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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Energy Res.</journal-id>
<journal-title>Frontiers in Energy Research</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Energy Res.</abbrev-journal-title>
<issn pub-type="epub">2296-598X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">882508</article-id>
<article-id pub-id-type="doi">10.3389/fenrg.2022.882508</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Energy Research</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Moisture Stability of Sulfide Solid-State Electrolytes</article-title>
<alt-title alt-title-type="left-running-head">Yersak et al.</alt-title>
<alt-title alt-title-type="right-running-head">Sulfide Solid-State Electrolyte Moisture Stability</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Yersak</surname>
<given-names>Thomas A.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1572065/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhang</surname>
<given-names>Yubin</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hao</surname>
<given-names>Fang</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/863753/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Cai</surname>
<given-names>Mei</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/123330/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Battery Cell Systems Research Laboratory</institution>, <institution>General Motors Global R&#x26;D</institution>, <addr-line>Warren</addr-line>, <addr-line>MI</addr-line>, <country>United States</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Optimal, Inc.</institution>, <addr-line>Plymouth</addr-line>, <addr-line>MI</addr-line>, <country>United States</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/763887/overview">Hui Wang</ext-link>, University of Louisville, United States</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/754610/overview">Yang Zhao</ext-link>, Western University, Canada</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/975896/overview">Jun Zhang</ext-link>, Zhejiang University of Technology, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Thomas A. Yersak, <email>thomas.yersak@gm.com</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Electrochemical Energy Conversion and Storage, a section of the journal Frontiers in Energy Research</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>09</day>
<month>05</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>882508</elocation-id>
<history>
<date date-type="received">
<day>23</day>
<month>02</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>06</day>
<month>04</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Yersak, Zhang, Hao and Cai.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Yersak, Zhang, Hao and Cai</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>In this report we detail a comprehensive study on the moisture stability of sulfide solid-state electrolytes in dry room environments. Although sulfide SSEs have many favorable attributes, this class of materials suffers from poor stability with water. Sulfide SSEs react with water to form gaseous H<sub>2</sub>S and a variety of solid byproducts like Li<sub>3</sub>PO<sub>4</sub> and LiOH, which go on to increase the interfacial impedance of solid-state batteries. Lab-scale research typically utilizes gloveboxes with &#x3c;1&#xa0;ppm water, however, the large-scale manufacturing of Li-ion batteries occurs in &#x2212;40&#xb0;C dewpoint dry rooms with around 126&#xa0;ppm water. Consequently, the moisture stability of sulfide SSEs must be addressed if the manufacture of solid-state batteries based on sulfide SSEs is to be scaled up. Here, we are the first to characterize the moisture stability of sulfide SSEs according to both H<sub>2</sub>S and the degradation of ionic conductivity at different moisture setpoints ranging from &#x2212;76&#xb0;C to &#x2212;40&#xb0;C dewpoint. A variety of different SSE compositions are studied; namely, (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub>, (Li<sub>2</sub>S)<sub>70</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>, (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>68</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub>, (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>63</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>, and (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI. We find that moisture stability improves with 75&#xa0;mol% Li<sub>2</sub>S modifier content and the introduction of a Li<sub>2</sub>O co-modifier. After a 30&#xa0;min exposure in a &#x2212;40&#xb0;C dewpoint dry room environment we found that (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI powder generated 0.1 cc/g H<sub>2</sub>S and its ionic conductivity decreased by over 50%. However, when SSE powder was exposed as a slurry in a dodecane carrier the same SSE composition generated 0 cc/g H<sub>2</sub>S and its ionic conductivity only dropped by 14%. Our results show that sulfide SSEs have acceptable moisture stability when appropriately processed in a dry room environment.</p>
</abstract>
<kwd-group>
<kwd>sulfide</kwd>
<kwd>solid-state</kwd>
<kwd>moisture stability</kwd>
<kwd>ionic conductivity</kwd>
