<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD with MathML3 v1.2 20190208//EN"  "JATS-archivearticle1-mathml3.dtd"><article xmlns:ali="http://www.niso.org/schemas/ali/1.0/" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" dtd-version="1.2"><front><journal-meta><journal-id journal-id-type="nlm-ta">elife</journal-id><journal-id journal-id-type="publisher-id">eLife</journal-id><journal-title-group><journal-title>eLife</journal-title></journal-title-group><issn publication-format="electronic" pub-type="epub">2050-084X</issn><publisher><publisher-name>eLife Sciences Publications, Ltd</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="publisher-id">84179</article-id><article-id pub-id-type="doi">10.7554/eLife.84179</article-id><article-categories><subj-group subj-group-type="display-channel"><subject>Short Report</subject></subj-group><subj-group subj-group-type="heading"><subject>Neuroscience</subject></subj-group></article-categories><title-group><article-title>Mechanotransduction events at the physiological site of touch detection</article-title></title-group><contrib-group><contrib contrib-type="author" id="author-296576"><name><surname>Ziolkowski</surname><given-names>Luke H</given-names></name><contrib-id authenticated="true" contrib-id-type="orcid">https://orcid.org/0000-0002-3420-6782</contrib-id><xref ref-type="aff" rid="aff1">1</xref><xref ref-type="fn" rid="con1"/><xref ref-type="fn" rid="conf1"/></contrib><contrib contrib-type="author" corresp="yes" id="author-52803"><name><surname>Gracheva</surname><given-names>Elena O</given-names></name><contrib-id authenticated="true" contrib-id-type="orcid">https://orcid.org/0000-0002-0846-3427</contrib-id><email>elena.gracheva@yale.edu</email><xref ref-type="aff" rid="aff1">1</xref><xref ref-type="aff" rid="aff2">2</xref><xref ref-type="aff" rid="aff3">3</xref><xref ref-type="aff" rid="aff4">4</xref><xref ref-type="other" rid="fund3"/><xref ref-type="fn" rid="con2"/><xref ref-type="fn" rid="conf2"/></contrib><contrib contrib-type="author" corresp="yes" id="author-74872"><name><surname>Bagriantsev</surname><given-names>Sviatoslav N</given-names></name><contrib-id authenticated="true" contrib-id-type="orcid">https://orcid.org/0000-0002-6661-3403</contrib-id><email>slav.bagriantsev@yale.edu</email><xref ref-type="aff" rid="aff1">1</xref><xref ref-type="other" rid="fund1"/><xref ref-type="other" rid="fund2"/><xref ref-type="other" rid="fund4"/><xref ref-type="other" rid="fund5"/><xref ref-type="fn" rid="con3"/><xref ref-type="fn" rid="conf1"/></contrib><aff id="aff1"><label>1</label><institution-wrap><institution-id institution-id-type="ror">https://ror.org/03v76x132</institution-id><institution>Department of Cellular and Molecular Physiology, Yale University School of Medicine</institution></institution-wrap><addr-line><named-content content-type="city">New Haven</named-content></addr-line><country>United States</country></aff><aff id="aff2"><label>2</label><institution-wrap><institution-id institution-id-type="ror">https://ror.org/03v76x132</institution-id><institution>Department of Neuroscience, Yale University School of Medicine</institution></institution-wrap><addr-line><named-content content-type="city">New Haven</named-content></addr-line><country>United States</country></aff><aff id="aff3"><label>3</label><institution-wrap><institution-id institution-id-type="ror">https://ror.org/03v76x132</institution-id><institution>Program in Cellular Neuroscience, Neurodegeneration and Repair, Yale University School of Medicine</institution></institution-wrap><addr-line><named-content content-type="city">New Haven</named-content></addr-line><country>United States</country></aff><aff id="aff4"><label>4</label><institution-wrap><institution-id institution-id-type="ror">https://ror.org/03v76x132</institution-id><institution>Kavli Institute for Neuroscience, Yale University School of Medicine</institution></institution-wrap><addr-line><named-content content-type="city">New Haven</named-content></addr-line><country>United States</country></aff></contrib-group><contrib-group content-type="section"><contrib contrib-type="editor"><name><surname>Giraldez</surname><given-names>Teresa</given-names></name><role>Reviewing Editor</role><aff><institution-wrap><institution-id institution-id-type="ror">https://ror.org/01r9z8p25</institution-id><institution>University of La Laguna</institution></institution-wrap><country>Spain</country></aff></contrib><contrib contrib-type="senior_editor"><name><surname>Aldrich</surname><given-names>Richard W</given-names></name><role>Senior Editor</role><aff><institution-wrap><institution-id institution-id-type="ror">https://ror.org/00hj54h04</institution-id><institution>The University of Texas at Austin</institution></institution-wrap><country>United States</country></aff></contrib></contrib-group><pub-date publication-format="electronic" date-type="publication"><day>06</day><month>01</month><year>2023</year></pub-date><pub-date pub-type="collection"><year>2023</year></pub-date><volume>12</volume><elocation-id>e84179</elocation-id><history><date date-type="received" iso-8601-date="2022-10-13"><day>13</day><month>10</month><year>2022</year></date><date date-type="accepted" iso-8601-date="2022-12-21"><day>21</day><month>12</month><year>2022</year></date></history><pub-history><event><event-desc>This manuscript was published as a preprint at bioRxiv.