Structural and Electrical Effects of Y-doped Li0.33La0.56−xYxTiO3 Solid Electrolytes on All-Solid-State Lithium Ion Batteries
Li 0.33 La 0.56 TiO 3 (LLTO) solid state electrolytes have been considered as candidates to substitute for organic liquid electrolytes in lithium batteries. LLTO consist of a mixture of cubic phases with Pm3m symmetry ( α -LLTO) and with tetragonal P4/mmm symmetry ( β -LLTO). The α -LLTO phase has a...
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creator | Lee, Seon-Jin Bae, Jin-Ju Son, Jong-Tae |
description | Li
0.33
La
0.56
TiO
3
(LLTO) solid state electrolytes have been considered as candidates to substitute for organic liquid electrolytes in lithium batteries. LLTO consist of a mixture of cubic phases with Pm3m symmetry (
α
-LLTO) and with tetragonal P4/mmm symmetry (
β
-LLTO). The
α
-LLTO phase has a higher Li ion conductivity than the
β
-LLTO phase. However,
α
-LLTO is characterized by high lattice strain, which induces the formation of
β
-LLTO due to the different atomic sizes of Li
+
(0.76 Å) and La
3+
(1.03 Å). In this study, to reduce lattice stress, we prepared Y-doped Li
0.33
La
0.56−
x
Y
x
TiO
3
(
x
= 0.02, 0.05, 0.1) by using the sol-gel method. Because the ionic radius of Y
3+
is 0.90 Å, that is, larger than that of Li
+
(0.76 Å) and smaller than that of La
3+
(1.03 Å), Y
3+
suppresses the lattice distortion that prevents the formation of
α
-LLTO. The structural, morphological, and electrical characteristics of pure and Y
3+
-doped LLTO were investigated. The results show that Li
0.33
La
0.46
Y
0.1
TiO
3
exhibits a better bulk conductivity (
σ
= 9.51 × 10
−4
S cm
−1
) at 25 °C due to the increasing volume fraction of the more conductive
α
-LLTO phase. |
doi_str_mv | 10.3938/jkps.74.73 |
format | Article |
fullrecord | <record><control><sourceid>crossref_sprin</sourceid><recordid>TN_cdi_crossref_primary_10_3938_jkps_74_73</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_3938_jkps_74_73</sourcerecordid><originalsourceid>FETCH-LOGICAL-c267t-e1cde84143fd88c6d6f9e969da566e566125de29fd61b2adc87498b9308e2d803</originalsourceid><addsrcrecordid>eNptkL9OwzAQxi0EEqWw8ASeQQ5O7PjPWKoClSJ1aBk6Ra7tQEqaVLYjtRMrM4_Ik-BS2BhOd6fv992dDoDrFCdEEnG3ftv6hNOEkxMwSCVnSOQZPQUDTDhFVAh6Di68X2NMCeFsAN7nwfU69E41ULUGThqrg6t1bCdVFWsPuwoukem21sCijntIoXCSs6-Pz91yt6hnBM67pv6zds0-2Ghq4ahp0I-C5kEFG83hte43cBq1exWCdbX1l-CsUo23V795CJ4fJovxEypmj9PxqEA6Yzwgm2pjBU0pqYwQmhlWSSuZNCpnzMZIs9zYTFaGpatMGS04lWIlCRY2MwKTIbg5ztWu897Zqty6eqPcvkxxeXhdeXhdyWnJSYRvj7CPUPtiXbnuetfG-_6jvwHbhnJM</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Structural and Electrical Effects of Y-doped Li0.33La0.56−xYxTiO3 Solid Electrolytes on All-Solid-State Lithium Ion Batteries</title><source>SpringerLink Journals</source><creator>Lee, Seon-Jin ; Bae, Jin-Ju ; Son, Jong-Tae</creator><creatorcontrib>Lee, Seon-Jin ; Bae, Jin-Ju ; Son, Jong-Tae</creatorcontrib><description>Li
0.33
La
0.56
TiO
3
(LLTO) solid state electrolytes have been considered as candidates to substitute for organic liquid electrolytes in lithium batteries. LLTO consist of a mixture of cubic phases with Pm3m symmetry (
α
-LLTO) and with tetragonal P4/mmm symmetry (
β
-LLTO). The
α
-LLTO phase has a higher Li ion conductivity than the
β
-LLTO phase. However,
α
-LLTO is characterized by high lattice strain, which induces the formation of
β
-LLTO due to the different atomic sizes of Li
+
(0.76 Å) and La
3+
(1.03 Å). In this study, to reduce lattice stress, we prepared Y-doped Li
0.33
La
0.56−
x
Y
x
TiO
3
(
x
