, together with previous biochemical work (<xref ref-type="bibr" rid="B32">Jensen et al., 2012b</xref>; <xref ref-type="bibr" rid="B1">Aduri et al., 2015</xref>) allows us to hypothesize that the selectivity of DtpC for dipeptides with C-terminal lysine or arginine residues is caused by swapping a salt bridge between the recurrent carboxyl group of the peptide terminus and the transporter (R21Y mutation), to a side chain specific salt bridge with D392. Since the R-peptide interaction is lost in DtpC, there is no requirement for E1 to destabilize R-peptide for release, which would explain the presence of a Q<sub>1</sub>XXE<sub>2</sub>Y motif instead of E<sub>1</sub>XXE<sub>2</sub>R.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Structural basis for ligand selectivity in DtpC and atypical POTs. <bold>(A)</bold> Key residues involved in substrate binding are colored and shown as sticks. In the close up view, an overlay of HsPepT2 (transparent residues) bound to the dipeptide Ala-Phe (beige) with DtpC is shown. Residues colored in grey are conserved while blue residues are exclusive to atypical POTs. <bold>(B)</bold> The arrangement of the E1XXE2R motif from PepT<sub>St</sub> is shown on the left panel, and the atypical Q1XXE2Y on the right. <bold>(C)</bold> The sequences of 13 POTs were aligned and residues involved in proton coupling and substrate binding are shown. The red squares mark residues strongly interacting with the charged termini of substrates peptides via salt bridges. The blue squares indicate two conserved asparagine residues stabilizing peptides through hydrogen bonds. The black squares point to residues constituting the side chain pocket of POTs, tuning ligand promiscuity or selectivity. <bold>(D)</bold> Surface representation colored by electrostatic potential, of the C-bundles of DtpC (top panel) and DtpA (bottom panel). A pose of the preferred substrate of DtpC, Ala-Lys, is proposed (top) and the co-crystallized valganciclovir drug hijacking canonical POTs is shown in DtpA (bottom). PDB accession codes of previously published work: HsPepT2 bound to Ala-Phe: 7PMY; PepT<sub>St</sub>: 5OXO; DtpA bound to valganciclovir: 6GS4.</p>
</caption>
<graphic xlink:href="fmolb-09-917725-g007.tif"/>
</fig>
<p>In summary, our work provides new insights into promiscuous versus selective substrate recognition in POTs and constitutes a step forward towards completing the family of <italic>E. coli</italic> POTs structures. Lastly, it displays some of the challenges related to high resolution cryo-EM structure determination of MFS transporters devoid of soluble domains, and manifests once again, the benefit of fiducial markers in overcoming those.</p>
</sec>
</sec>
<sec id="s3">
<title>3 Material and Methods</title>
<sec>
<title>3.1 Expression and purification of membrane protein constructs: DtpC; split sfGFP-DtpC (full length split sfGFP-DtpC<sub>FL</sub>, and truncated constructs split sfGFP-DtpC<sub>1-475</sub> and split sfGFP-DtpC<sub>1-470</sub>); split sfGFP-<italic>Hs</italic>PepT1 (full length split sfGFP-<italic>Hs</italic>PepT1<sub>FL</sub>, and truncated constructs split sfGFP-<italic>Hs</italic>PepT1<sub>1-672</sub> and split sfGFP-<italic>Hs</italic>PepT1<sub>10-672</sub>)</title>
