{"id":157,"date":"2022-09-03T23:16:57","date_gmt":"2022-09-04T06:16:57","guid":{"rendered":"https:\/\/faculty.engineering.asu.edu\/chan\/?page_id=157"},"modified":"2022-09-07T18:44:36","modified_gmt":"2022-09-08T01:44:36","slug":"clathrate-electrochemistry","status":"publish","type":"page","link":"https:\/\/faculty.engineering.asu.edu\/chan\/clathrate-electrochemistry\/","title":{"rendered":"Clathrate Electrochemistry"},"content":{"rendered":"\n<div style=\"height:30px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h2 class=\"wp-block-heading\"><span class=\"highlight-gold\">Overview<\/span><\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">The group 14 or Tetrel (<em>Tt<\/em>) elements (Si, Ge, Sn) have received significant attention as high capacity anodes for Li-ion batteries due to their ability to alloy with large amounts of Li. Tetrel clathrates have cage-like structures composed of face-sharing <em>Tt<\/em><sub>20<\/sub>, <em>Tt<\/em><sub>24<\/sub>, and <em>Tt<\/em><sub>28<\/sub> polyhedra that boast strong<em> Tt<\/em>\u2013<em>Tt<\/em> bonds with covalent <em>sp<\/em><sup>3<\/sup>-character. Due to the large number of possible structures and compositions in the clathrate family, these materials have great potential to display a diverse range of electrochemical properties. With support from the National Science Foundation Solid-State Materials Chemistry program within the Division of Materials Research, we have established several important trends concerning the relationships between the clathrate structure and its electrochemical properties.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\" \/>\n\n\n\n<h2 class=\"wp-block-heading\"><span class=\"highlight-gold\">Silicon Clathrates<\/span><\/h2>\n\n\n\n<div style=\"height:30px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-medium is-resized is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/ChemElectroChem-cover-353x500.png\" alt=\"\" class=\"wp-image-334\" width=\"265\" height=\"375\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/ChemElectroChem-cover-353x500.png 353w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/ChemElectroChem-cover-1059x1500.png 1059w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/ChemElectroChem-cover-706x1000.png 706w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/ChemElectroChem-cover-1084x1536.png 1084w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/ChemElectroChem-cover-1446x2048.png 1446w\" sizes=\"auto, (max-width: 265px) 100vw, 265px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Electrochemical Cycling of Sodium-Filled Silicon Clathrate<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Nicholas A. Wagner, Rahul Raghavan, Ran Zhao, Dr. Qun Wei, Xihong Peng, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1002\/celc.201300104\"><em>ChemElectroChem<\/em><\/a> 2014, 1, 347-353<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A mixture of type I and type II silicon clathrate with sodium guest atoms is studied as a potential anode material for lithium-ion batteries. An electrochemical, structural, and first-principles analysis is conducted to understand the phase changes occurring upon lithium insertion and removal from these cage-like silicon structures.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"701\" height=\"565\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/AdvSci-clathrate.png\" alt=\"\" class=\"wp-image-175\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/AdvSci-clathrate.png 701w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/AdvSci-clathrate-500x403.png 500w\" sizes=\"auto, (max-width: 701px) 100vw, 701px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Type I Clathrates as Novel Silicon Anodes: An Electrochemical and Structural Investigation<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Ying Li, Rahul Raghavan, Nicholas A. Wagner, Stephen K. Davidowski, Lo\u00efc Baggetto, Ran Zhao, Qian Cheng, Jeffery L. Yarger, Gabriel M. Veith, Carol Ellis-Terrell, Michael A. Miller, Kwai S. Chan, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1002\/advs.201500057\"><em>Adv. Sci.<\/em><\/a> 2015, 2, 1500057<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Silicon clathrates contain cage-like structures that can encapsulate various guest atoms or molecules. An electrochemical evaluation of type I silicon clathrates based on Ba<sub>8<\/sub>Al<em><sub>y<\/sub><\/em>Si<sub>46\u2212<em>y<\/em><\/sub> as the anode material for lithium-ion batteries is presented here. Postcycling characterization with nuclear magnetic resonance and X-ray diffraction shows no discernible structural or volume changes even after electrochemical insertion of 44 Li (\u22481 Li\/Si) into the clathrate structure. The observed properties are in stark contrast with lithiation of other silicon anodes, which become amorphous and suffer from large volume changes. The electrochemical reactions are proposed to occur as single phase reactions at approximately 0.2 and 0.4 V versus Li\/Li<sup>+<\/sup> during lithiation and delithiation, respectively, distinct from diamond cubic or amorphous silicon anodes. Reversible capacities as high as 499 mAh g\u2212<sup>1<\/sup> at a 5 mA g<sup>\u22121<\/sup> rate were observed for silicon clathrate with composition Ba<sub>8<\/sub>Al<sub>8.54<\/sub>Si<sub>37.46<\/sub>, corresponding to \u22481.18 Li\/Si. These results show that silicon clathrates could be promising durable anodes for lithium-ion batteries.