= 0.02, 0.05, 0.1) by using the sol-gel method. Because the ionic radius of Y
3+
is 0.90 Å, that is, larger than that of Li
+
(0.76 Å) and smaller than that of La
3+
(1.03 Å), Y
3+
suppresses the lattice distortion that prevents the formation of
α
-LLTO. The structural, morphological, and electrical characteristics of pure and Y
3+
-doped LLTO were investigated. The results show that Li
0.33
La
0.46
Y
0.1
TiO
3
exhibits a better bulk conductivity (
σ
= 9.51 × 10
−4
S cm
−1
) at 25 °C due to the increasing volume fraction of the more conductive
α
-LLTO phase.</description><identifier>ISSN: 0374-4884</identifier><identifier>EISSN: 1976-8524</identifier><identifier>DOI: 10.3938/jkps.74.73</identifier><language>eng</language><publisher>Seoul: The Korean Physical Society</publisher><subject>Mathematical and Computational Physics ; Particle and Nuclear Physics ; Physics ; Physics and Astronomy ; Theoretical</subject><ispartof>Journal of the Korean Physical Society, 2019, Vol.74 (1), p.73-77</ispartof><rights>The Korean Physical Society 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c267t-e1cde84143fd88c6d6f9e969da566e566125de29fd61b2adc87498b9308e2d803</citedby><cites>FETCH-LOGICAL-c267t-e1cde84143fd88c6d6f9e969da566e566125de29fd61b2adc87498b9308e2d803</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.3938/jkps.74.73$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.3938/jkps.74.73$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Lee, Seon-Jin</creatorcontrib><creatorcontrib>Bae, Jin-Ju</creatorcontrib><creatorcontrib>Son, Jong-Tae</creatorcontrib><title>Structural and Electrical Effects of Y-doped Li0.33La0.56−xYxTiO3 Solid Electrolytes on All-Solid-State Lithium Ion Batteries</title><title>Journal of the Korean Physical Society</title><addtitle>J. Korean Phys. Soc</addtitle><description>Li
0.33
La
0.56
TiO
3
(LLTO) solid state electrolytes have been considered as candidates to substitute for organic liquid electrolytes in lithium batteries. LLTO consist of a mixture of cubic phases with Pm3m symmetry (
α
-LLTO) and with tetragonal P4/mmm symmetry (
β
-LLTO). The
α
-LLTO phase has a higher Li ion conductivity than the
β
-LLTO phase. However,
α
-LLTO is characterized by high lattice strain, which induces the formation of
β
-LLTO due to the different atomic sizes of Li
+
(0.76 Å) and La
3+
(1.03 Å). In this study, to reduce lattice stress, we prepared Y-doped Li
0.33
La
0.56−
x
Y
x
TiO
3
(
x
= 0.02, 0.05, 0.1) by using the sol-gel method. Because the ionic radius of Y
3+
is 0.90 Å, that is, larger than that of Li
+
(0.76 Å) and smaller than that of La
3+
(1.03 Å), Y
3+
suppresses the lattice distortion that prevents the formation of
α
-LLTO. The structural, morphological, and electrical characteristics of pure and Y
3+
-doped LLTO were investigated. The results show that Li
0.33
La
0.46
Y
0.1
TiO
3
exhibits a better bulk conductivity (
σ
= 9.51 × 10
−4
S cm
−1
) at 25 °C due to the increasing volume fraction of the more conductive
α
-LLTO phase.</description><subject>Mathematical and Computational Physics</subject><subject>Particle and Nuclear Physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Theoretical</subject><issn>0374-4884</issn><issn>1976-8524</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNptkL9OwzAQxi0EEqWw8ASeQQ5O7PjPWKoClSJ1aBk6Ra7tQEqaVLYjtRMrM4_Ik-BS2BhOd6fv992dDoDrFCdEEnG3ftv6hNOEkxMwSCVnSOQZPQUDTDhFVAh6Di68X2NMCeFsAN7nwfU69E41ULUGThqrg6t1bCdVFWsPuwoukem21sCijntIoXCSs6-Pz91yt6hnBM67pv6zds0-2Ghq4ahp0I-C5kEFG83hte43cBq1exWCdbX1l-CsUo23V795CJ4fJovxEypmj9PxqEA6Yzwgm2pjBU0pqYwQmhlWSSuZNCpnzMZIs9zYTFaGpatMGS04lWIlCRY2MwKTIbg5ztWu897Zqty6eqPcvkxxeXhdeXhdyWnJSYRvj7CPUPtiXbnuetfG-_6jvwHbhnJM</recordid><startdate>2019</startdate><enddate>2019</enddate><creator>Lee, Seon-Jin</creator><creator>Bae, Jin-Ju</creator><creator>Son, Jong-Tae</creator><general>The