<p>The full-length cDNA of DtpC wild type (WT) was amplified from the <italic>Escherichia coli</italic> genome, and cloned into a pNIC-CTHF vector by ligation-independent cloning (LIC). This vector contains a C-terminal His-Tag and a Tobacco Etch virus (TEV) cleavage site and a kanamycin resistance gene as selectable marker. The first 6&#xa0;N-terminal beta strands of sfGFP were fused to the N-terminus of DtpC, and the beta strands 7 to 11 fused to the C-terminus. We named this construct split sfGFP-DtpC<sub>FL</sub>. Two additional constructs were cloned with truncations of 5 (split sfGFP-DtpC<sub>1-475</sub>), and 10 residues (split sfGFP-DtpC<sub>1-470</sub>), on the C-terminal side of DtpC.</p>
<p>
<italic>Hs</italic>PepT1 was previously cloned into a pXLG vector containing an expression cassette composed of an N-terminal Twin-Streptavidin tag followed by the HRV-3C protease recognition sequence (<xref ref-type="bibr" rid="B35">Killer et al., 2021</xref>). Similarly, as for DtpC, the two self-assembling parts of split-sfGFP were first inserted into the N- and C-termini of the full-length version of <italic>Hs</italic>PepT1, and on two other versions with i) a C-terminal truncation of 36 residues (split sfGFP-HsPepT11-672), and ii) a C-terminal truncation of 36 residues and a N-terminal truncation of 10 residues (split sfGFP-HsPepT110-672) were cloned.</p>
<p>Recombinant DtpC, and the three split sfGFP-DtpC constructs were expressed in <italic>E. coli</italic> C41(DE3) cells grown in terrific broth (TB) media supplemented with 30&#xa0;&#x3bc;g/ml kanamycin according to established procedures (<xref ref-type="bibr" rid="B39">L&#xf6;w et al., 2012</xref>; <xref ref-type="bibr" rid="B40">L&#xf6;w et al., 2013</xref>). Cultures were grown at 37&#xb0;C and protein expression was induced with 0.2&#xa0;mM IPTG at an OD<sub>600 nm</sub> of 0.6&#x2013;0.8. After induction, culture growth continued at 18&#xb0;C for 16-18&#xa0;h. Cells were harvested by centrifugation (10,000 &#x00D7; g, 15&#xa0;min, 4&#xb0;C), and the pellet was stored at -20&#xb0;C until further use. Cell pellets were resuspended in lysis buffer (20&#xa0;mM NaPi at pH 7.5, 300&#xa0;mM NaCl, 5% (v/ v) glycerol, 15&#xa0;mM imidazole, with 3&#xa0;ml of lysis buffer per Gram of wet weight pellet), supplemented with lysozyme, DNase and 0.5&#xa0;mM tris(2-carboxyethyl)phosphine (TCEP). The cells were lysed by three cycles using an Avestin Emulsiflex homogenizer at 10,000&#x2013;15,000 psi. Recovered material was centrifuged to remove non-lysed cells (10,000 &#xd7; <italic>g</italic>, 15&#xa0;min, 4&#xb0;C) and the supernatant was subjected to ultracentrifugation to separate the membrane fraction (100,000 &#xd7; <italic>g</italic>, 1&#xa0;h, 4&#xb0;C using an Optima XE-90, Beckman Coulter centrifuge). Membranes were resuspended in lysis buffer supplemented with cOmplete EDTA-free protease inhibitors (Roche), and solubilized by adding 1% n-Dodecyl-&#x3b2;-D-Maltoside (DDM) detergent (Anatrace). The sample was centrifuged for 50&#xa0;min at 90,000 &#xd7; <italic>g</italic>, and the supernatant was applied to Ni-NTA beads for immobilized-metal affinity chromatography (IMAC) on a gravity column. The beads were pre-equilibrated in lysis buffer and incubated with the solubilized membrane proteins for one hour at 4&#xb0;C on a rotating