<kwd>dry room</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Sulfide solid-state electrolytes (SSEs) have garnered much interest in academia and industry due to their high ionic conductivity up to 10<sup>&#x2212;2</sup>&#xa0;S/cm and good processability (<xref ref-type="bibr" rid="B20">Zhang et al., 2020</xref>; <xref ref-type="bibr" rid="B22">Zheng et al., 2021a</xref>; <xref ref-type="bibr" rid="B2">Chen et al., 2021</xref>; <xref ref-type="bibr" rid="B16">Pang et al., 2022</xref>). Unfortunately, the poor moisture stability of sulfide SSEs presents a major obstacle to the commercialization of solid-state batteries utilizing these SSEs (<xref ref-type="bibr" rid="B7">Hao et al., 2018</xref>; <xref ref-type="bibr" rid="B3">Chen et al., 2019</xref>; <xref ref-type="bibr" rid="B18">Randau et al., 2020</xref>). In academic studies, sulfide SSEs are typically handled in inert gloveboxes with a moisture content of &#x3c;1&#xa0;ppm H<sub>2</sub>O (&#x2212;80&#xb0;C dew point) since they are readily hydrolyzed by moisture in air to release H<sub>2</sub>S. For context, conventional Li-ion batteries are typically assembled in dry rooms with &#x2212;40&#xb0;C dew point (127&#xa0;ppm H<sub>2</sub>O). If sulfide SSE-based solid-state batteries are to be manufactured using the same capital equipment and facilities as those used to make conventional Li-ion batteries, then the moisture stability of sulfide SSEs must be improved. Accordingly, previous studies have evaluated the moisture stability of xLi<sub>2</sub>S&#xb7;(100-x)P<sub>2</sub>S<sub>5</sub> sulfide SSEs with different compositions (<xref ref-type="bibr" rid="B11">Muramatsu et al., 2011</xref>), with additives (<xref ref-type="bibr" rid="B13">Ohtomo et al., 2013a</xref>; <xref ref-type="bibr" rid="B9">Hayashi et al., 2013</xref>; <xref ref-type="bibr" rid="B8">Hayashi et al., 2014</xref>), with a Li<sub>2</sub>O co-modifier (<xref ref-type="bibr" rid="B14">Ohtomo et al., 2013b</xref>; <xref ref-type="bibr" rid="B12">Ohtomo et al., 2013c</xref>; <xref ref-type="bibr" rid="B15">Ohtomo et al., 2013d</xref>), with a LiI dopant (<xref ref-type="bibr" rid="B1">Calpa et al., 2021</xref>), or with a hydrophilic binder (<xref ref-type="bibr" rid="B19">Tan et al., 2019</xref>).</p>
<p>The aforementioned studies used H<sub>2</sub>S generation as a proxy for moisture stability. H<sub>2</sub>S generation is an important metric from a safety perspective (<xref ref-type="bibr" rid="B6">Evans, 1967</xref>), however, no data has been published on how well sulfide SSEs retain their ionic conductivity after exposure to air. Furthermore, previous work evaluated the moisture stability of sulfide SSEs under ambient conditions and often moisture level was not reported. If ambient condition is considered to be air at a temperature of 25&#xb0;C and 30% relative humidity, then this equates to an extremely high water content of 0.95% by volume (9,500&#xa0;ppm). It is much better to characterize the moisture stability of sulfide SSEs under conditions that match those of a cell manufacturing plant. In this study, we therefore report the moisture stability of sulfide SSEs in a dry room environment and quantify moisture stability as both H<sub>2</sub>S generation and how well a sulfide SSE retains its ionic conductivity after exposure.</p>
<p>We will first present the stability of several glass sulfide SSE compositions when exposed in a &#x2212;40&#xb0;C dew point dry room to obtain a comprehensive understanding for how sulfide glass composition influences hygroscopicity. Sulfide SSEs compositions were chosen to probe the influence of glass modifier (Li<sub>2</sub>S) content, glass co-modifier (Li<sub>2</sub>O), and LiI dopant. A description of these glass SSE constituents can be found elsewhere (<xref ref-type="bibr" rid="B10">Martin, 2016</xref>). The five different SSE compositions studied were (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub>, (Li<sub>2</sub>S)<sub>70</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>, (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>68</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub>, (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>63</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>, and (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI. Consistent with previous studies, we generally found that glasses with 75&#xa0;mol% of modifier content yielded the best moisture stability (<xref ref-type="bibr" rid="B11">Muramatsu et al., 2011</xref>). Raman spectroscopic analysis of samples before and after exposure determined that the comparatively stable PS<sub>4</sub>