</event-desc><date date-type="preprint" iso-8601-date="2022-10-24"><day>24</day><month>10</month><year>2022</year></date><self-uri content-type="preprint" xlink:href="https://doi.org/10.1101/2022.10.23.513402"/></event></pub-history><permissions><copyright-statement>© 2023, Ziolkowski et al</copyright-statement><copyright-year>2023</copyright-year><copyright-holder>Ziolkowski et al</copyright-holder><ali:free_to_read/><license xlink:href="http://creativecommons.org/licenses/by/4.0/"><ali:license_ref>http://creativecommons.org/licenses/by/4.0/</ali:license_ref><license-p>This article is distributed under the terms of the <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution License</ext-link>, which permits unrestricted use and redistribution provided that the original author and source are credited.</license-p></license></permissions><self-uri content-type="pdf" xlink:href="elife-84179-v2.pdf"/><abstract><p>Afferents of peripheral mechanoreceptors innervate the skin of vertebrates, where they detect physical touch via mechanically gated ion channels (mechanotransducers). While the afferent terminal is generally understood to be the primary site of mechanotransduction, the functional properties of mechanically activated (MA) ionic current generated by mechanotransducers at this location remain obscure. Until now, direct evidence of MA current and mechanically induced action potentials in the mechanoreceptor terminal has not been obtained. Here, we report patch-clamp recordings from the afferent terminal innervating Grandry (Meissner) corpuscles in the bill skin of a tactile specialist duck. We show that mechanical stimulation evokes MA current in the afferent with fast kinetics of activation and inactivation during the dynamic phases of the mechanical stimulus. These responses trigger rapidly adapting firing in the afferent detected at the terminal and in the afferent fiber outside of the corpuscle. Our findings elucidate the initial electrogenic events of touch detection in the mechanoreceptor nerve terminal.</p></abstract><kwd-group kwd-group-type="author-keywords"><kwd>mechanosensitivity</kwd><kwd>mechanosensation</kwd><kwd>Meissner corpuscle</kwd><kwd>Grandry corpuscle</kwd><kwd>duck</kwd><kwd><italic>Anas platyrhynchos</italic></kwd></kwd-group><kwd-group kwd-group-type="research-organism"><title>Research organism</title><kwd>Other</kwd><kwd>Mallard</kwd></kwd-group><funding-group><award-group id="fund1"><funding-source><institution-wrap><institution-id institution-id-type="FundRef">http://dx.doi.org/10.13039/100000001</institution-id><institution>National Science Foundation</institution></institution-wrap></funding-source><award-id>1923127</award-id><principal-award-recipient><name><surname>Bagriantsev</surname><given-names>Sviatoslav N</given-names></name></principal-award-recipient></award-group><award-group id="fund2"><funding-source><institution-wrap><institution-id institution-id-type="FundRef">http://dx.doi.org/10.13039/100000001</institution-id><institution>National Science Foundation</institution></institution-wrap></funding-source><award-id>2114084</award-id><principal-award-recipient><name><surname>Bagriantsev</surname><given-names>Sviatoslav N</given-names></name></principal-award-recipient></award-group><award-group id="fund3"><funding-source><institution-wrap><institution-id institution-id-type="FundRef">http://dx.doi.org/10.13039/100000001</institution-id><institution>National Science Foundation</institution></institution-wrap></funding-source><award-id>1754286</award-id><principal-award-recipient><name><surname>Gracheva</surname><given-names>Elena O</given-names></name></principal-award-recipient></award-group><award-group id="fund4"><funding-source><institution-wrap><institution-id institution-id-type="FundRef">http://dx.doi.org/10.13039/100000002</institution-id><institution>National Institutes of Health</institution></institution-wrap></funding-source><award-id>R01NS097547</award-id><principal-award-recipient><name><surname>Bagriantsev</surname><given-names>Sviatoslav N</given-names></name></principal-award-recipient></award-group><award-group id="fund5"><funding-source><institution-wrap><institution-id institution-id-type="FundRef">http://dx.doi.org/10.13039/100000002</institution-id><institution>National Institutes of Health</institution></institution-wrap></funding-source><award-id>R01NS126277</award-id><principal-award-recipient><name><surname>Bagriantsev</surname><given-names>Sviatoslav N</given-names></name></principal-award-recipient></award-group><funding-statement>The funders had no role in study design, data collection and interpretation, or the decision to submit the work for publication.</funding-statement></funding-group><custom-meta-group><custom-meta specific-use="meta-only"><meta-name>Author impact statement</meta-name><meta-value>A novel experimental approach reveals how mechanical force acting on the skin is converted into electrical signaling in sensory neurons to evoke the sensation of touch.</meta-value></custom-meta></custom-meta-group></article-meta></front><body><sec id="s1" sec-type="intro"><title>Introduction</title><p>In vertebrates, extrinsic touch is detected in the skin by cutaneous mechanoreceptors and somatosensory neurons of the peripheral nervous system. The afferent nerve fibers of these cells innervate the skin, where they form specialized ending structures which sense mechanical stimuli. Within the afferent terminals, mechanically gated ion channels (mechanotransducers), such as Piezo2, detect touch and transform it into mechanically activated (MA) current (<xref ref-type="bibr" rid="bib3">Handler and Ginty, 2021</xref>). Extracellular recordings of mechanoreceptor afferents have previously revealed voltage changes originating from the terminals in response to mechanical stimulation, but the intracellular dynamics of these signals are not understood (<xref ref-type="bibr" rid="bib5">Loewenstein and Rathkamp, 1958</xref>). As a result, direct evidence of mechanotransduction and MA current in the nerve endings of mechanoreceptors is lacking.