wheel. Loaded beads were washed with buffer with increasing imidazole concentrations (20&#xa0;mM NaPi at pH 7.5, 300&#xa0;mM NaCl, 5% glycerol, 15-30&#xa0;mM imidazole, 0.5&#xa0;mM TCEP, 0.03% DDM). The proteins were eluted from the column with a buffer containing high imidazole concentration (20&#xa0;mM NaPi at pH 7.5, 150&#xa0;mM NaCl, 5% glycerol, 250&#xa0;mM imidazole, 0.5&#xa0;mM TCEP, 0.03% DDM) and combined with 1&#xa0;mg of TEV protease to perform the His-tag cleavage during dialysis overnight at 4&#xb0;C. The dialysis buffer contained 20&#xa0;mM HEPES at pH 7.5, 150&#xa0;mM NaCl, 5% glycerol, 0.5&#xa0;mM TCEP, 0.03% DDM. The cleaved protein was recovered by negative IMAC, concentrated to 4&#xa0;ml using a 50&#xa0;kDa concentrator (Corning<sup>&#xae;</sup> Spin-X<sup>&#xae;</sup> UF concentrators) and run on an &#xc4;KTA Pure system (GE Healthcare Life Sciences), using a HiLoad 16/ 600 Superdex 200 column for DtpC, and a Superdex 200 Increase 10/300 column for the split sfGFP-DtpC constructs. Fractions containing the protein were pooled, concentrated, flash frozen and stored at -80&#xb0;C until further use.</p>
<p>For the split sfGFP-<italic>Hs</italic>PepT1 constructs, expression was done in mammalian cells as described previously (<xref ref-type="bibr" rid="B51">Pieprzyk et al., 2018</xref>; <xref ref-type="bibr" rid="B35">Killer et al., 2021</xref>). Briefly, HEK293F&#xa0;cells were collected 48&#xa0;h after transient transfection, and stored at &#x2212;80&#xb0;C until further use. Frozen cell pellets were resuspended in 300&#xa0;mM NaCl, 20&#xa0;mM NaPi (pH 7.5), 0.5&#xa0;mM TCEP, and 5% glycerol, supplemented with cOmplete EDTA-free protease inhibitors, and were disrupted using an Avestin Emulsiflex homogenizer at 10,000&#x2013;15,000 psi. The lysate was centrifuged for 10&#xa0;min at 10,000 &#x00D7; g, 4&#xb0;C, and the supernatant was centrifuged for 90&#xa0;min at 100,000 &#x00D7; g, 4&#xb0;C. The pellet containing the membrane fraction was solubilized in 1% N-Dodecyl-&#x3b2;-D-Maltopyranoside (DDM) and 0.1% cholesteryl hemisuccinate (CHS; Tris Salt, Anatrace) for 1&#xa0;h at 4&#xb0;C. The sample was centrifuged for 50&#xa0;min at 90,000 &#xd7; <italic>g</italic>, and the supernatant was applied to Strep-TactinXT beads (IBA). After 20&#xa0;min of incubation on a rotating wheel, the suspension was transferred to a gravity column. Following two wash steps with 300&#xa0;mM NaCl, 20&#xa0;mM HEPES (pH 7.5), 0.03% DDM, and 0.003% CHS, split sfGFP-<italic>Hs</italic>PepT1comnstructs were eluted with 0.03% DDM, 0.003% CHS, 150&#xa0;mM NaCl, 20&#xa0;mM HEPES (pH 7.5), and 10&#xa0;mM desthiobiotin (Sigma-Aldrich).</p>
</sec>
<sec id="s3-1">
<title>3.2 Selection, Expression and Purification of Nanobodies Against DtpC</title>
<p>To generate DtpC specific nanobodies, two non-inbred llamas were injected six times at weekly intervals with a mixture of 94 different proteins including DtpC purified in the detergent DDM (50&#xa0;&#xb5;g of each antigen weekly). After 6&#xa0;weeks of immunization, two separate phage display libraries were constructed, one from each animal, in the pMESy2 vector, which is a derivative of pMESy4 that contain a C-terminal EPEA-tag for affinity purification. After pooling both libraries, nanobodies were selected