<sup>3-</sup> structural unit accounts for the moisture stability of these samples. Our results also show that the (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>68</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> SSE produced nearly zero H<sub>2</sub>S after a 30&#xa0;min exposure to a &#x2212;40&#xb0;C dew point dry room, but its ionic conductivity still dropped by over 50%. We conclude that any quantification of moisture stability must therefore consider the ionic conductivity of the sulfide SSE after exposure. Our study then evaluated the moisture stability of the (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI SSE as a function of dry room moisture level from &#x2212;40 to &#x2212;76&#xb0;C dew point. Degradation of sulfide SSE ionic conductivity was found to be nonlinear with respect to H<sub>2</sub>O concentration. As a final test, the moisture stability of sulfide SSE slurries was evaluated to mimic the handling of SSE material during an electrode or separator tape casting process (<xref ref-type="bibr" rid="B21">Zheng et al., 2021b</xref>). The (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI SSE was suspended in either anhydrous dodecane or anisole and exposed to a dry room environment with &#x2212;40&#xb0;C dew point. The dodecane slurry generated zero H<sub>2</sub>S and the sulfide SSE retained 95.3% of its pristine ionic conductivity. The results of this study suggest that even though sulfide SSEs are hygroscopic, there are ways to handle sulfide SSEs in a typical cell manufacturing environment without damaging the sulfide SSEs&#x2019; function.</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<title>Materials and Methods</title>
<p>During preparation all materials were handled under an argon atmosphere with less than 1&#xa0;ppm water and oxygen. Solid-state electrolyte (SSE) precursor materials included Li<sub>2</sub>S (99.5% Sigma Aldrich), Li<sub>2</sub>O (99.5%, Alfa Aesar), P<sub>2</sub>S<sub>5</sub> (98% Sigma Aldrich), and LiI (99.9%, Aldrich). Five different SSE compositions were prepared: (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> (75-25 LPS), (Li<sub>2</sub>S)<sub>70</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub> (70-30 LPS), (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>68</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> (7-68-25 LPSO), (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>63</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub> (7-63-30 LPSO), and (Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI (LPSI). SSEs were prepared by planetary ball milling (Frisch Pulverisette 7). In this process, 4g SSE precursors of the appropriate stoichiometry were first combined in a 40&#xa0;ml zirconia milling jar along with 10&#xa0;ml of dried hexane (4&#xc5; molecular sieve) and 80&#xa0;g of milling media. Next, each sample was milled for total of 20&#xa0;h at 500&#xa0;rpm. Finally, the hexane was removed by gently heating opened milling jars at 60&#xb0;C for 12&#xa0;h. SSE powders were pale yellow to off-white in color as shown in <xref ref-type="fig" rid="F1">Figure 1A</xref>.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>
<bold>(A)</bold> A picture of the pristine sulfide SSE powders. <bold>(B)</bold> Powder XRD patterns of the pristine glassy SSEs. <bold>(C)</bold> A picture of the sulfide SSE powders after exposed in dry room. <bold>(D)</bold> Powder XRD patterns of the glassy SSEs. after exposed in dry room.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g001.tif"/>
</fig>
<p>The long-range structure of glasses was studied using powder x-ray diffraction (pXRD) (Bruker D8 Advance). pXRD data are provided in <xref ref-type="fig" rid="F1">Figure 1B</xref>, and the absence of strong reflections indicate that all samples are amorphous. A weak reflection at approximately 27&#xb0; 2&#x3b8; indicates some samples do have trace amounts of Li<sub>2</sub>S (<xref ref-type="bibr" rid="B17">Jain et al., 2013</xref>). The implications of trace Li<sub>2</sub>S on moisture stability will be discussed in the next section. The short-range structure of glasses before and after exposure to a dry room environment was studied using Raman spectroscopy (Renishaw InVia) with a 532&#xa0;nm excitation line and a &#xd7;20 objective lens.</p>
<p>An actual dry room was not used in this study. Rather, a dry room environment was simulated inside a 300&#xa0;L tabletop acrylic glovebox (MBraun, MB-GB-2202) using synthetic air (Airgas, AI UZ300, 76.5&#x2013;80.5% nitrogen, 19.5&#x2013;23.5% oxygen) as shown in <xref ref-type="fig" rid="F2">Figure 2</xref>. The glovebox was outfitted with a custom moisture control system to maintain humidity levels to within &#xb1;2&#xb0;C of a desired target dew point. Unless otherwise noted, the humidity level was set to &#x2212;40&#xb0;C dew point (127&#xa0;ppm H<sub>2</sub>O) for each experiment. The control system consisted of a cartridge-based desiccator (VAC, Genesis), a moisture probe (VAC, LM-H<sub>2</sub>O-A), and an Arduino microcontroller. The microcontroller was programmed to monitor the moisture probe voltage output and send a digital signal to a solid-state relay that turned the desiccator fan on and off as needed. The desiccant system was disabled during SSE exposure experiments since it also scrubbed H<sub>2</sub>S from the atmosphere. During each experiment, 0.6&#xa0;g of sulfide SSE powder was spread out onto a flat surface and exposed to air for 30&#xa0;min. The exposure of powder more closely mimics an actual manufacturing process than the exposure of compacted pellets. A fan was run to constantly mix the atmosphere within the glovebox to ensure a uniform mix of H<sub>2</sub>O and H<sub>2</sub>S. H<sub>2</sub>S concentration was measured using a personal safety sensor (ToxiRAE) oriented 4 inches above the sample powder as shown in <xref ref-type="fig" rid="F2">Figure 2</xref>. After exposure, the SSE powder was packaged in a glass vial and transferred back into an argon atmosphere with less 1&#xa0;ppm water and oxygen. The box was cleaned and purged between each experiment to ensure a 0.0&#xa0;ppm H<sub>2</sub>S starting baseline. Scanning electron microscopy (SEM) (Hitachi S-4800) was used to observe the morphology before and after exposure. Energy-dispersive X-ray spectroscopy (EDS) (Ametek EDAX) equipped on the SEM was used to characterize the SSE elemental compositions before and after exposure.