</p><p>Studies of MA current and mechanotransducer biophysics have been limited to heterologous expression systems and dissociated somatosensory neurons <italic>in vitro</italic> (<xref ref-type="bibr" rid="bib2">Coste et al., 2010</xref>; <xref ref-type="bibr" rid="bib4">Lewis et al., 2017</xref>; <xref ref-type="bibr" rid="bib10">Schneider et al., 2017</xref>; <xref ref-type="bibr" rid="bib15">Zheng et al., 2019</xref>). Most notably, Piezo2, which mediates the detection of touch, displays fast-inactivating MA current in cultured cells and in dissociated neurons (<xref ref-type="bibr" rid="bib13">von Buchholtz et al., 2021</xref>; <xref ref-type="bibr" rid="bib1">Chesler et al., 2016</xref>; <xref ref-type="bibr" rid="bib2">Coste et al., 2010</xref>; <xref ref-type="bibr" rid="bib8">Ranade et al., 2014</xref>; <xref ref-type="bibr" rid="bib14">Wang et al., 2019</xref>). However, it is unclear whether electrophysiological responses from somas of dissociated neurons accurately reflect that of MA current in the afferent terminal in the skin, due to potential differences in membrane geometry, level of ion channel expression, intracellular factors, and cellular/tissue environment between the two (<xref ref-type="bibr" rid="bib9">Richardson et al., 2022</xref>). To our knowledge, intracellular recordings of mechanoreceptor terminals have not been previously reported due to the technical difficulties of accessing the axonal endings with patch-clamp electrodes. Consequently, the functional characteristics of mechanotransduction at the normal physiological site of touch detection remain unknown.</p><p>To address this gap in knowledge, we acquired patch-clamp recordings from the afferent terminals of Grandry (Meissner) corpuscles in the bill skin of the tactile specialist Mallard duck (<italic>Anas platyrhynchos domesticus</italic>). The Grandry corpuscle is an avian tactile end-organ innervated by rapidly adapting mechanoreceptors, which form thin terminals between Schwann cell-derived lamellar cells (<xref ref-type="bibr" rid="bib7">Nikolaev et al., 2020</xref>; <xref ref-type="bibr" rid="bib10">Schneider et al., 2017</xref>). The Grandry corpuscle’s layered architecture, rapid adaptation, and sensitivity to transient touch make it structurally and functionally analogous to the mammalian Meissner corpuscle (<xref ref-type="bibr" rid="bib6">Neubarth et al., 2020</xref>; <xref ref-type="bibr" rid="bib11">Schwaller et al., 2021</xref>; <xref ref-type="bibr" rid="bib16">Ziolkowski et al., 2022</xref>). Compared to mammals, the high density of corpuscles in the bill of tactile-foraging waterfowl enables persistent electrophysiological investigation of the afferent terminals in these end-organs, the results of which we report here.</p></sec><sec id="s2" sec-type="results|discussion"><title>Results and discussion</title><p>We acquired patch-clamp recordings from the afferent terminal within the Grandry corpuscle using an <italic>ex vivo</italic> bill-skin preparation from late-stage duck embryos (<xref ref-type="fig" rid="fig1">Figure 1A</xref>). Mechanical stimulation of the voltage-clamped afferent terminal revealed fast-inactivating MA current only in response to the dynamic onset (ON) and offset (OFF) phases of the stimulus (<xref ref-type="fig" rid="fig1">Figure 1B</xref>). In current-clamp, both indentation with a probe (<xref ref-type="fig" rid="fig1">Figure 1C</xref>) and current injection (<xref ref-type="fig" rid="fig1">Figure 1D</xref>) caused depolarization of the membrane voltage, which initiated action potentials (APs) in the terminal during both phases. In three corpuscles in which the afferent terminal was patched, simultaneous single-fiber nerve recordings were also established using a section of the same afferent outside of the corpuscle (<xref ref-type="fig" rid="fig1">Figure 1A and E</xref>). In these cases, propagating APs from the afferent terminal were recorded in the afferent fiber with a one-to-one correlation to APs in the terminal (<xref ref-type="fig" rid="fig1">Figure 1B–D</xref>, bottom). When comparing the responses during the ON and OFF phases, we detected a difference between the rates of current inactivation (<xref ref-type="fig" rid="fig1">Figure 1F</xref>), but not the rates of activation, current-indentation relationship, or AP threshold (<xref ref-type="fig" rid="fig1">Figure 1E–I</xref>). The inactivation rate of MA current in the ON phase (<italic>τ</italic>=8.95 ± 1.82 ms) in the terminal is notably similar to the inactivation rate of fast-inactivating MA current measured from the somas of murine and duck mechanoreceptors <italic>in vitro</italic> (<xref ref-type="bibr" rid="bib2">Coste et al., 2010</xref>; <xref ref-type="bibr" rid="bib10">Schneider et al., 2017</xref>; <xref ref-type="bibr" rid="bib12">Viatchenko-Karpinski and Gu, 2016</xref>). Though duck Piezo2 also displays fast-inactivating MA current (<italic>τ</italic>&lt;10 ms at negative membrane potentials; <xref ref-type="bibr" rid="bib10">Schneider et al., 2017</xref>), whether the ON phase MA current in the terminal is mediated by Piezo2 or another, unknown ion channel remains to be determined. Interestingly, the MA current seen during the OFF phase is a unique response not reported in dissociated neurons or expression systems, even though the OFF response is typical of rapidly adapting mechanoreceptors in <italic>ex vivo</italic> single-fiber recordings. The fast inactivation rate of the OFF response compared to the ON response implies a distinct or modified mechanism of mechanotransduction. This could potentially be dependent on the cellular structure or function of lamellar cells in the corpuscle.