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"1386\" height=\"773\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-1.png\" alt=\"\" class=\"wp-image-328\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-1.png 1386w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-1-500x279.png 500w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-1-1000x558.png 1000w\" sizes=\"auto, (max-width: 1386px) 100vw, 1386px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Synthesis and Characterization of Empty Silicon Clathrates for Anode Applications in Li-ion Batteries<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Kwai S. Chan, Michael A. Miller, Carol Ellis-Terrell, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1557\/adv.2016.434\">MRS Advances<\/a><\/em> 2016, 1, 3043-3048<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Several processing methods were developed and evaluated for synthesizing empty silicon clathrates. A solution synthesis method based on the Hofmann-elimination oxidation reaction was successfully utilized to produce 20 mg of empty Si<sub>46<\/sub>. Half-cells using the Si<sub>46<\/sub> electrodes were successfully cycled for 1000 cycles at rate of 5.3C. The capacity of the Si<sub>46<\/sub> electrode in long-term tests was 675 mAh\/g at the 4th cycle, but increased to 809 mAh\/g at 50 cycles. The corresponding Coulombic efficiency was better than 99%. The capacity dropped from 809 to 553 mAh\/g after 1000 cycles while maintaining a 99% Coulombic efficiency. In comparison, a Ba<sub>8<\/sub>Al<sub>8<\/sub>Si<sub>38 <\/sub>electrode could be cycled for about 200 cycles with a lower capacity and Coulombic efficiency. Potential applications of empty silicon clathrates as anode materials in Li-ion batteries are discussed.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"280\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-surface.png\" alt=\"\" class=\"wp-image-237\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Anodes for Lithium-Ion Batteries Based on Type I Silicon Clathrate Ba<sub>8<\/sub>Al<sub>16<\/sub>Si<sub>30<\/sub> &#8211; Role of Processing on Surface Properties and Electrochemical Behavior<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Ran Zhao,&nbsp;Svilen Bobev,&nbsp;Lakshmi Krishna,&nbsp;Ting Yang,&nbsp;J. Mark Weller,&nbsp;Hangkun Jing,&nbsp;Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1021\/acsami.7b12810\">ACS Appl. Mater. Interfaces<\/a><\/em> 2017, 9, 47, 41246\u201341257<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Type I silicon clathrates based on Ba<sub>8<\/sub>Al<sub><em>y<\/em><\/sub>Si<sub>46-<em>y<\/em><\/sub> (8 &lt; <em>y<\/em> &lt; 12) have been studied as potential anodes for lithium-ion batteries and display electrochemical properties that are distinct from those found in conventional silicon anodes. Processing steps such as ball-milling (typically used to reduce the particle size) and acid\/base treatment (used to remove nonclathrate impurities) may modify the clathrate surface structure or introduce defects, which could affect the observed electrochemical properties. In this work, we perform a systematic investigation of Ba<sub>8<\/sub>Al<sub><em>y<\/em><\/sub>Si<sub>46-<em>y<\/em><\/sub> clathrates with y \u2248 16, i.e, having a composition near Ba<sub>8<\/sub>Al<sub>16<\/sub>Si<sub>30<\/sub>, which perfectly satisfies the Zintl condition. The roles of ball-milling and acid\/base treatment were investigated using electrochemical, X-ray diffraction, electron microscopy, X-ray photoelectron and Raman spectroscopy analysis. The results showed that acid\/base treatment removed impurities from the synthesis, but also led to formation of a surface oxide layer that inhibited lithiation. Ball-milling could remove the surface oxide and result in the formation of an amorphous surface layer, with the observed charge storage capacity correlated with the thickness of this amorphous layer. According to the XRD and electrochemical analysis, all lithiation\/delithiation processes are proposed to occur in single phase reactions at the surface with no discernible changes to the crystal structure in the bulk. Electrochemical impedance spectroscopy results suggest that the mechanism of lithiation is through surface-dominated, Faradaic processes. This suggests that for off-stoichiometric clathrates, as we studied in our previous work, Li<sup>+<\/sup> insertion at defects or vacancies on the framework may be the origin of reversible Li cycling. However, for clathrates Ba<sub>8<\/sub>Al<sub><em>y<\/em><\/sub>Si<sub>46-<em>y<\/em><\/sub> with y \u2248 16, Li insertion in the structure is unfavorable and low capacities are observed unless amorphous surface layers are introduced by ball-milling.