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>A picture of the experimental setup used to expose sulfide SSE powders to a dry room environment. The setup includes a 300L volume tabletop glovebox, a cartridge-based desiccant system, a microcontroller system to control the moisture setpoint, a personal H<sub>2</sub>S detector, and a fan to continuously mix the glovebox air.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g002.tif"/>
</fig>
<p>The ionic conductivity of sulfide SSEs was measured by assembling Li/SSE/Li symmetric cells with SSE powder collected before and after exposure to air. To assemble each cell, 150&#x2013;200&#xa0;mg of sulfide SSE powder was compacted using a 13&#xa0;mm diameter polyetheretherketone (PEEK) die and stainless steel plungers with a pressure of 370&#xa0;MPa. Li metal foil (MTI, 0.5&#xa0;mm thick) was then attached to both sides of the compacted SSE powder disc. AC impedance of these cells was then measured immediately after assembly using a frequency range 1&#xa0;MHz to 0.1&#xa0;Hz and an excitation current of 10&#xa0;&#x3bc;A (Biologic VMP-3). Total real impedances (R<sub>T</sub>) were interpolated from the minima of the Nyquist plot spectra. The thickness (<italic>t</italic>) and area (<italic>a</italic>) of each glass sample was measured using digital calipers and ionic conductivity was then calculated using <xref ref-type="disp-formula" rid="e1">Eq. 1</xref> from values of R<sub>T</sub>, <italic>t</italic> and <italic>a</italic>.<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:mi>&#x3c3;</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mi>t</mml:mi>
<mml:mrow>
<mml:mi>a</mml:mi>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mi>T</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
</p>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>Results and Discussion</title>
<p>In the first experiment of this study, a variety of sulfide SSE powders were exposed to a &#x2212;40&#xb0;C dew point dry room environment for 30&#xa0;min. During this experiment H<sub>2</sub>S gas generation was monitored and the data are provided in <xref ref-type="fig" rid="F3">Figure 3A</xref>. Our results are consistent with the findings of previous studies with respect to the influence of glass modifier (Li<sub>2</sub>S) content, glass co-modifier (Li<sub>2</sub>O), and LiI dopant on H<sub>2</sub>S generation. First, sulfide SSEs with 75&#xa0;mol% glass modifier produced the least amount of H<sub>2</sub>S (<xref ref-type="bibr" rid="B11">Muramatsu et al., 2014</xref>). 75-25 LPS, 7-68-25 LPSO, and 75-25 LPSI all generated a maximum of 0.1&#xa0;g/cc H<sub>2</sub>S, whereas 70-30 LPS and 7-63-30 LPSO generated a maximum of 0.6&#x2013;0.7&#xa0;g/cc H<sub>2</sub>S. Second, a Li<sub>2</sub>O co-modifier modestly reduced the H<sub>2</sub>S generation of sulfide SSEs (<xref ref-type="bibr" rid="B14">Ohtomo et al., 2013b</xref>; <xref ref-type="bibr" rid="B12">Ohtomo et al., 2013c</xref>; <xref ref-type="bibr" rid="B15">Ohtomo et al., 2013d</xref>). Even though our H<sub>2</sub>S device had a resolution of only 0.1&#xa0;ppm, which is equivalent to 0.1 cc/g, we could still track the time it took before each sample registered a non-zero value. 75-25 LPS registered its first non-zero value at 22&#xa0;min whereas 7-68-25 LPSO only registered one non-zero value at 29&#xa0;min. No appreciable difference was observed between 70 and 30 LPS and 7-63-30 LPSO. Finally, a LiI dopant did not increase H<sub>2</sub>S generation since both 75-25 and 75-25 LPSI generated a maximum of 0.1&#xa0;g/cc H<sub>2</sub>S (<xref ref-type="bibr" rid="B12">Ohtomo et al., 2013c</xref>). <xref ref-type="bibr" rid="B1">Calpa et al. (2021)</xref> previously reported that a LiI dopant reduces the H<sub>2</sub>S generation of sulfide SSEs exposed to ambient air at 40% relative humidity. Our study differed from Calpa et al. in that our moisture level was much lower and we exposed SSE powder instead of pellets.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>
<bold>(A)</bold> H<sub>2</sub>S generation of different SSEs in a &#x2212;40&#xb0;C dew point dry room as a function of time. <bold>(B)</bold> Reduction in ionic conductivity versus maximum H<sub>2</sub>S reading for different sulfide SSEs.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g003.tif"/>
</fig>