against individual antigens in two rounds of parallel panning in 96-well plates containing one immobilized antigen in each well. After two selection rounds on DtpC, 60 clones were picked for sequence analysis, 13 clones encoded antigen-specific nanobodies as tested in ELISA, grouping them in 5 different sequence families. A nanobody family is defined as a group of nanobodies with a high similarity in their CDR3 sequence (identical length and &#x3e;80% sequence identity). Nanobodies from the same family derive from the same B-cell lineage and likely bind to the same epitope on the target. Immunizations, library construction, selection by panning and nanobody characterization were performed according to standard procedures (<xref ref-type="bibr" rid="B48">Pardon et al., 2014</xref>). Five nanobodies were further characterized.</p>
<p>The nanobodies were expressed in <italic>E. coli</italic> WK6 cells and purified following standard procedures. Specifically, the cell pellet was resuspended in TES buffer (0.2&#xa0;M TRIS, pH 8, 0.5&#xa0;mM EDTA, 0.5&#xa0;M sucrose) supplemented with one protease inhibitor tablet (Roche). Osmotic shock was performed by the addition of diluted TES buffer to release the periplasmic proteins. The solution was first centrifuged for 20&#xa0;min at 10,000 &#xd7; <italic>g</italic> and additionally for 30&#xa0;min at 100,000 &#xd7; <italic>g</italic>. The supernatant was applied to CaptureSelect beads (Thermo Fisher Scientific), which were equilibrated with wash buffer (20&#xa0;mM NaPi, pH 7.5, 20&#xa0;mM NaCl). After three column volumes of washing, the nanobody was eluted with 20&#xa0;mM HEPES, pH 7.5, 1.5&#xa0;M MgCl<sub>2</sub>. The nanobodies were further purified on a HiLoad 16/600 Superdex 75&#xa0;pg column in 20&#xa0;mM HEPES, pH 7.5, 150&#xa0;mM NaCl, 5% glycerol, concentrated with a 5&#xa0;kDa cut-off concentrator, flash-frozen and stored at -80&#xb0;C until further use.</p>
</sec>
<sec id="s3-2">
<title>3.3 Expression and Purification of Macrobody 26</title>
<p>The nanobody 26 (Nb26) was first inserted into a pBXNPH3 vector containing a C-terminal penta-histidine tag preceded of a HRV-3C protease recognition sequence. The maltose binding protein (MBP) was then inserted in frame with the 3&#x2019; end of the nanobody, with two proline residues as a linker between the two genes similar as described in (Botte et al., 2021). The resulting Pro-macrobody 26 (Mb26) was expressed in <italic>E. coli</italic> WK6 cells as above. The cell pellet was resuspended in TES buffer (0.2&#xa0;M TRIS, pH 8, 0.5&#xa0;mM EDTA, 0.5&#xa0;M sucrose) supplemented with one protease inhibitor tablet (Roche). Osmotic shock was performed by the addition of diluted TES buffer to release the periplasmic proteins. The solution was first centrifuged for 20&#xa0;min at 10,000 &#xd7; <italic>g</italic> and additionally for 30&#xa0;min at 142,000 &#xd7; <italic>g</italic>. The supernatant was further purified by immobilized-metal affinity chromatography (IMAC) on a gravity column. The beads were pre-equilibrated in 20&#xa0;mM NaPi at pH 7.5, 300&#xa0;mM NaCl, 5% glycerol, 15-30&#xa0;mM imidazole, 0.5&#xa0;mM TCEP and incubated. Loaded beads were washed with increasing imidazole concentrations (20&#xa0;mM NaPi at pH 7.5, 300&#xa0;mM NaCl, 