</p><fig id="fig1" position="float"><label>Figure 1.</label><caption><title>Mechanotransduction in the afferent terminal of the Grandry (Meissner) corpuscle.</title><p>(<bold>A</bold>) Illustrated representation of the experimental setup. (<bold>B</bold>) The mechanical step stimulus applied with a glass probe (top), representative mechanically activated (MA) current responses in the terminal while voltage-clamped at –60 mV (middle), and simultaneous extracellular voltage signal from the connected afferent (bottom). (<bold>C</bold>) The mechanical stimulus (top), voltage responses and action potentials (APs) in the terminal in current-clamp (middle), and APs measured further along the afferent (bottom). (<bold>D</bold>) The current injection stimulus (top), voltage responses and action potentials in the terminal in current-clamp (middle), and APs measured in the afferent (bottom). (<bold>E</bold>) Example bright-field image of the experimental setup. (<bold>F</bold>) Quantification of the kinetics of MA current inactivation, (<bold>G</bold>) activation, (<bold>H</bold>) peak MA current-indentation relationship (n=7/6 afferent terminals for onset [ON]/offset [OFF], respectively), and (<bold>I</bold>) AP threshold measured in the dynamic ON phase of the stimulus and the dynamic OFF phase of the stimulus. Only the difference in inactivation τ between the ON and OFF phase was statistically significant (p&lt;0.05). Statistics: Mann-Whitney U test (<bold>F, G, and I</bold>) or two-way ANOVA (<bold>H</bold>). Symbols indicate data from individual cells. Data in F–I were obtained from at least three independent skin preparations and shown as mean ± SEM.</p><p><supplementary-material id="fig1sdata1"><label>Figure 1—source data 1.</label><caption><title>Original data for <xref ref-type="fig" rid="fig1">Figure 1F–I</xref>.</title></caption><media mimetype="application" mime-subtype="xlsx" xlink:href="elife-84179-fig1-data1-v2.xlsx"/></supplementary-material></p></caption><graphic mimetype="image" mime-subtype="tiff" xlink:href="elife-84179-fig1-v2.tif"/></fig><p>As expected, the addition of tetrodotoxin (TTX) to the bill-skin preparation blocked APs and voltage-gated sodium current in the afferent terminal (<xref ref-type="fig" rid="fig2">Figure 2A–D</xref>). In some voltage-clamp experiments, mechanical stimulation resulted in large (&gt;1000 pA) depolarizing currents (<xref ref-type="fig" rid="fig2">Figure 2C</xref>) which did not follow the expected current-indentation relationship (<xref ref-type="fig" rid="fig1">Figure 1H</xref>). These currents were blocked by TTX and therefore were voltage-gated sodium currents resulting from a brief loss of voltage clamp, likely due to the complex geometry of the afferent.</p><fig id="fig2" position="float"><label>Figure 2.</label><caption><title>Electrogenic events in mechanoreceptor terminal and lamellar cells are carried out by different mechanisms.</title><p>(<bold>A</bold>) A suprathreshold mechanical stimulus (top), action potentials (APs) in the terminal (middle), and propagated APs from the connected afferent (bottom). (<bold>B</bold>) A suprathreshold mechanical stimulus applied in 1 μM tetrodotoxin (TTX; top), AP-absent voltage responses in the terminal in current-clamp (middle), and extracellular receptor potentials in the afferent (bottom). (<bold>C</bold>) A suprathreshold mechanical stimulus (top), current responses in the terminal while voltage-clamped at –60 mV without 1 μM TTX (middle), and with 1 μM TTX (bottom). (<bold>D</bold>) Voltage-indentation relationship in the absence or presence of 1 μM TTX (n=5 for each group). (<bold>E</bold>) The number of APs from increasing current injections in lamellar cells and afferent terminals (n=5 for each group). Inset shows exemplar action potentials from a lamellar cell (blue) and afferent (black). (<bold>F</bold>) Resting membrane potential (RMP), (<bold>G</bold>) peak AP amplitude, (<bold>H</bold>) AP width at the half-maximum, and (<bold>I</bold>) the maximum slope of the AP rise or decay in the afferent terminal versus lamellar cells of the corpuscle. The AP-current injection relationship, RMP, width at half-maximum, max rise slope, and max decay slope were significantly different between the afferent terminal and lamellar cells (p&lt;0.05). Statistics: Mann-Whitney U test (<bold>F–I</bold>) or two-way ANOVA with Holm-Sidak post-hoc test (<bold>D and E</bold>). **p=0.0084, ***p=0.0004, ****p&lt;0.0001. Symbols indicate data from individual cells. Data in D–I were obtained from at least three independent skin preparations and shown as mean ± SEM.</p><p><supplementary-material id="fig2sdata1"><label>Figure 2—source data 1.</label><caption><title>Original data for <xref ref-type="fig" rid="fig2">Figure 2D–I</xref>.