<p>In addition to monitoring H<sub>2</sub>S gas generation, this study is the first to report on the ionic conductivity of sulfide SSEs before and after exposure to a &#x2212;40&#xb0;C dew point dry room environment and the data are provided in <xref ref-type="fig" rid="F3">Figure 3B</xref> and <xref ref-type="table" rid="T1">Table 1</xref>. Every sample experienced a significant drop in ionic conductivity with 70-30 LPS having the largest drop of 76.5% and 7-68-25 LPSO having the smallest drop of 51.6%. The products of sulfide SSE hydrolysis may include compounds such as LiOH (<xref ref-type="bibr" rid="B11">Muramatsu et al., 2014</xref>), Li<sub>3</sub>PO<sub>4</sub> (<xref ref-type="bibr" rid="B13">Ohtomo et al., 2013a</xref>), and LiI&#xb7;H<sub>2</sub>O (<xref ref-type="bibr" rid="B1">Calpa et al., 2021</xref>). These compounds are poor ionic conductors, and if formed on the surface of sulfide SSE particles will act to substantially increase interparticle impedance once the powders are consolidated into pellets or films. We conclude that H<sub>2</sub>S generation is not a sufficient metric for the moisture stability of sulfide SSEs and that moisture stability should also comprehend functional characteristics like ionic conductivity.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Ionic conductivity and H2S generation data for sulfide SSE powders exposed to a &#x2212;40&#xb0;C dew point dry room environment for 30&#xa0;min.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Composition</th>
<th align="center">Pristine &#x3c3; (mS/cm)</th>
<th align="center">Exposed &#x3c3; (mS/cm)</th>
<th align="center">&#x394;&#x3c3;</th>
<th align="center">H<sub>2</sub>S generation (cc/g)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">(Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub>
</td>
<td align="center">0.43</td>
<td align="center">0.17</td>
<td align="center">&#x2212;60.5%</td>
<td align="center">0.2</td>
</tr>
<tr>
<td align="left">(Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>68</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub>
</td>
<td align="center">0.31</td>
<td align="center">0.15</td>
<td align="center">&#x2212;51.6%</td>
<td align="center">0.1</td>
</tr>
<tr>
<td align="left">(Li<sub>2</sub>S)<sub>70</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>
</td>
<td align="center">0.26</td>
<td align="center">0.061</td>
<td align="center">&#x2212;76.5%</td>
<td align="center">0.6</td>
</tr>
<tr>
<td align="left">(Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>63</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>
</td>
<td align="center">0.18</td>
<td align="center">0.062</td>
<td align="center">&#x2212;65.6%</td>
<td align="center">0.7</td>
</tr>
<tr>
<td align="left">(Li<sub>2</sub>S)<sub>75</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>25</sub> &#x2b; 20&#xa0;mol% LiI</td>
<td align="center">1.21</td>
<td align="center">0.39</td>
<td align="center">&#x2212;67.8%</td>
<td align="center">0.1</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>In the next phase of this work the SSEs were characterized with pXRD, SEM, Raman spectroscopy, and EDS to understand the effect of hydrolysis on SSE particle morphology and SSE structure. After exposure the SSE powders appeared unchanged (<xref ref-type="fig" rid="F1">Figure 1C</xref>) and no new reflections were detected by pXRD (<xref ref-type="fig" rid="F1">Figure 1D</xref>). The pXRD data suggest that the products of SSE hydrolysis in a dry room environment were either amorphous or in a small quantity below the detection limit of our equipment. SEM images of 75-25 LPS and 7-68-25 LPSO before and after exposure are provided in <xref ref-type="fig" rid="F4">Figure 4</xref>. SSE particles range in size from approximately 1&#xa0;&#xb5;m to greater than 10&#xa0;&#xb5;m in diameter and no discernable difference was observed after exposure. Finally, the elemental compositions of the 75-25 LPS and 7-68-25 LPSO were characterized using EDS. <xref ref-type="fig" rid="F5">Figure 5</xref> provides the EDS oxygen K&#x3b1; principle line (0.52&#xa0;keV) for SSEs before and after exposure. All EDS spectra were normalized to the phosphorus K&#x3b1; principle line (2.01&#xa0;keV) and the full dataset is provided in <xref ref-type="sec" rid="s10">Supplementary Figure S1</xref>. The pristine samples both exhibit an oxygen signal (red). An oxygen signal is expected for 7-68-25 LPSO since it contains a Li<sub>2</sub>O co-modifier. The oxygen signal for 75-25 LPS can be explained by precursor impurities and a brief exposure to ambient air during sample transfer to the SEM. After dry room exposure (&#x2212;40&#xb0;C dewpoint) for 30&#xa0;min the oxygen signal for 75-25 LPS increased slightly while that of the 7-68-25 LPSO remained unchanged (green). To effect a measurable change on both samples we also exposed SSEs to ambient air (20&#xb0;C, 20% relative humidity) for 5&#xa0;min. In this case, both samples exhibit a substantially increased oxygen signal (blue). As we will discuss later on, an increase in the oxygen signal suggests that the hydrolysis of SSEs leads to the formation of oxygen containing compounds.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>SEM images of 75-25 LPS and 7-68-25 LPSO sulfide SSEs before and after exposure.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g004.tif"/>
</fig>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>EDS oxygen K&#x3b1; principle line (0.52&#xa0;keV) for 75-25 LPS <bold>(A)</bold> and 7-68-25 LPSO <bold>(B)</bold> before (red) and after exposure to either a dry room environment (green) or ambient air (blue).</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g005.tif"/>
</fig>
