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Toward understanding the second universality—A journey inspired by Arthur Stanley Nowick
In 1991, Arthur Stanley Nowick and his co-workers discovered a new universality, now known as nearly constant loss (NCL) or second universality. This mini-review, written in honor of A.S. Nowick, reports on the present authors’ more recent endeavors and advances on their way toward understanding the...
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Published in: | Journal of electroceramics 2015-02, Vol.34 (1), p.4-14 |
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description | In 1991, Arthur Stanley Nowick and his co-workers discovered a new universality, now known as nearly constant loss (NCL) or second universality. This mini-review, written in honor of A.S. Nowick, reports on the present authors’ more recent endeavors and advances on their way toward understanding the second-universality phenomenon. In pursuit of that goal, new ideas and new data have led us to new questions and new answers. The essence of the
new ideas
was to consider time-dependent single-particle potentials, caused by Coulomb interactions and experienced by locally mobile ions. The dynamics of such ions were described in terms of a rate equation, and model conductivity spectra showing the NCL effect could be derived from it, with the help of linear response theory.
New data
corroborated the predictions made by the model. Also, our experimental data suggested a gradual transition, occurring with decreasing temperature, from a slightly activated NCL-type behavior to the non-activated features of the second universality. Two
new questions
have emerged. (i) Is it possible to quantify the transition mentioned above? (ii) Is there a crossover of the low-temperature, second-universality ionic conductivity from its characteristic linear frequency dependence to a quadratic one at low frequencies?
New answers
to our two questions can now be given, both of them in the affirmative. In particular, the crossover in the frequency dependence has been identified as an implication of the localization of the non-activated ionic motion. |
doi_str_mv | 10.1007/s10832-014-9898-0 |
format | article |
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new ideas
was to consider time-dependent single-particle potentials, caused by Coulomb interactions and experienced by locally mobile ions. The dynamics of such ions were described in terms of a rate equation, and model conductivity spectra showing the NCL effect could be derived from it, with the help of linear response theory.
New data
corroborated the predictions made by the model. Also, our experimental data suggested a gradual transition, occurring with decreasing temperature, from a slightly activated NCL-type behavior to the non-activated features of the second universality. Two
new questions
have emerged. (i) Is it possible to quantify the transition mentioned above? (ii) Is there a crossover of the low-temperature, second-universality ionic conductivity from its characteristic linear frequency dependence to a quadratic one at low frequencies?
New answers
to our two questions can now be given, both of them in the affirmative. In particular, the crossover in the frequency dependence has been identified as an implication of the localization of the non-activated ionic motion.</description><identifier>ISSN: 1385-3449</identifier><identifier>EISSN: 1573-8663</identifier><identifier>DOI: 10.1007/s10832-014-9898-0</identifier><language>eng</language><publisher>Boston: Springer US</publisher><subject>Ceramics ; Characterization and Evaluation of Materials ; Chemistry and Materials Science ; Composites ; Constants ; Coulomb friction ; Crossovers ; Crystallography and Scattering Methods ; Electrochemistry ; Glass ; Ionic conductivity ; Journeys ; Low frequencies ; Materials Science ; Mathematical analysis ; Mathematical models ; Natural Materials ; Optical and Electronic Materials</subject><ispartof>Journal of electroceramics, 2015-02, Vol.34 (1), p.4-14</ispartof><rights>The Author(s) 2014</rights><rights>Springer Science+Business Media New York 2015</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c462t-e07226fdb09d9438dd6802b9f075be3efbaa260b578d396ffa51135e702a46673</citedby><cites>FETCH-LOGICAL-c462t-e07226fdb09d9438dd6802b9f075be3efbaa260b578d396ffa51135e702a46673</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Funke, Klaus</creatorcontrib><creatorcontrib>Banhatti, Radha D.</creatorcontrib><creatorcontrib>Badr, Layla G.</creatorcontrib><creatorcontrib>Laughman, David M.</creatorcontrib><creatorcontrib>Jain, Himanshu</creatorcontrib><title>Toward understanding the second universality—A journey inspired by Arthur Stanley Nowick</title><title>Journal of electroceramics</title><addtitle>J Electroceram</addtitle><description>In 1991, Arthur Stanley Nowick and his co-workers discovered a new universality, now known as nearly constant loss (NCL) or second universality. This mini-review, written in honor of A.S. Nowick, reports on the present authors’ more recent endeavors and advances on their way toward understanding the second-universality phenomenon. In pursuit of that goal, new ideas and new data have led us to new questions and new answers. The essence of the
new ideas
was to consider time-dependent single-particle potentials, caused by Coulomb interactions and experienced by locally mobile ions. The dynamics of such ions were described in terms of a rate equation, and model conductivity spectra showing the NCL effect could be derived from it, with the help of linear response theory.
New data
corroborated the predictions made by the model. Also, our experimental data suggested a gradual transition, occurring with decreasing temperature, from a slightly activated NCL-type behavior to the non-activated features of the second universality. Two
new questions
have emerged. (i) Is it possible to quantify the transition mentioned above? (ii) Is there a crossover of the low-temperature, second-universality ionic conductivity from its characteristic linear frequency dependence to a quadratic one at low frequencies?