</title></caption><media mimetype="application" mime-subtype="xlsx" xlink:href="elife-84179-fig2-data1-v2.xlsx"/></supplementary-material></p></caption><graphic mimetype="image" mime-subtype="tiff" xlink:href="elife-84179-fig2-v2.tif"/></fig><p>Importantly, APs in the afferent terminal are physiologically distinct from APs fired by Grandry lamellar cells (<xref ref-type="fig" rid="fig2">Figure 2E–I</xref>). Lamellar cell APs are mediated by voltage-gated calcium channels, which are insensitive to TTX (<xref ref-type="bibr" rid="bib7">Nikolaev et al., 2020</xref>). Lamellar cells fire multiple APs in response to large current injections, whereas the afferent terminal fires a maximum of one AP during the same stimuli (<xref ref-type="fig" rid="fig2">Figure 2E</xref>). Additionally, there were significant differences in resting membrane potential, AP width at half-maximum, and maximum slope of rise and decay between the two cell types. These results, along with the single-fiber afferent voltage data which mirrors the terminal voltage (<xref ref-type="fig" rid="fig1">Figure 1B–D</xref>), demonstrate that the recordings acquired here are unequivocally from the afferent terminal within the corpuscle.</p><p>Here, we have shown that mechanical stimulation evokes MA current in the afferent terminal which initiates propagating APs. Critically, MA current in the terminal has properties closely resembling those observed in dissociated neuron somas. This ultimately confirms the validity of using <italic>in vitro</italic> models to study mechanotransducers. At the same time, an important aspect of the afferent terminal response <italic>in situ</italic> is absent from cultured cells: the MA current in the OFF phase. Further studies of rapidly adapting corpuscles and other mechanoreceptor endings will be required to understand the mechanisms underlying both the OFF and ON responses. Together, these findings reveal fundamental characteristics of mechanotransduction at the physiological site of touch detection in mechanosensory neurons.</p></sec><sec id="s3" sec-type="materials|methods"><title>Materials and methods</title><table-wrap id="keyresource" position="anchor"><label>Key resources table</label><table frame="hsides" rules="groups"><thead><tr><th align="left" valign="bottom">Reagent type <break/>(species) or <break/>resource</th><th align="left" valign="bottom">Designation</th><th align="left" valign="bottom">Source or reference</th><th align="left" valign="bottom">Identifiers</th><th align="left" valign="bottom">Additional information</th></tr></thead><tbody><tr><td align="left" valign="bottom">Biological sample</td><td align="left" valign="bottom">Duck bill skin <break/>(<italic>Anas platyrhynchos <break/>domesticus</italic>)<break/></td><td align="left" valign="bottom">Metzer Farms</td><td align="left" valign="bottom"/><td align="left" valign="bottom">Embryonic day E25-E27, <break/>Sex undetermined</td></tr><tr><td align="left" valign="bottom">Software and algorithm</td><td align="left" valign="bottom">pClamp 10</td><td align="left" valign="bottom">Molecular Devices</td><td align="left" valign="bottom">RRID: <ext-link ext-link-type="uri" xlink:href="https://identifiers.org/RRID/RRID:SCR_011323">SCR_011323</ext-link></td><td align="left" valign="bottom"/></tr><tr><td align="left" valign="bottom">Software and algorithm</td><td align="left" valign="bottom">GraphPad Prism 9.4.1</td><td align="left" valign="bottom">GraphPad Software, LLC</td><td align="left" valign="bottom">RRID: <ext-link ext-link-type="uri" xlink:href="https://identifiers.org/RRID/RRID:SCR_002798">SCR_002798</ext-link></td><td align="left" valign="bottom"/></tr></tbody></table></table-wrap><sec id="s3-1"><title><italic>Ex vivo</italic> bill-skin preparation</title><p>Experiments with duck embryos (<italic>Anas platyrhynchos domesticus</italic>) were approved by and performed in accordance with guidelines of the Institutional Animal Case and Use Committee of Yale University, protocol 11526. The bill-skin preparation was slightly modified from previously published methods (<xref ref-type="bibr" rid="bib7">Nikolaev et al., 2020</xref>). Intact skin was carefully removed from the bill of duck embryos (aged embryonic day 25–27, sex not determined) using a sharp scalpel tip in ice-cold L-15 media. The bill-skin was placed upside-down (epidermis on bottom) in the recording chamber under a slice anchor. Corpuscles and afferents in the dermis were visualized on an Olympus BX51WI upright microscope with an ORCA-Flash 4.0 LT camera (Hamamatsu). At room temperature (22–23°C), the bill-skin preparation was treated for 5 min with 2 mg/mL collagenase P (Roche) in Krebs solution containing (in mM) 117 NaCl, 3.5 KCl, 2.5 CaCl<sub>2</sub>, 1.2 MgCl<sub>2</sub>, 1.2 NaH<sub>2</sub>PO<sub>4</sub>, 25 NaHCO<sub>3</sub>, and 11 glucose, saturated with 95% O<sub>2</sub> and 5% CO<sub>2</sub> (pH = 7.3–7.4), then washed with fresh Krebs solution.