5% glycerol, 15-30&#xa0;mM imidazole, 0.5&#xa0;mM TCEP, 0.03% DDM). The proteins were eluted from the column with a buffer containing high imidazole concentration (20&#xa0;mM NaPi at pH 7.5, 150&#xa0;mM NaCl, 5% glycerol, 250&#xa0;mM imidazole, 0.5&#xa0;mM TCEP, 0.03% DDM) and combined with 1&#xa0;mg of 3C protease to perform the His-tag cleavage. The cleaved protein was recovered by negative IMAC, concentrated to 0.5&#xa0;ml using a 30&#xa0;kDa concentrator (Corning<sup>&#xae;</sup> Spin-X<sup>&#xae;</sup> UF concentrators) and run on an &#xc4;KTA Pure system (GE Healthcare Life Sciences), using a Superdex 75 Increase 10/300 column. Fractions containing the protein were pooled, concentrated, flash frozen and stored at -80&#xb0;C until further use.</p>
</sec>
<sec id="s3-3">
<title>3.4 Thermal Stability Measurements</title>
<p>The differential scanning fluorimetry method was used to follow the thermal unfolding event (<xref ref-type="bibr" rid="B36">Kotov et al., 2019</xref>) of Nb17, Nb26, Nb38, DtpC, DtpC-Nb17, DtpC-Nb26, DtpC-Nb38, Mb26, DtpC-Mb26, and split sfGFP-DtpC<sub>1-475</sub>-Nb26 with a Prometheus NT.48 device (NanoTemper Technologies, Munich, Germany). The purified proteins were diluted to 16 &#xb5;M, and the complexes were formed using a 1:1.5&#xa0;M ratio of membrane protein: fiducial. The fluorescence at 330 and 350&#xa0;nm was recorded over a temperature gradient scan from 15&#xb0; to 95&#xb0;C and processed in GraphPad Prism 9.0 (GraphPad Software).</p>
</sec>
<sec id="s3-4">
<title>3.5 AlphaFold2 Predictions</title>
<p>Structures with the following sequences were used as input for AlphaFold2 structure prediction (<xref ref-type="bibr" rid="B34">Jumper et al., 2021</xref>), and AMBER relaxation. The best ranked models were used for visualization.</p>
<sec id="s3-4-1">
<title>3.5.1 Split sfGFP-DtpC<sub>1-475</sub>
</title>
<p>MSKGEELFTGVVPILVELDGDVNGHKFSVRGEGEGDATNGKLTLKFICTTGKLPVPWPTLVTTLTYGVQCFSRYPDHMKRHDFFKSAMPEGYVQERTISFKDDGTYKTRAEVKFEGDTLVNRIELKGIDFKEDGNILGHKLEYNKTPSQPRAIYYIVAIQIWEYFSFYGMRALLILYLTHQLGFDDNHAISLFSAYASLVYVTPILGGWLADRLLGNRTAVIAGALLMTLGHVVLGIDTNSTFSLYLALAIIICGYGLFKSNISCLLGELYDENDHRRDGGFSLLYAAGNIGSIAAPIACGLAAQWYGWHVGFALAGGGMFIGLLIFLSGHRHFQSTRSMDKKALTSVKFALPVWSWLVVMLCLAPVFFTLLLENDWSGYLLAIVCLIAAQIIARMMIKFPEHRRALWQIVLLMFVGTLFWVLAQQGGSTISLFIDRFVNRQAFNIEVPTALFQSVNAIAVMLAGVVLAWLASPESRGNSTLRVWLKFAFGLLLMACGFMLLAFDARHAAADGQASMGVMISGLALMGFAELFIDPVAIAQITRLKMSGVLTGIYMLATGAVANWLAGVVAQQTTESQISGMAIAAYQRFFSQMGEWTLACVAIIVVLAFATRFLFSTPNSHNVYITADKQKNGIKANFKIRHNVEDGSVQLADHYQQNTPIGDGPVLLPDNHYLSTQSVLSKDPNEKRDHMVLLEFVTAAGITHGMDELYK.</p>
</sec>
<sec id="s3-4-2">
<title>3.5.2 Split sfGFP-DtpC<sub>FL</sub>
</title>
<p>MSKGEELFTGVVPILVELDGDVNGHKFSVRGEGEGDATNGKLTLKFICTTGKLPVPWPTLVTTLTYGVQCFSRYPDHMKRHDFFKSAMPEGYVQERTISFKDDGTYKTRAEVKFEGDTLVNRIELKGIDFKEDGNILGHKLEYNKTPSQPRAIYYIVAIQIWEYFSFYGMRALLILYLTHQLGFDDNHAISLFSAYASLVYVTPILGGWLADRLLGNRTAVIAGALLMTLGHVVLGIDTNSTFSLYLALAIIICGYGLFKSNISCLLGELYDENDHRRDGGFSLLYAAGNIGSIAAPIACGLAAQWYGWHVGFALAGGGMFIGLLIFLSGHRHFQSTRSMDKKALTSVKFALPVWSWLVVMLCLAPVFFTLLLENDWSGYLLAIVCLIAAQIIARMMIKFPEHRRALWQIVLLMFVGTLFWVLAQQGGSTISLFIDRFVNRQAFNIEVPTALFQSVNAIAVMLAGVVLAWLASPESRGNSTLRVWLKFAFGLLLMACGFMLLAFDARHAAADGQASMGVMISGLALMGFAELFIDPVAIAQITRLKMSGVLTGIYMLATGAVANWLAGVVAQQTTESQISGMAIAAYQRFFSQMGEWTLACVAIIVVLAFATRFLFSTPTNMIQESNDNSHNVYITADKQKNGIKANFKIRHNVEDGSVQLADHYQQNTPIGDGPVLLPDNHYLSTQSVLSKDPNEKRDHMVLLEFVTAAGITHGMDELYK.</p>