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image size-full is-resized is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-SECM.png\" alt=\"\" class=\"wp-image-171\" width=\"364\" height=\"354\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-SECM.png 727w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-SECM-500x487.png 500w\" sizes=\"auto, (max-width: 364px) 100vw, 364px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em><strong>Surface Properties of Battery Materials Elucidated Using Scanning Electrochemical Microscopy: The Case of Type I Silicon Clathrate<\/strong><\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Tsvetan Tarnev, Patrick Wilde, Andrew Dopilka,Wolfgang Schuhmann, Candace K. Chan, Edgar Ventosa<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1002\/celc.201901688\" data-type=\"URL\" data-id=\"https:\/\/doi.org\/10.1002\/celc.201901688\">ChemElectroChem<\/a> <\/em>2020, 7, 665-671<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Silicon clathrates have attracted interest as potential anodes for lithium-ion batteries with unique framework structures. However, very little is known about the surface reactivity and solid electrolyte interphase (SEI) properties of clathrates. In this study, <em>operando<\/em> scanning electrochemical microscopy (SECM) is used to investigate the effect of pre-treatment on the formation dynamics and intrinsic properties of the SEI in electrodes prepared from type\u2005I Ba<sub>8<\/sub>Al<sub>16<\/sub>Si<sub>30<\/sub> silicon clathrates. Although X-ray photoelectron spectroscopy (XPS) analysis does not reveal large changes in SEI composition, it is found through SECM measurements that ball-milling combined with chemical acid\/base etching of the clathrates lead to a more stable and rapidly formed SEI as compared to purely ball-milled samples, resulting in enhanced Coulombic efficiency.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"1334\" height=\"834\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Type-II-alloying.png\" alt=\"\" class=\"wp-image-331\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Type-II-alloying.png 1334w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Type-II-alloying-500x313.png 500w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Type-II-alloying-1000x625.png 1000w\" sizes=\"auto, (max-width: 1334px) 100vw, 1334px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Electrochemical Lithium Alloying Behavior of Guest-Free Type II Silicon Clathrates<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Amanda Childs, Svilen Bobev, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.1c04020\" data-type=\"URL\" data-id=\"https:\/\/doi.org\/10.1021\/acs.jpcc.1c04020\"><em>J. Phys. Chem. C<\/em><\/a> 2021, 125, 35, 19110\u201319118<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The guest-free type II Si clathrate (Si<sub>136<\/sub>) is an open framework polymorph of Si that displays unique electrochemical reactions with Li. Li ions are first topotactically inserted into the vacant clathrate cages, followed by an alloying reaction that forms an amorphous lithium silicide phase. The alloying reaction voltage is higher than those seen in other Si electrodes, suggesting that there are structural differences in the formed amorphous phases. Synchrotron X-ray total scattering measurements and pair distribution function analysis are employed to characterize the amorphous phases formed after lithiation. The results show that the clathrate becomes completely amorphous at an earlier stage of lithiation when compared to diamond cubic Si, forming a phase with comparatively larger amounts of Si\u2013Si bonding. The initial insertion of Li into the clathrate cages establishes important Li diffusion paths that kinetically enable the formation of an amorphous phase with lower Li content than typically seen in other silicon-based electrodes. After the initial crystalline-to-amorphous conversion reaction, lithiation takes place via solid-solution alloying. These results demonstrate how the topotactic insertion of Li into an alloying host can kinetically enable modified reaction pathways leading to more homogeneous lithiation throughout the electrode, which is beneficial for Li-ion battery applications.