</p></sec><sec id="s3-2"><title>Patch-clamp electrophysiology</title><p>Recordings were acquired at room temperature using a MultiClamp 700B amplifier, Digidata 1550 A digitizer, and pClamp 10 software (Molecular Devices). Standard-wall, 1.5 mm diameter borosilicate pipettes with tip resistances of 2–5 MΩ were pulled using a P-1000 micropipette puller (Sutter Instruments). Pipettes were filled with intracellular solution containing (in mM) 135 K-gluconate, 5 KCl, 0.5 CaCl<sub>2</sub>, 2 MgCl<sub>2</sub>, 5 EGTA, 5 HEPES, 5 Na<sub>2</sub>ATP, and 0.5 Na<sub>2</sub>GTP (pH 7.3 with KOH). All experiments were performed in Krebs solution at room temperature. Data were sampled at 20 kHz and low-pass filtered at 2 kHz. Terminals were recorded in whole-cell mode and were held at –60 mV during voltage-clamp experiments. Resting membrane potential was measured in current-clamp mode shortly after breaking in. In both voltage- and current-clamp, mechanical stimuli were applied to a single corpuscle using a blunt glass probe (2–10 μm tip diameter) mounted on a piezoelectric-driven actuator (Physik Instrumente GmbH). A mechanical step stimulus was applied to corpuscles starting at 1 μm and increasing by 1 μm after each indentation. The static plateau of the step stimulus lasted 150 ms, while the ramp had a duration of 3 ms for both the ON and OFF phases. For both phases in each terminal, the inactivation rate (τ) of the MA current was calculated by fitting a single exponential function (I = I<sub>0</sub>×exp^(− <italic>t</italic>/τ), where I<sub>0</sub> is the baseline-subtracted peak current amplitude, <italic>t</italic> is the time from the peak current, and τ is the inactivation constant) to the decaying portion of the largest three MA current responses and averaging the fitted τ values. The activation τ was calculated similarly using the rise portion of the response (<xref ref-type="bibr" rid="bib7">Nikolaev et al., 2020</xref>). The threshold was measured in current-clamp as the smallest indentation which elicited an AP. In current-clamp, depolarizing current steps (from 10 to 100 pA in 10 pA increments) were applied to elicit APs in the afferent terminal and lamellar cells. The first AP in these recordings was used to calculate the peak amplitude, width at half-maximum, and maximum slope of rise and decay for the terminal versus lamellar cells. Experiments were not corrected for liquid-junction potential.</p></sec><sec id="s3-3"><title>Single-fiber recording</title><p>Recordings from single afferent fibers of corpuscles were acquired simultaneously with patch-clamp recordings for three corpuscles, using the second channel of the MultiClamp 700B amplifier. Single-fiber recording pipettes were manufactured from thin-wall, 1.5 mm diameter borosilicate glass capillaries using a P-1000 micropipette puller (Sutter Instruments) to create tip diameters of 5–30 μm, then filled with Krebs solution. Pipettes were placed on an electrode headstage connected to a High-Speed Pressure Clamp (ALA Scientific Instruments). Light (1–20 mmHg) positive pressure was applied from the recording electrode to clear away tissue from a corpuscle-associated afferent. Negative pressure was then applied until a large section (~5 μm) of the afferent was sucked into the pipette. Extracellular afferent voltage was recording in current-clamp mode, sampled at 20 kHz and low-pass filtered at 1 kHz.</p></sec><sec id="s3-4"><title>Data analysis</title><p>Data from afferent terminals and lamellar cells were acquired from separate, individual preparations from different animals. Data were analyzed and plotted in GraphPad Prism 9.4.1 (GraphPad Software, LLC) as individual data points or means ± SEM unless otherwise indicated.</p></sec></sec></body><back><sec sec-type="additional-information" id="s4"><title>Additional information</title><fn-group content-type="competing-interest"><title>Competing interests</title><fn fn-type="COI-statement" id="conf1"><p>No competing interests declared</p></fn><fn fn-type="COI-statement" id="conf2"><p>No competing interests declared</p></fn></fn-group><fn-group content-type="author-contribution"><title>Author contributions</title><fn fn-type="con" id="con1"><p>Conceptualization, Data curation, Formal analysis, Validation, Investigation, Visualization, Methodology, Writing – original draft, Writing – review and editing</p></fn><fn fn-type="con" id="con2"><p>Conceptualization, Data curation, Supervision, Funding acquisition, Methodology, Writing – original draft, Project administration, Writing – review and editing</p></fn><fn fn-type="con" id="con3"><p>Conceptualization, Data curation, Supervision, Funding acquisition, Writing – original draft, Project administration, Writing – review and editing</p></fn></fn-group><fn-group content-type="ethics-information"><title>Ethics</title><fn fn-type="other"><p>Experiments with duck embryos (Anas platyrhynchos domesticus) were approved by and performed in accordance with guidelines of the Institutional Animal Care and Use Committee of Yale University, protocol 11526.</p></fn></fn-group></sec><sec sec-type="supplementary-material" id="s5"><title>Additional files</title><supplementary-material id="mdar"><label>MDAR checklist</label><media xlink:href="elife-84179-mdarchecklist1-v2.docx" mimetype="application" mime-subtype="docx"/></supplementary-material></sec><sec sec-type="data-availability" id="s6"><title>Data availability</title><p>All data generated or analysed during this study are included in the manuscript and supporting file. Source data files have been provided for Figures 1 and 2.</p></sec><ack id="ack"><title>Acknowledgements</title><p>We thank Dr. Yury Nikolaev for help with establishing the skin preparation, and members of the SNB and EOG laboratories for their contributions throughout the project. 