</sec>
<sec id="s3-4-3">
<title>3.5.3 Split sfGFP-DtpC<sub>&#x2b;5Gly</sub>
</title>
<p>MSKGEELFTGVVPILVELDGDVNGHKFSVRGEGEGDATNGKLTLKFICTTGKLPVPWPTLVTTLTYGVQCFSRYPDHMKRHDFFKSAMPEGYVQERTISFKDDGTYKTRAEVKFEGDTLVNRIELKGIDFKEDGNILGHKLEYNKTPSQPRAIYYIVAIQIWEYFSFYGMRALLILYLTHQLGFDDNHAISLFSAYASLVYVTPILGGWLADRLLGNRTAVIAGALLMTLGHVVLGIDTNSTFSLYLALAIIICGYGLFKSNISCLLGELYDENDHRRDGGFSLLYAAGNIGSIAAPIACGLAAQWYGWHVGFALAGGGMFIGLLIFLSGHRHFQSTRSMDKKALTSVKFALPVWSWLVVMLCLAPVFFTLLLENDWSGYLLAIVCLIAAQIIARMMIKFPEHRRALWQIVLLMFVGTLFWVLAQQGGSTISLFIDRFVNRQAFNIEVPTALFQSVNAIAVMLAGVVLAWLASPESRGNSTLRVWLKFAFGLLLMACGFMLLAFDARHAAADGQASMGVMISGLALMGFAELFIDPVAIAQITRLKMSGVLTGIYMLATGAVANWLAGVVAQQTTESQISGMAIAAYQRFFSQMGEWTLACVAIIVVLAFATRFLFSTPTNMIQESNDGGGGGNSHNVYITADKQKNGIKANFKIRHNVEDGSVQLADHYQQNTPIGDGPVLLPDNHYLSTQSVLSKDPNEKRDHMVLLEFVTAAGITHGMDELYK.</p>
</sec>
</sec>
<sec id="s3-5">
<title>3.6 Cryo-EM Sample Preparation, Data Collection, Image Analysis, and Atomic Modelling</title>
<p>One hour before vitrification, the purified protein complexes were thawed on ice and run on a Superdex Increase 200 5/150 column in 0.015% DDM, 100&#xa0;mM NaCl, 10&#xa0;mM HEPES (pH 7.5), 0.5&#xa0;mM TCEP in order to remove the excess of empty detergent micelles earlier generated upon sample concentration. The top fraction reached a concentration ranging between 3 and 6&#xa0;mg/ml, and for each sample, 3.6&#xa0;&#x3bc;l were applied to glow-discharged gold holey carbon 2/1 300-mesh grids (Quantifoil). Grids were blotted for 4&#xa0;s at 0 force and 1-s wait time before being vitrified in liquid propane using a Mark IV Vitrobot (Thermo Fisher Scientific). The blotting chamber was maintained at 4&#xb0;C and 100% humidity during freezing.</p>
<p>All movies were collected using a Titan Krios (Thermo Fisher Scientific) outfitted with a K3 camera and BioQuantum energy filter (Gatan) set to 10&#xa0;eV. Automated data acquisitions were set using EPU (Thermo Fisher Scientific). The applied defocus ranged between -0.9&#xa0;&#xb5;m and -1.8&#xa0;&#xb5;m in all datasets.</p>
<p>For DtpC-Nb26 and DtpC-Mb26, movies were collected at a nominal magnification of &#xd7;105,000 and a physical pixel size of 0.85&#xa0;&#xc5;, with a 70-&#x3bc;m C2 aperture and 100-&#x3bc;m objective aperture at a dose rate of 19.5 e&#x2212;/pixel per second. A total dose of 75 e&#x2212;/&#xc5;<sup>2</sup> was used with 2.8&#xa0;s exposure time, fractionated in 50 frames. For split sfGFP-DtpC<sub>1-475</sub>-Nb26, movies were collected at a nominal magnification of &#xd7;,130,000 and a physical pixel size of 0.67&#xa0;&#xc5;, with a 50-&#x3bc;m C2 aperture and 100-&#x3bc;m objective aperture at a dose rate of 19.0 e&#x2212;/pixel per second. A total dose of 57 e&#x2212;/&#xc5;<sup>2</sup> was used with 3&#xa0;s exposure time fractionated in 40 frames.</p>
<p>All movies were motion-corrected using Relion-3.1 (<xref ref-type="bibr" rid="B62">Scheres, 2012</xref>; <xref ref-type="bibr" rid="B78">Zivanov et al., 2018</xref>) own implementation of MotionCor2 (<xref ref-type="bibr" rid="B77">Zheng et al., 2017</xref>). Contrast transfer function parameters were calculated using CTFFIND4 (<xref ref-type="bibr" rid="B60">Rohou and Grigorieff, 2015</xref>) and putative particle coordinates were initially defined using CrYOLO (<xref ref-type="bibr" rid="B73">Wagner et al., 2019</xref>).</p>