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-large is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"1500\" height=\"539\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Structural-origin-clathrate-1500x539.png\" alt=\"\" class=\"wp-image-333\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Structural-origin-clathrate-1500x539.png 1500w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Structural-origin-clathrate-500x180.png 500w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Structural-origin-clathrate-1000x360.png 1000w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Structural-origin-clathrate-1536x552.png 1536w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Structural-origin-clathrate.png 1963w\" sizes=\"auto, (max-width: 1500px) 100vw, 1500px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Structural Origin of Reversible Li Insertion in Guest\u2010Free, Type\u2010II Silicon Clathrates<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, J. Mark Weller, Alexander Ovchinnikov, Amanda Childs, Svilen Bobev, Xihong Peng, Candace K Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1002\/aesr.202000114\"><em>Adv. Energy Sustainability Res.<\/em><\/a> 2021, 2, 2000114<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The guest-free, type-II Si clathrate (Si<sub>136<\/sub>) is an open cage polymorph of Si with structural features amenable to electrochemical Li storage. However, the detailed mechanism for reversible Li insertion and migration within the vacant cages of Si<sub>136<\/sub> is not established. Herein, X-ray characterization and density functional theory (DFT) calculations are used to understand the structural origin of electrochemical Li insertion into the type-II clathrate structure. At low Li content, instead of alloying with Si, topotactic Li insertion into the empty cages occurs at \u22480.3\u2009V versus Li\/Li<sup>+<\/sup> with a capacity of \u2248231\u2009mAh\u2009g<sup>\u22121<\/sup> (corresponding to composition Li<sub>32<\/sub>Si<sub>136<\/sub>). A synchrotron powder X-ray diffraction analysis of electrodes after lithiation shows evidence of Li occupation within the Si<sub>20<\/sub> and Si<sub>28<\/sub> cages and a volume expansion of 0.22%, which is corroborated by DFT calculations. Nudged elastic band calculations suggest a low barrier (0.2\u2009eV) for Li migration through interconnected Si<sub>28<\/sub> cages, whereas there is a higher barrier for Li migration into Si<sub>20<\/sub> cages (2.0\u2009eV). However, if Li is present in a neighboring cage, a cooperative migration pathway with a barrier of 0.65\u2009eV is possible. The results show that the type-II Si clathrate displays unique electrochemical properties for potential applications as Li-ion battery anodes.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"1287\" height=\"599\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/HTEC-JECS.png\" alt=\"\" class=\"wp-image-162\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/HTEC-JECS.png 1287w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/HTEC-JECS-500x233.png 500w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/HTEC-JECS-1000x465.png 1000w\" sizes=\"auto, (max-width: 1287px) 100vw, 1287px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><strong><em>Solid-State Electrochemical Synthesis of Silicon Clathrates Using a Sodium-Sulfur Battery Inspired Approach<\/em><\/strong><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Amanda Childs, Svilen Bobev, Candace K Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1149\/1945-7111\/abdfe5\">J. Electrochem. Soc.<\/a> <\/em>2021, 168, 020516 <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em>Focus Issue on Future of Intercalation Chemistry for Energy Storage and Conversion in Honor of M. Stanley Whittingham<\/em><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Clathrates of Tetrel elements (Si, Ge, Sn) have attracted interest for their potential use in batteries and other applications. Sodium-filled silicon clathrates are conventionally synthesized through thermal decomposition of the Zintl precursor Na<sub>4<\/sub>Si<sub>4<\/sub>, but phase selectivity of the product is often difficult to achieve. Herein, we report the selective formation of the type I clathrate Na<sub>8<\/sub>Si<sub>46<\/sub> using electrochemical oxidation at 450 \u00b0C and 550 \u00b0C. A two-electrode cell design inspired by high-temperature sodium-sulfur batteries is employed, using Na<sub>4<\/sub>Si<sub>4<\/sub> as working electrode, Na <em>\u03b2&#8221;<\/em>-alumina solid electrolyte, and counter electrode consisting of molten Na or Sn. Galvanostatic intermittent titration is implemented to observe the oxidation characteristics and reveals a relatively constant cell potential under quasi-equilibrium conditions, indicating a two-phase reaction between Na<sub>4<\/sub>Si<sub>4<\/sub> and Na<sub>8<\/sub>Si<sub>46<\/sub>. We further demonstrate that the product selection and morphology can be altered by tuning the reaction temperature and Na vapor pressure. Room temperature lithiation of the synthesized Na<sub>8<\/sub>Si<sub>46<\/sub> is evaluated for the first time, showing similar electrochemical characteristics to those in the type II clathrate Na<sub>24<\/sub>Si<sub>136<\/sub>. The results show that solid-state electrochemical oxidation of Zintl phases at high temperatures can lead to opportunities for more controlled crystal growth and a deeper understanding of the formation processes of intermetallic clathrates.