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specific-use="editor">Reviewing Editor</role><aff><institution-wrap><institution-id institution-id-type="ror">https://ror.org/01r9z8p25</institution-id><institution>University of La Laguna</institution></institution-wrap><country>Spain</country></aff></contrib></contrib-group></front-stub><body><p>This fundamental work by Ziolkowski et al provides an exceptional advance in our understanding of the physiological sense of touch by directly perfoming in vivo patch-clamp recordings from vertebrate skin mechanoreceptor terminals. The provided evidence is compelling, overcoming a long-existing technical challenge and providing an experimental model to investigate the neuronal response to mechanical stimulation at the site of force detection that is of broad interest to physiologists, neuroscientists and biophysicists working on mechanoreceptors and mechanically activated ion channels.</p></body></sub-article><sub-article article-type="decision-letter" id="sa1"><front-stub><article-id pub-id-type="doi">10.7554/eLife.84179.sa1</article-id><title-group><article-title>Decision letter</article-title></title-group><contrib-group content-type="section"><contrib contrib-type="editor"><name><surname>Giraldez</surname><given-names>Teresa</given-names></name><role>Reviewing Editor</role><aff><institution-wrap><institution-id institution-id-type="ror">https://ror.org/01r9z8p25</institution-id><institution>University of La Laguna</institution></institution-wrap><country>Spain</country></aff></contrib></contrib-group></front-stub><body><boxed-text id="sa2-box1"><p>In the interests of transparency, eLife publishes the most substantive revision requests and the accompanying author responses.</p></boxed-text><p><bold>Decision letter after peer review:</bold></p><p>Thank you for submitting your article &quot;Mechanotransduction events at the physiological site of touch detection&quot; for consideration by <italic>eLife</italic>. Your article has been reviewed by three peer reviewers, one of whom is a member of our Board of Reviewing Editors, and the evaluation has been overseen by a Senior Editor. The reviewers have opted to remain anonymous.</p><p>The individual reviews are provided below. Please note that the reviewers have pointed out some suggestions that may help to improve the manuscript. You may consider incorporating these suggestions to the final version for publication. Please take note of the points below and we hope you will continue to support eLife by reviewing for us and by submitting other papers going forward.</p><p><italic>Reviewer #1 (Recommendations for the authors):</italic></p><p>The manuscript by Ziolkowski et al. shows unprecedented in vivo recordings from skin mechanoreceptors. These recordings produce rapid excitatory currents (with fast activation and inactivation kinetics) when applying the mechanical stimulus (ON) and after removing it (OFF). This mechanically activated ionic current (MA) propagates through action potentials out of the terminals from a certain threshold. These action potentials are also sensitive to TTX, demonstrating a role of voltage-gated sodium channels in the process. In this study the authors overcome a long-existing technical challenge and present an experimental model to study skin mechanoreceptors. The contents seem adequate for a short report, and future work should warrant more detailed characterization of the ion channels involved in these MA currents (Piezo2 seems to be the clearest candidate due to all the literature on the subject).</p><p>This short report is very well written and structured. Suggestions that may help to improve the manuscript are:</p><p>– The activation and inactivation kinetics (Figure 1F-G) of the MA current, both ON and OFF, is fast and very similar, although for inactivation, the MA OFF current seems to be twice as fast as the ON current ( figure 1F). However, this difference is not clearly inferred from the recordings of panel 1B. The authors could consider including an inset directly comparing zoomed/scaled MA-ON and OFF currents, so this significant difference in the inactivation kinetics is made more evident.</p><p>– Figure 2E shows an example of the APs of the lamellar cell, blue line. Perhaps it would be interesting to accompany them with the AP that is generated in the afferent terminal (black line), which would be similar to what is shown in 1D. This would provide a comparison at-a-glance of some of the distinct properties of lamellar cell vs afferent terminals which are then summarized in 2G-I.</p><p><italic>Reviewer #2 (Recommendations for the authors):</italic></p><p>Overall, the experiments conducted by the authors were well designed and all claims and conclusions made were well supported by the data. Additionally, the experiments and data collected are required for a comprehensive understanding of touch detection which, up until now, has not been done. This is already a very strong manuscript with no major issues that need to be addressed. I only have one minor point to take into consideration.</p><p>The manuscript would improve if the significance of the study was better explained; i.e. why are these results so fundamental for our understanding of the sense of touch?</p><p><italic>Reviewer #3 (Recommendations for the authors):</italic></p><p>This short communication builds up on the idea that most electrophysiological recordings to study mechanoreceptors and the mechanically activated current responses are performed on the dissociated neurons soma and far away from the site of action. Here the authors performed elegant recordings from afferent terminal (within the Grandry corpuscles) as well as afferent fiber (single-fiber recordings), not done before to the best of our knowledge. This strategy is useful and establishes the fundamental characteristics of mechanotransduction at the physiological site of touch/mechanical detection in the mechanosensory neurons.