<p>The local structure of sulfide SSEs before and after exposure was determined by Raman spectroscopy and the data are provided in <xref ref-type="fig" rid="F6">Figure 6</xref>, <xref ref-type="fig" rid="F7">Figure 7</xref>, and <xref ref-type="table" rid="T2">Table 2</xref>. <xref ref-type="fig" rid="F6">Figure 6</xref> presents the Raman spectra for sulfide SSEs with 75&#xa0;mol% modifier content; namely, 75-25 LPS, 7-68-25 LPSO, and 75-25 LPSI. The spectra for these sulfide SSEs are dominated by a single feature centered at 421&#xa0;cm<sup>&#x2212;1</sup> attributable to the PS<sub>4</sub>
<sup>3-</sup> structural unit. After exposure, this feature does not shift or change shape suggesting that the local structure of sulfide SSEs with 75&#xa0;mol% modifier content remains the same. <xref ref-type="fig" rid="F7">Figure 7</xref> presents the Raman spectra for sulfide SSEs with 70&#xa0;mol% modifier content; namely, 70-30 LPS and 7-63-30 LPSO. Similarly, the spectra are dominated by a single feature, however, this feature may be deconvoluted into multiple peaks attributable to PS<sub>4</sub>
<sup>3-</sup> (421&#xa0;cm<sup>&#x2212;1</sup>), P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup> (406&#xa0;cm<sup>&#x2212;1</sup>), and P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup> (387&#xa0;cm<sup>&#x2212;1</sup>) structural units (<xref ref-type="fig" rid="F7">Figures 7B,E</xref>; <xref ref-type="table" rid="T2">Table 2</xref>).The local structure of sulfide SSEs with 70&#xa0;mol% modifier content is more complicated since the glass former is not fully de-networked. This results in the formation of larger structural units like P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup> and P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup>, which are more susceptible to hydrolysis due to labile bridging sulfur and P-P bonds, respectively (<xref ref-type="bibr" rid="B19">Tan et al., 2019</xref>). In fact, after exposure the relative abundance of P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup> and P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup> structural units decreased compared to that of PS<sub>4</sub>
<sup>3-</sup> (<xref ref-type="fig" rid="F7">Figures 7C,F</xref>; <xref ref-type="table" rid="T2">Table 2</xref>). For example, the peak area attributable to PS<sub>4</sub>
<sup>3-</sup> went from 25.3% before exposure to 33.1% after exposure for 7-63-30 LPSO (<xref ref-type="table" rid="T2">Table 2</xref>). From these data we conclude that the PS<sub>4</sub>
<sup>3-</sup> structural unit is comparatively more stable than P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup> or P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup>. Sulfide SSEs with 75&#xa0;mol% modifier content therefore produce less H<sub>2</sub>S because they are primarily composed of PS<sub>4</sub>
<sup>3-</sup> structural units, which react with moisture at a slower rate than the larger structural units found in sulfide SSEs with 70&#xa0;mol% modifier content.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Raman spectroscopy spectra for 75-25 LPS, 7-68-25 LSPO, and LPSI sulfide SSEs before and after exposure to a &#x2212;40&#xb0;C dew point dry room for 30&#xa0;min.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g006.tif"/>
</fig>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Raman spectra of sulfide SSEs before and after exposure to a &#x2212;40&#xb0;C dew point dry room environment for 30&#xa0;min. The primary peak was deconvoluted into three peaks attributed to PS<sub>4</sub>
<sup>3-</sup> (green, 420&#xa0;cm&#x2212;1), P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup> (red, 406&#xa0;cm&#x2212;1), and P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup> (blue, 387&#xa0;cm&#x2212;1) structural units. <bold>(A)</bold> Raman spectra for 70-30 LPS before and after exposure. <bold>(B)</bold> Fitted Raman spectrum for 70-30 LPS before exposure. Insets provide ball and stick models for PS<sub>4</sub>
<sup>3-</sup>, P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup>, and P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup> structural units. <bold>(C)</bold> Fitted Raman spectrum for 70-30 LPS after exposure. <bold>(D)</bold> Raman spectra for 7-63-30 LPSO before and after exposure. <bold>(E)</bold> Fitted Raman spectrum for 7-68-30 LPSO before exposure. <bold>(F)</bold> Fitted Raman spectrum for 7-68-30 LPSO after exposure.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g007.tif"/>
</fig>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Summary of Raman spectra peak fitting and deconvolution.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Sample</th>
<th align="center">PS<sub>4</sub>
<sup>3-</sup> (%)(421 cm<sup>-1</sup>)</th>
<th align="center">P<sub>2</sub>S<sub>7</sub>
<sup>4-</sup> (%) (406 cm<sup>-1</sup>)</th>
<th align="center">P<sub>2</sub>S<sub>6</sub>
<sup>4-</sup> (%) (387 cm<sup>-1</sup>)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Pristine (Li<sub>2</sub>S)<sub>70</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>
</td>
<td align="center">27.0</td>
<td align="center">60.2</td>
<td align="center">12.8</td>
</tr>
<tr>
<td align="left">Exposed (Li<sub>2</sub>S)<sub>70</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>
</td>
<td align="center">28.2</td>
<td align="center">57.8</td>
<td align="center">14.0</td>
</tr>
<tr>
<td align="left">Pristine (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>63</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>