<\/p>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\" \/>\n\n\n\n<h2 class=\"wp-block-heading\"><span class=\"highlight-gold\">Germanium Clathrates<\/span><\/h2>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"297\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Ge-clathrate-1.png\" alt=\"\" class=\"wp-image-249\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><a><em>Experimental and Computational Study of the Lithiation of Ba<sub>8<\/sub>Al<sub>y<\/sub>Ge<sub>46-y<\/sub> Based Type I Germanium Clathrates<\/em><\/a><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Ran Zhao, J. Mark Weller, Svilen Bobev, Xihong Peng, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1021\/acsami.8b11509\">ACS Appl. Mater. Interfaces<\/a><\/em> 2018, 10, 44, 37981\u201337993<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">In this work, we investigate the electrochemical properties of Ba<sub>8<\/sub>Al<sub><em>y<\/em><\/sub>Ge<sub>46\u2013<em>y<\/em><\/sub> (<em>y<\/em> = 0, 4, 8, 12, 16) clathrates prepared by arc-melting. These materials have cage-like structures with large cavity volumes and can also have vacancies on the Ge framework sites, features which may be used to accommodate Li. Herein, a structural, electrochemical, and theoretical investigation is performed to explore these materials as anodes in Li-ion batteries, including analysis of the effect of the Al content and framework vacancies on the observed electrochemical properties. Single-crystal X-ray diffraction (XRD) studies indicate the presence of vacancies at the 6c site of the clathrate framework as the Al content decreases, and the lithiation potentials and capacities are observed to decrease as the degree of Al substitution increases. From XRD, electrochemical, and transmission electron microscopy analysis, we find that all of the clathrate compositions undergo two-phase reactions to form Li-rich amorphous phases. This is different from the behavior observed in Si clathrate analogues, where there is no amorphous phase transition during electrochemical lithiation nor discernible changes to the lattice constant of the bulk structure. From density functional theory calculations, we find that Li insertion into the three framework vacancies in Ba<sub>8<\/sub>Ge<sub>43<\/sub> is energetically favorable, with a calculated lithiation voltage of 0.77 V versus Li\/Li<sup>+<\/sup>. However, the calculated energy barrier for Li diffusion between vacancies and around Ba guest atoms is at least 1.6 eV, which is too high for significant room-temperature diffusion. These results show that framework vacancies in the Ge clathrate structure are unlikely to significantly contribute to lithiation processes unless the Ba guest atoms are absent, but suggest that guest atom vacancies could open diffusion paths for Li, allowing for empty framework positions to be occupied.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"583\" height=\"256\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Ge-clathrate-synchrotron.png\" alt=\"\" class=\"wp-image-161\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Ge-clathrate-synchrotron.png 583w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Ge-clathrate-synchrotron-500x220.png 500w\" sizes=\"auto, (max-width: 583px) 100vw, 583px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Understanding the Amorphous Lithiation Pathway of the Type I Ba<sub>8<\/sub>Ge<sub>43 <\/sub>Clathrate with Synchrotron X-ray Characterization<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Amanda Childs, Svilen Bobev, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acs.chemmater.0c03641\"><em>Chem. Mater.<\/em> <\/a>2020, 32, 21, 9444\u20139457<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Tetrel (Tt = Si, Ge, and Sn) clathrates have highly tunable host\u2013guest structures and have been investigated as novel electrode materials for Li-ion batteries. However, there is little understanding of how the clathrate structure affects the lithiation processes and phase evolution. Herein, the electrochemical lithiation pathway of type I clathrate Ba<sub>8<\/sub>Ge<sub>43<\/sub> is investigated with synchrotron X-ray diffraction (XRD) and pair distribution function (PDF) analyses and compared to the lithiation of germanium with a diamond cubic structure (\u03b1-Ge). The results confirm previous laboratory XRD studies showing that Ba<sub>8<\/sub>Ge<sub>43<\/sub> goes through a solely amorphous phase transformation, which contrasts with the crystalline phase transformations that take place during lithiation of micrometer-sized \u03b1-Ge particles. The local structure of framework-substituted clathrate