</p><p>A few significant differences are found in the properties of mechanically activated responses recorded from lamellar cells and afferent terminal, suggesting distinct mechanism of action. Though the mechanisms are not explored in this study, this strategy provides the baseline for future electrophysiological studies for various mechanoreceptors.</p><p>Another interesting aspect of this study is the presence of electrical responses during the off phase (retrieval of mechanical stimuli). Usually in dissociated neurons and in other in vitro studies, mechanical stimuli evoke currents during the start of the stimulus. Here the authors were able to look into the unique aspect of the current responses during the ON phase and the OFF phase. The results are summarized elegantly and the data supports the claim, with substantial discussion points.</p><p>The work is complete in its current format, the data supports the claim. It's a nice sweet short paper, to the point. The authors didn't leave much room for suggestions but here are my two cents.</p><p>1) A little more analysis or a line or two on the kinetics of &quot;off and on phase&quot;. This is an important finding and can be highlighted a bit more. By the look of the traces seems like the decay of current is fitted with a single exponential. Did you try fitting with two or more?</p><p>2) Action potential is recorded first time from these cell types. This point can be highlighted a bit more in the text.</p><p>3) Possibility of Piezo2 as the major MA channel or an unknown mechano channel can also be discussed.</p></body></sub-article><sub-article article-type="reply" id="sa2"><front-stub><article-id pub-id-type="doi">10.7554/eLife.84179.sa2</article-id><title-group><article-title>Author response</article-title></title-group></front-stub><body><disp-quote content-type="editor-comment"><p>Reviewer #1 (Recommendations for the authors):</p><p>This short report is very well written and structured. Suggestions that may help to improve the manuscript are:</p><p>– The activation and inactivation kinetics (Figure 1F-G) of the MA current, both ON and OFF, is fast and very similar, although for inactivation, the MA OFF current seems to be twice as fast as the ON current ( figure 1F). However, this difference is not clearly inferred from the recordings of panel 1B. The authors could consider including an inset directly comparing zoomed/scaled MA-ON and OFF currents, so this significant difference in the inactivation kinetics is made more evident.</p></disp-quote><p>We changed Figure 1B to a more representative trace where the slower inactivation in the ON phase compared to the OFF phase is more visually clear.</p><disp-quote content-type="editor-comment"><p>– Figure 2E shows an example of the APs of the lamellar cell, blue line. Perhaps it would be interesting to accompany them with the AP that is generated in the afferent terminal (black line), which would be similar to what is shown in 1D. This would provide a comparison at-a-glance of some of the distinct properties of lamellar cell vs afferent terminals which are then summarized in 2G-I.</p></disp-quote><p>In Figure 2E, we added an inset of afferent terminal AP response below lamellar cell AP response with added scale bar.</p><disp-quote content-type="editor-comment"><p>Reviewer #2 (Recommendations for the authors):</p><p>The manuscript would improve if the significance of the study was better explained; i.e. why are these results so fundamental for our understanding of the sense of touch?</p></disp-quote><p>In abstract, we added &quot;Until now, direct evidence of MA current and mechanically-induced action potentials in the mechanoreceptor terminal has not been obtained.&quot;</p><disp-quote content-type="editor-comment"><p>Reviewer #3 (Recommendations for the authors):</p><p>The work is complete in its current format, the data supports the claim. It's a nice sweet short paper, to the point. The authors didn't leave much room for suggestions but here are my two cents.</p><p>1) A little more analysis or a line or two on the kinetics of &quot;off and on phase&quot;. This is an important finding and can be highlighted a bit more. By the look of the traces seems like the decay of current is fitted with a single exponential. Did you try fitting with two or more?</p></disp-quote><p>We used single-fit only because it was sufficient to capture the decay kinetics in our experiments.</p><disp-quote content-type="editor-comment"><p>2) Action potential is recorded first time from these cell types. This point can be highlighted a bit more in the text.</p></disp-quote><p>In abstract, we added &quot;Until now, direct evidence of MA current and mechanically-induced action potentials in the mechanoreceptor terminal has not been obtained.&quot;</p><disp-quote content-type="editor-comment"><p>3) Possibility of Piezo2 as the major MA channel or an unknown mechano channel can also be discussed.</p></disp-quote><p>We added the following: “Though duck Piezo2 also displays fast-inactivating MA current (Schneider et al., 2017), whether the ON phase MA current in the terminal is mediated by Piezo2 or another, unknown ion channel remains to be determined.&quot;</p></body></sub-article></article>