<p>For DtpC-Mb26, 13,257 movies were collected, 3,062,337 coordinates were picked and used for 2D averaging and clustering. For split sfGFP-DtpC<sub>1-475</sub>-Nb26, 7602 movies were collected, 1,049,399 coordinates were picked and used for 2D averaging and clustering. For DtpC-Nb26, 24,333 movies were collected, 6,464,070 coordinates were picked and used for 2D averaging and clustering, and 878,428 particles were used in the final 3D reconstruction. Briefly, DtpC-Nb26 dimeric population was clustered using 3D class averaging in Relion3.1 (<xref ref-type="bibr" rid="B62">Scheres, 2012</xref>). Particle trajectories and cumulative beam damage were further corrected by Bayesian polishing in Relion3.1 (<xref ref-type="bibr" rid="B79">Zivanov et al., 2019</xref>), and the resulting shiny particles were exported to cryoSPARCv3 (<xref ref-type="bibr" rid="B56">Punjani et al., 2017</xref>) for further 3D clustering via successive heterogeneous refinement cycles using &#x201c;bad&#x201d; and &#x201c;good&#x201d; volumes as references to denoise the dataset. Non uniform refinement (<xref ref-type="bibr" rid="B57">Punjani et al., 2020</xref>), followed by a local refinement using a soft mask around one transporter unit resulted in a 2.7&#xa0;&#xc5; reconstruction of DtpC. The overall resolution was estimated in CryoSPARCv3 using the FSC &#x3d; 0.143 cutoff. Local resolution estimations were also calculated in CryoSPARCv3 using the 0.5 FSC cutoff. The two half maps were used as inputs to assess various post-processing strategies such as the CryoSPARC&#x2019;s sharpening tool, DeepEMhancer (<xref ref-type="bibr" rid="B61">Sanchez-Garcia et al., 2021</xref>), and Resolve_cryo-em (<xref ref-type="bibr" rid="B69">Terwilliger et al., 2020</xref>). The latter led to a slightly better defined contour of the atoms, and was subsequently used for the last atomic-model refinement of DtpC. The initial models of DtpC and Nb26 were generated using AlphaFold2, and refined against the experimental maps; first in Isolde (<xref ref-type="bibr" rid="B12">Croll, 2018</xref>), and last in Phenix (<xref ref-type="bibr" rid="B2">Afonine et al., 2018</xref>), principally to refine atomic displacement parameters (B-factors) and perform a slight energy minimization while keeping restrains from Isolde&#x2019;s reference model. Half-maps, and postprocessed maps of the dimeric arrangement and of the focused refinement, as well as the atomic model of DtpC were deposited in the PDB and EMDB as deposition numbers 7ZC2, and EMD-14618. The atomic model of the dimeric DtpC-Nb26 is available upon request.</p>
</sec>
<sec id="s3-6">
<title>3.7 Small-Angle X-Ray Scattering Data Collection and Analysis</title>