Ba<sub>8<\/sub>Al<sub>16<\/sub>Ge<sub>30<\/sub> after lithiation is found to proceed through an amorphous phase transformation similar to that in Ba<sub>8<\/sub>Ge<sub>43<\/sub>. <em>In situ<\/em> PDF and XRD during heating show that the amorphous phases derived from lithiation of Ba<sub>8<\/sub>Ge<sub>43<\/sub> are structurally related to various Li\u2013Ge phases and crystallize at low temperatures (350\u2013420 K). We conclude that the Ba atoms inside the clathrate structure act to break up the long-range ordering of Li\u2013Ge clusters and kinetically prevent the nucleation and growth of bulk crystalline phases. The amorphous phase evolution of the clathrate structure during lithiation results in electrochemical properties distinct from those in \u03b1-Ge, such as a single-phase reaction mechanism and lower voltage, suggesting possible advantages of clathrates over elemental phases for use as anodes in Li-ion batteries.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"173\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Ge-clathrate-HTEC.png\" alt=\"\" class=\"wp-image-272\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Synthesis of Type II Ge and Ge\u2013Si Alloyed Clathrates Using Solid-State Electrochemical Oxidation of Zintl Phase Precursors<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Alexander Ovchinnikov, Amanda Childs, Svilen Bobev, Xihong Peng, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acs.inorgchem.2c01748\"><em>Inorg. Chem.<\/em><\/a> 2022, 61, 31, 12363\u201312372<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Germanium clathrates with the type II structure are open-framework materials that show promise for various applications, but the difficulty of achieving phase-pure products via traditional synthesis routes has hindered their development. Herein, we demonstrate the synthesis of type II Ge clathrates in a two-electrode electrochemical cell using Na<sub>4<\/sub>Ge<sub>4\u2013<em>y<\/em><\/sub>Si<em><sub>y<\/sub><\/em> (<em>y<\/em> = 0, 1) Zintl phase precursors as the working electrode, Na metal as the counter\/reference electrode, and Na-ion conducting \u03b2\u2033-alumina as the solid electrolyte. The galvanostatic oxidation of Na<sub>4<\/sub>Ge<sub>4<\/sub> resulted in voltage plateaus around 0.34\u20130.40 V vs Na\/Na<sup>+<\/sup> with the formation of different products depending on the reaction temperature. When using Na<sub>4<\/sub>Ge<sub>3<\/sub>Si as a precursor, nearly phase-pure, alloyed type II Ge\u2013Si clathrate was obtained at 350 \u00b0C. The Na atoms in the large (Ge,Si)<sub>28<\/sub> cages of the clathrate occupied off-centered positions according to Rietveld refinement and density functional theory calculations. The results indicate that electrochemical oxidation of Zintl phase precursors is a promising pathway for synthesizing Ge clathrates with type II structure and that Si alloying of the Zintl phase precursor can promote selective clathrate product formation over other phases.<\/p>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\" \/>\n\n\n\n<h2 class=\"wp-block-heading\"><span class=\"highlight-gold\">Tin Clathrates<\/span><\/h2>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"216\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Sn-clathrate.png\" alt=\"\" class=\"wp-image-267\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>Structural and Electrochemical Properties of Type VIII Ba<sub>8<\/sub>Ga<sub>16\u2212\u03b4<\/sub>Sn<sub>30+\u03b4<\/sub> Clathrate (\u03b4 \u2248 1) during Lithiation<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Amanda Childs, Alexander Ovchinnikov, Ran Zhao, Svilen Bobev, Xihong Peng, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acsami.1c07240\"><em>ACS Appl. Mater. Interfaces<\/em><\/a> 2021, 13, 36, 42564\u201342578<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Clathrates of the tetrel (Tt = Si, Ge, Sn) elements are host\u2013guest structures that can undergo Li alloying reactions with high capacities. However, little is known about how the cage structure affects the phase transformations that take place during lithiation. To further this understanding, the structural changes of the type VIII clathrate Ba<sub>8<\/sub>Ga<sub>16\u2212\u03b4<\/sub>Sn<sub>30+\u03b4<\/sub> (\u03b4 \u2248 1) during lithiation are investigated and compared to those in \u03b2-Sn with <em>ex situ<\/em> X-ray total scattering measurements and pair distribution function (PDF) analysis. The results show that the type VIII clathrate undergoes an alloying reaction to form Li-rich amorphous phases (Li<sub><em>x<\/em><\/sub>Ba<sub>0.17<\/sub>Ga<sub>0.33<\/sub>Sn<sub>0.67<\/sub>, <em>x<\/em> = 2\u20133) with local structures similar to those in the crystalline binary Li\u2013Sn phases that form during the lithiation of \u03b2-Sn. As a result of the amorphous phase transition, the type VIII clathrate reacts at a lower voltage (0.25 V <em>vs<\/em> Li\/Li<sup>+<\/sup>) compared