Korean Physical Society</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>2019</creationdate><title>Structural and Electrical Effects of Y-doped Li0.33La0.56−xYxTiO3 Solid Electrolytes on All-Solid-State Lithium Ion Batteries</title><author>Lee, Seon-Jin ; Bae, Jin-Ju ; Son, Jong-Tae</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c267t-e1cde84143fd88c6d6f9e969da566e566125de29fd61b2adc87498b9308e2d803</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Mathematical and Computational Physics</topic><topic>Particle and Nuclear Physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Theoretical</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lee, Seon-Jin</creatorcontrib><creatorcontrib>Bae, Jin-Ju</creatorcontrib><creatorcontrib>Son, Jong-Tae</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of the Korean Physical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lee, Seon-Jin</au><au>Bae, Jin-Ju</au><au>Son, Jong-Tae</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural and Electrical Effects of Y-doped Li0.33La0.56−xYxTiO3 Solid Electrolytes on All-Solid-State Lithium Ion Batteries</atitle><jtitle>Journal of the Korean Physical Society</jtitle><stitle>J. Korean Phys. Soc</stitle><date>2019</date><risdate>2019</risdate><volume>74</volume><issue>1</issue><spage>73</spage><epage>77</epage><pages>73-77</pages><issn>0374-4884</issn><eissn>1976-8524</eissn><abstract>Li
0.33
La
0.56
TiO
3
(LLTO) solid state electrolytes have been considered as candidates to substitute for organic liquid electrolytes in lithium batteries. LLTO consist of a mixture of cubic phases with Pm3m symmetry (
α
-LLTO) and with tetragonal P4/mmm symmetry (
β
-LLTO). The
α
-LLTO phase has a higher Li ion conductivity than the
β
-LLTO phase. However,
α
-LLTO is characterized by high lattice strain, which induces the formation of
β
-LLTO due to the different atomic sizes of Li
+
(0.76 Å) and La
3+
(1.03 Å). In this study, to reduce lattice stress, we prepared Y-doped Li
0.33
La
0.56−
x
Y
x
TiO
3
(
x
= 0.02, 0.05, 0.1) by using the sol-gel method. Because the ionic radius of Y
3+
is 0.90 Å, that is, larger than that of Li
+
(0.76 Å) and smaller than that of La
3+
(1.03 Å), Y
3+
suppresses the lattice distortion that prevents the formation of
α
-LLTO. The structural, morphological, and electrical characteristics of pure and Y
3+
-doped LLTO were investigated. The results show that Li
0.33
La
0.46
Y
0.1
TiO
3
exhibits a better bulk conductivity (
σ
= 9.51 × 10
−4
S cm
−1
) at 25 °C due to the increasing volume fraction of the more conductive
α
-LLTO phase.</abstract><cop>Seoul</cop><pub>The Korean Physical Society</pub><doi>10.3938/jkps.74.73</doi><tpages>5</tpages></addata></record> |
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issn | 0374-4884 1976-8524 |
language | eng |
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source | SpringerLink Journals |
subjects | Mathematical and Computational Physics Particle and Nuclear Physics Physics Physics and Astronomy Theoretical |
title | Structural and Electrical Effects of Y-doped Li0.33La0.56−xYxTiO3 Solid Electrolytes on All-Solid-State Lithium Ion Batteries |
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