<p>Synchrotron SAXS data from solutions of DtpC-Nb26 in &#x3b2;-DDM micelles (SEC-SAXS) were collected on the EMBL P12 (<xref ref-type="bibr" rid="B4">Blanchet et al., 2015</xref>) beamline at the PETRA III storage ring (Hamburg, Germany), in a buffer consisting of 0.015% DDM, 100&#xa0;mM NaCl, 10&#xa0;mM HEPES (pH 7.5), and 0.5&#xa0;mM TCEP. Sample (10&#xa0;mg/ml) was injected onto a Superdex Increase 200 10/300 column (Cytiva) and run at 0.5&#xa0;ml/min at 20&#xb0;C. 3000 successive 1&#xa0;s frames were collected using a Pilatus 2M detector at a sample-detector distance of 3.1&#xa0;m and at a wavelength of &#x3bb; &#x3d; 0.124&#xa0;nm (I(s) vs. s, where s &#x3d; 4&#x3c0;sin&#x3b8;/&#x3bb;, and 2&#x3b8; is the scattering angle). The data were normalized to the intensity of the transmitted beam and radially averaged; the scattering of the solvent-blank was subtracted using CHROMIXS (<xref ref-type="bibr" rid="B47">Panjkovich and Svergun, 2018</xref>). Cryo-EM volume maps of DtpC-Nb26 were fit to the scattering data across the low-angle range (shape region only) using EM2DAM (<xref ref-type="bibr" rid="B20">Franke et al., 2017</xref>) at a density threshold of 0.1.</p>
</sec>
<sec id="s3-7">
<title>3.8 Data Visualization</title>
<p>Graphs were generated using GraphPad Prism 9.0 (GraphPad Software). Molecular graphics and analyses performed with UCSF ChimeraX-1.2.5 (<xref ref-type="bibr" rid="B50">Pettersen et al., 2021</xref>). Figures were prepared in Adobe Illustrator 2021.</p>
</sec>
</sec>
</body>
<back>
<sec id="s4" sec-type="data-availability">
<title>Data Availability Statement</title>
<p>The datasets presented in this study can be found in online repositories. The names of the repository/repositories and accession number(s) can be found below: <ext-link ext-link-type="uri" xlink:href="http://www.wwpdb.org/">http://www.wwpdb.org/</ext-link>, 7ZC2 <ext-link ext-link-type="uri" xlink:href="https://www.ebi.ac.uk/pdbe/emdb/">https://www.ebi.ac.uk/pdbe/emdb/</ext-link>, EMD-14618.</p>
</sec>
<sec id="s5">
<title>Author Contributions</title>
<p>Conceptualization: MK, CL. Methodology: MK, GF, HM, EP. Investigation: MK, GF, HM, EP. Visualization: MK, HM. Funding acquisition: DS, JS, CL. Project administration: CL. Supervision: DS, JS, CL. Writing&#x2014;original draft: MK, CL. Writing&#x2014;review and editing: MK, GF, HM, DS, EP, JS, CL.</p>
</sec>
<sec id="s6">
<title>Funding</title>
<p>This work was supported by a grant from the BMBF (grant number: 05K18YEA). Part of this work was performed at the CryoEM Facility at CSSB, supported by the UHH and DFG grant numbers (INST 152/772&#x2013;1&#x7c;152/774&#x2013;1&#x7c;152/775&#x2013;1&#x7c;152/776&#x2013;1&#x7c;152/777&#x2013;1 FUGG).</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<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 sec-type="disclaimer" id="s8">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<ack>
<p>We thank the Sample Preparation and Characterization facility of EMBL Hamburg for support in this project and the beamlines P13 and P14 at EMBL Hamburg for regular access. We acknowledge Instruct-ERIC and the FWO for their support to the Nb discovery and Saif Saifuzzaman for the technical assistance during Nb discovery. All past and current group members are acknowledged for their input to this manuscript and their efforts to crystallize DtpC over the years.</p>
</ack>
<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/fmolb.2022.917725/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmolb.2022.917725/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet1.PDF" id="SM1" mimetype="application/PDF" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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