to \u03b2-Sn (0.45 V) and goes through a solid-solution reaction after the initial conversion of the crystalline clathrate phase. Cycling experiments suggest that the amorphous phase persists after the first lithiation and results in considerably better cycling than in \u03b2-Sn. Density functional theory (DFT) calculations suggest that topotactic Li insertion into the clathrate lattice is not favorable due to the high energy of the Li sites, which is consistent with the experimentally observed amorphous phase transformation. The local structure in the clathrate featuring Ba atoms surrounded by a cage of Ga and Sn atoms is hypothesized to kinetically circumvent the formation of Li\u2013Sn or Li\u2013Ga crystalline phases, which results in better cycling and a lower reaction voltage. Based on the improved electrochemical performance, clathrates could act as tunable precursors to form amorphous Li alloying phases with novel electrochemical properties.<\/p>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\" \/>\n\n\n\n<h2 class=\"wp-block-heading\"><span class=\"highlight-gold\">Ab Initio Studies<\/span><span class=\"highlight-gold\"><\/span><\/h2>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"256\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/Clathrate-DFT.png\" alt=\"\" class=\"wp-image-212\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>First-Principles Study of Lithiation of Type I Ba-doped Silicon Clathrates<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Xihong Peng, Qun Wei, Ying Li, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.5b07523\">J. Phys. Chem. C<\/a><\/em> 2015, 119, 51, 28247\u201328257<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Silicon clathrate materials, previously known for their superconducting and thermoelectric characteristics, have also recently been investigated for their electrochemical properties as anodes for lithium-ion batteries due to their unique cage structure and ability to incorporate extrinsic guest atoms. To better understand the preferred structures for small degrees of lithiation, first-principles density functional theory (DFT) was used to investigate the type I clathrate compounds Si<sub>46<\/sub>, Li<sub><em>x<\/em><\/sub>Ba<sub><em>y<\/em><\/sub>Si<sub>46<\/sub> (0 \u2264 <em>x<\/em> \u2264 8; <em>y<\/em> = 6, 8), and Li<sub><em>x<\/em><\/sub>Ba<sub><em>y<\/em><\/sub>Al<sub>6<\/sub>Si<sub>40<\/sub> (0 \u2264 <em>x<\/em> \u2264 8; <em>y<\/em> = 6). The formation energies, electronic band structures, and density of states (DOS) were calculated. Lithium occupation in framework vacancies, empty and Ba-occupied cage cavities, and near the pentagonal and hexagonal faces of the clathrate polyhedra was considered. The data showed that Li insertion into framework or Ba vacancies could stabilize the clathrate structure. Silicon substitution by Al lowered the formation energies of the lithiated compounds and mitigated the calculated volume increase upon lithiation. The results also showed that it is energetically feasible for multiple guest atoms to be placed in the Si<sub>24<\/sub> cages. Changes in the clathrate atomic structure (e.g., bond lengths and angles) and electronic structure were highly dependent on the location of the Li and guest atom spacing within the clathrate framework. The results from this study can elucidate the preferred structural configurations for Li in type I, Ba-doped silicon clathrates and also be informative for efforts related to understanding the structures obtained after electrochemical insertion of lithium into silicon clathrates.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"690\" height=\"501\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/EmptySi46-JMR.png\" alt=\"\" class=\"wp-image-326\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/EmptySi46-JMR.png 690w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/EmptySi46-JMR-500x363.png 500w\" sizes=\"auto, (max-width: 690px) 100vw, 690px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><em>First Principles and Experimental Studies of Empty Si<sub>46<\/sub> as Anode Materials for Li-ion Batteries<\/em><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Kwai S. Chan, Michael A. Miller, Wuwei Liang, Carol Ellis-Terrell, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><em><a href=\"https:\/\/doi.org\/10.1557\/jmr.2016.408\">J. Mater. Res.