</td>
<td align="center">25.3</td>
<td align="center">59.7</td>
<td align="center">15.0</td>
</tr>
<tr>
<td align="left">Exposed (Li<sub>2</sub>O)<sub>7</sub>(Li<sub>2</sub>S)<sub>63</sub>(P<sub>2</sub>S<sub>5</sub>)<sub>30</sub>
</td>
<td align="center">33.1</td>
<td align="center">53.3</td>
<td align="center">13.6</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>We just outlined the mechanism for how modifier content affects moisture stability. Before moving on to the results of the last two experiments, let&#x2019;s first consider the effect that a Li<sub>2</sub>O co-modifier or LiI dopant may have on ionic conductivity. Both Li<sub>2</sub>O and LiI were found to reduce the generation of H<sub>2</sub>S; however, we just showed that ionic conductivity was significantly degraded irrespective of sulfide SSE composition (<xref ref-type="table" rid="T1">Table 1</xref>). It was previously suggested that Li<sub>2</sub>O may displace excess, unreacted Li<sub>2</sub>S and that unreacted Li<sub>2</sub>S is a significant source of H<sub>2</sub>S gas (<xref ref-type="bibr" rid="B14">Ohtomo et al., 2013b</xref>; <xref ref-type="bibr" rid="B11">Muramatsu et al., 2014</xref>). In fact, several of our samples do have a trace amount of Li<sub>2</sub>S as evidenced by a weak reflection at about 27&#xb0; 2&#x3b8; in pXRD data of pristine samples (<xref ref-type="fig" rid="F1">Figure 1B</xref>). Li<sub>2</sub>S reacts with H<sub>2</sub>O to form LiOH and H<sub>2</sub>S gas as shown in <xref ref-type="disp-formula" rid="e2">Eq. 2</xref>. Li<sub>2</sub>O also reacts with H<sub>2</sub>O to form LiOH, but it does not release H<sub>2</sub>S gas as shown in <xref ref-type="disp-formula" rid="e3">Eq. 3</xref>. Similarly, LiI reacts with H<sub>2</sub>O to form LiI&#xb7;H<sub>2</sub>O as shown in <xref ref-type="disp-formula" rid="e4">Eq. 4</xref>. These reaction schemes are supported by the aforementioned EDS data, which show a higher prevalence of oxygen in SSE samples after exposure to air (<xref ref-type="fig" rid="F5">Figure 5</xref>; <xref ref-type="sec" rid="s10">Supplementary Figure S1</xref>). As stated earlier, H<sub>2</sub>S generation is an insufficient measure of moisture stability. Both Li<sub>2</sub>O and LiI do not generate H<sub>2</sub>S, but still react with H<sub>2</sub>O to form the insulating solid products of LiOH and LiI&#xb7;H<sub>2</sub>O. Combining measurements of H<sub>2</sub>S generation with ionic conductivity therefore provides a more complete characterization of moisture stability.<disp-formula id="e2">
<mml:math id="m2">
<mml:mrow>
<mml:mi mathvariant="normal">L</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">i</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">S&#x2b;2</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">O&#x2192;</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">S&#x2191;&#x2b;2LiOH</mml:mi>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
<disp-formula id="e3">
<mml:math id="m3">
<mml:mrow>
<mml:mi mathvariant="normal">L</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">i</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">O&#x2b;</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">O&#x2192;2LiOH</mml:mi>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>
<disp-formula id="e4">
<mml:math id="m4">
<mml:mrow>
<mml:mi mathvariant="normal">L</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">i</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">I&#x2b;</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">O&#x2192;LiI&#xd7;</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">H</mml:mi>
<mml:mi mathvariant="normal">2</mml:mi>
</mml:msub>
<mml:mi mathvariant="normal">O</mml:mi>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>
</p>
<p>In the next experiment, the moisture stability of 75-25 LPSI was measured as a function of dew point and the data are provided in <xref ref-type="fig" rid="F8">Figure 8</xref>. H<sub>2</sub>S generation is not reported since the maximum value at the end of each 30&#xa0;min exposure was below the 0.1&#xa0;ppm detection limit of our sensor. Pristine 75-25 LPSI has an ionic conductivity of 1.21&#xa0;mS/cm at room temperature when only handled inside an inert glovebox with 1&#xa0;ppm H<sub>2</sub>O (-76&#xb0;C dewpoint). Exposing 75-25 LPSI powder to a dry room environment results in degradation of ionic conductivity that trends as the negative log of moisture content (<xref ref-type="fig" rid="F8">Figure 8</xref>). This result implies that over-sizing dry room air handling equipment may not adequately address the poor moisture stability of sulfide SSEs. Designing a dry room to maintain a moisture level of less than &#x2212;60&#xb0;C dew point is prohibitively expensive.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Ionic conductivity of LPSI sulfide SSE after exposure as a dry powder to different dry room environments for 30&#xa0;min. The star marks the ionic conductivity of LPSI sulfide SSE after exposure to a &#x2212;40&#xb0;C dew point dry room for 30&#xa0;min while immersed in anhydrous dodecane.</p>
</caption>
<graphic xlink:href="fenrg-10-882508-g008.tif"/>
</fig>