<\/a><\/em> 2016, 31, 3657-3665<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The objective of this investigation was to utilize the first-principles molecular dynamics computational approach to investigate the lithiation characteristics of empty silicon clathrates (Si<sup><sub>46<\/sub><\/sup>) for applications as potential anode materials in lithium-ion batteries. The energy of formation, volume expansion, and theoretical capacity were computed for empty silicon clathrates as a function of Li. The theoretical results were compared against experimental data of long-term cyclic tests performed on half-cells using electrodes fabricated from Si<sub>46 <\/sub>prepared using a Hofmann-type elimination\u2013oxidation reaction. The comparison revealed that the theoretically predicted capacity (of 791.6 mAh\/g) agreed with experimental data (809 mAh\/g) that occurred after insertion of 48 Li atoms. The calculations showed that overlithiation beyond 66 Li atoms can cause large volume expansion with a volume strain as high as 120%, which may correlate to experimental observations of decreasing capacities from the maximum at 1030 mAh\/g to 553 mA h\/g during long-term cycling tests. The finding suggests that overlithiation beyond 66 Li atoms may have caused damage to the cage structure and led to lower reversible capacities.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-930feb06 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image size-full is-style-drop-shadow\"><img loading=\"lazy\" decoding=\"async\" width=\"704\" height=\"398\" src=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/DFT-guestfree.png\" alt=\"\" class=\"wp-image-160\" srcset=\"https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/DFT-guestfree.png 704w, https:\/\/faculty.engineering.asu.edu\/chan\/wp-content\/uploads\/sites\/47\/2022\/09\/DFT-guestfree-500x283.png 500w\" sizes=\"auto, (max-width: 704px) 100vw, 704px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<h3 class=\"wp-block-heading\"><strong><em><a>Ab Initio <\/a>Investigation of Li and Na Migration in Guest Free, Type I Clathrates<\/em><\/strong><\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Andrew Dopilka, Xihong Peng, Candace K. Chan<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/doi.org\/10.1021\/acs.jpcc.9b06424\" target=\"_blank\" rel=\"noreferrer noopener\"><em>J. Phys. Chem. C<\/em><\/a> 2019, 123, 37, 22812\u201322822<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Guest-free, type I clathrates with formula Tt<sub>46<\/sub> (Tt = Si, Ge, Sn) are comprised of open, cage-like frameworks with the potential for facile Li or Na conduction. Herein, ab initio density functional theory (DFT) is used to evaluate the ionic mobility of Li and Na through the clathrate crystal structures. The favorable Li and Na positions inside the clathrate structures are determined, and the migration pathways and barriers are evaluated using the nudged elastic band (NEB) method. The results show that it is energetically favorable for a Li atom to occupy the center position inside the small Tt<sub>20<\/sub> cages while preferring the off-center positions in the larger Tt<sub>24<\/sub> cages. The lowest Li migration barriers are found to be 0.35, 0.13 and 0.37 eV for Si<sub>46<\/sub>, Ge<sub>46<\/sub>, and Sn<sub>46<\/sub>, respectively, with the dominant diffusion pathway along channels of Tt<sub>24<\/sub> cages connected by hexagonal faces. Li accessibility to the Si<sub>20<\/sub> cage in Si<sub>46<\/sub> appears to be restricted in the dilute regime due to a high energy barrier (2.0 eV) except for the case in which Li atoms are present in adjacent cages; this lowers the migration barrier to 0.77 eV via a mechanism where a Si\u2013Si bond is temporarily broken. In contrast, Na atoms show preference for the cage centers and display higher migration barriers than Li. Overall, the Tt<sub>24<\/sub> channel sizes in the guest-free, type I clathrates are ideal for fast Li diffusion, while Na is too large to migrate effectively between cages. The energy landscape for Li inside the type I clathrates is uniquely different than that in diamond cubic structures, leading to significantly lower energy barriers for Li migration. These results suggest that open frameworks of intermetallic elements may enable facile Li migration and have potential use as Li-ion battery anodes.<\/p>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p class=\"mb-2\">Overview The group 14 or Tetrel (Tt) elements (Si, Ge, Sn) have received significant attention as high capacity anodes for Li-ion batteries due to their ability to alloy with large amounts of Li. Tetrel clathrates have cage-like structures composed of face-sharing Tt20, Tt24, and Tt28 polyhedra that boast strong Tt\u2013Tt bonds with covalent sp3-character. Due&#8230;<\/p>\n","protected":false},"author":105,"featured_media":0,"parent":0,"menu_order":9,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-157","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/pages\/157","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/users\/105"}],"replies":[{"embeddable":true,"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/comments?post=157"}],"version-history":[{"count":0,"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/pages\/157\/revisions"}],"wp:attachment":[{"href":"https:\/\/faculty.engineering.asu.edu\/chan\/wp-json\/wp\/v2\/media?parent=157"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}