<p>Solid-state batteries will likely be manufactured using tape casting processes analogous to those used to fabricate conventional Li-ion battery electrodes. Exposure of slurries therefore better simulates the handling of sulfide SSEs in an actual manufacturing process. As a final experiment, slurries of 75-25 LPSI were prepared with either dodecane or anisole and exposed to a &#x2212;40&#xb0;C dew point dry room and the data are provided in <xref ref-type="table" rid="T3">Table 3</xref>. The solvents were also dried with 3&#xc5; molecular sieve prior to use. After exposure to a dry room environment while immersed in dodecane, the ionic conductivity of 75-25 LPSI dropped by only 14% (<xref ref-type="fig" rid="F8">Figure 8</xref> star). On the other hand, the ionic conductivity of 75-25 LPSI dropped by 49.6% when exposed to a dry room environment while immersed in anisole. The degradation in ionic conductivity is attributed to two sources of water; namely, trace moisture in the solvent and moisture in the air. To determine what fraction of the degradation should be attributed to trace moisture in the solvent, 75-25 LPSI was soaked in dodecane or anisole while being kept inside an inert, argon-filled glovebox. This yielded a 1.7 and 16.5% drop in ionic conductivity for 75-25 LPSI soaked in dodecane and anisole, respectively. pXRD patterns of these 75-25 LPSI samples are also provided in <xref ref-type="sec" rid="s10">Supplementary Figure S2</xref>. We conclude that a majority of the ionic conductivity degradation should be attributed to moisture from the air. The difference between samples can be explained by the fact that anisole&#x2019;s miscibility with water (1.6&#xa0;g/L) is much higher than that of dodecane (4.91 &#xd7; 10<sup>&#x2212;6</sup>&#xa0;g/L) (<xref ref-type="bibr" rid="B4">Desmurs and Ratton, 1996</xref>; <xref ref-type="bibr" rid="B5">ECHA, n, d</xref>). Dodecane&#x2019;s immiscibility with water makes it easier to dry with molecular sieve and protects the sulfide SSE from hydrolysis just like a hydrophilic polystyrene-block-polyethylene-ranbutylene-block-polystyrene (SEBS) binder was recently shown to do the same for Li<sub>6</sub>PS<sub>5</sub>Cl (<xref ref-type="bibr" rid="B19">Tan et al., 2019</xref>).</p>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Ionic conductivity and H<sub>2</sub>S generation data for LPSI SSE powders exposed to a &#x2212;40&#xb0;C dew point dry room environment as a slurry for 30&#xa0;min.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Sample</th>
<th align="center">Pristine &#x3c3; (mS/cm)</th>
<th align="center">Exposed &#x3c3; (mS/cm)</th>
<th align="center">&#x394;&#x3c3; w.r.t. dry LPSI (%)</th>
<th align="center">H2S generation (cc/g)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Dry 75-25 LPSI powder</td>
<td align="center">1.21</td>
<td align="center">0.39</td>
<td align="center">67.8</td>
<td align="center">0.1</td>
</tr>
<tr>
<td align="left">75-25 LPSI &#x2b; Dodecane</td>
<td align="center">1.21</td>
<td align="center">1.04</td>
<td align="center">14.0</td>
<td align="center">0.0</td>
</tr>
<tr>
<td align="left">75-25 LPSI &#x2b; Anisole</td>
<td align="center">1.21</td>
<td align="center">0.613</td>
<td align="center">49.6</td>
<td align="center">0.1</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>We conclude that moisture stability is best defined as a combination of H<sub>2</sub>S gas generation and ionic conductivity measurement. Furthermore, sulfide SSEs can be handled in a dry room environment provided that the SSE composition is chosen appropriately and proper engineering controls are put in place. Sulfide SSEs will be handled in a dry room in the presence of solvents and binders and the measurement of moisture stability should seek to mimic this condition. Our results also reinforce the importance of water immiscible solvents for sulfide SSE slurries.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="sec" rid="s10">Supplementary Material</xref>, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s6">
<title>Author Contributions</title>
<p>TY conceived the work, collected data, and wrote the manuscript. YZ and FH collected data, analyzed the results, and contributed to writing the manuscript. MC contributed to writing and reviewing the manuscript.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>This work was funded by the Battery Materials Research Program (BMR) in the United States Department of Energy&#x2019;s (DOE) Office of Energy Efficiency and Renewable Energy&#x2019;s (EERE) Vehicle Technology Office (VTO) (DE-EE0008857).</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of Interest</title>
<p>TY and MC are employed by General Motors Company. FH and YZ are employed by Optimal, Inc. </p>
<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="s9">
<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 would like to thank our colleagues for their support of our project; namely, Drs. Nicholas Pieczonka, Michael Balogh, and James Salvador.</p>
</ack>
<sec id="s10">
<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/fenrg.2022.882508/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fenrg.2022.882508/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet1.docx" id="SM1" mimetype="application/docx" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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