New answers
to our two questions can now be given, both of them in the affirmative. In particular, the crossover in the frequency dependence has been identified as an implication of the localization of the non-activated ionic motion.</description><subject>Ceramics</subject><subject>Characterization and Evaluation of Materials</subject><subject>Chemistry and Materials Science</subject><subject>Composites</subject><subject>Constants</subject><subject>Coulomb friction</subject><subject>Crossovers</subject><subject>Crystallography and Scattering Methods</subject><subject>Electrochemistry</subject><subject>Glass</subject><subject>Ionic conductivity</subject><subject>Journeys</subject><subject>Low frequencies</subject><subject>Materials Science</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Natural Materials</subject><subject>Optical and Electronic Materials</subject><issn>1385-3449</issn><issn>1573-8663</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp1kLtOw0AQRS0EEiHwAXSWaGgMsw_vo4wiXlIEBaGhWa2968TBscOuTeSOj-AL-RI2mAIhUc1I99yrmRtFpwguEAC_9AgEwQkgmkghRQJ70QilnCSCMbIfdiLShFAqD6Mj71cAIAVFo-h53my1M3FXG-t8q2tT1ou4XdrY27ypd0L5FhRdlW3_-f4xiVdN52rbx2XtN6WzJs76eOLaZefix-CvgnTfbMv85Tg6KHTl7cnPHEdP11fz6W0ye7i5m05mSU4ZbhMLHGNWmAykkZQIY5gAnMkCeJpZYotMa8wgS7kwRLKi0ClCJLUcsKaMcTKOzofcjWteO-tbtS59bqtK17bpvEJMpFxSSllAz_6g39-E6wLFBKESUxQoNFC5a7x3tlAbV6616xUCtWtbDW2r0Lbata0gePDg8YGtF9b9Sv7X9AW4YoN9</recordid><startdate>20150201</startdate><enddate>20150201</enddate><creator>Funke, Klaus</creator><creator>Banhatti, Radha D.</creator><creator>Badr, Layla G.</creator><creator>Laughman, David M.</creator><creator>Jain, Himanshu</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20150201</creationdate><title>Toward understanding the second universality—A journey inspired by Arthur Stanley Nowick</title><author>Funke, Klaus ; Banhatti, Radha D. ; Badr, Layla G. ; Laughman, David M. ; Jain, Himanshu</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c462t-e07226fdb09d9438dd6802b9f075be3efbaa260b578d396ffa51135e702a46673</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Ceramics</topic><topic>Characterization and Evaluation of Materials</topic><topic>Chemistry and Materials Science</topic><topic>Composites</topic><topic>Constants</topic><topic>Coulomb friction</topic><topic>Crossovers</topic><topic>Crystallography and Scattering Methods</topic><topic>Electrochemistry</topic><topic>Glass</topic><topic>Ionic conductivity</topic><topic>Journeys</topic><topic>Low frequencies</topic><topic>Materials Science</topic><topic>Mathematical analysis</topic><topic>Mathematical models</topic><topic>Natural Materials</topic><topic>Optical and Electronic Materials</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Funke, Klaus</creatorcontrib><creatorcontrib>Banhatti, Radha D.</creatorcontrib><creatorcontrib>Badr, Layla G.</creatorcontrib><creatorcontrib>Laughman, David M.</creatorcontrib><creatorcontrib>Jain, Himanshu</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of electroceramics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Funke, Klaus</au><au>Banhatti, Radha D.</au><au>Badr, Layla G.</au><au>Laughman, David M.</au><au>Jain, Himanshu</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Toward understanding the second universality—A journey inspired by Arthur Stanley Nowick</atitle><jtitle>Journal of electroceramics</jtitle><stitle>J Electroceram</stitle><date>2015-02-01</date><risdate>2015</risdate><volume>34</volume><issue>1</issue><spage>4</spage><epage>14</epage><pages>4-14</pages><issn>1385-3449</issn><eissn>1573-8663</eissn><abstract>In 1991, Arthur Stanley Nowick and his co-workers discovered a new universality, now known as nearly constant loss (NCL) or second universality. This mini-review, written in honor of A.S. Nowick, reports on the present authors’ more recent endeavors and advances on their way toward understanding the second-universality phenomenon. In pursuit of that goal, new ideas and new data have led us to new questions and new answers. The essence of the
new ideas
was to consider time-dependent single-particle potentials, caused by Coulomb interactions and experienced by locally mobile ions. The dynamics of such ions were described in terms of a rate equation, and model conductivity spectra showing the NCL effect could be derived from it, with the help of linear response theory.
New data
corroborated the predictions made by the model. Also, our experimental data suggested a gradual transition, occurring with decreasing temperature, from a slightly activated NCL-type behavior to the non-activated features of the second universality. Two
new questions
have emerged. (i) Is it possible to quantify the transition mentioned above? (ii) Is there a crossover of the low-temperature, second-universality ionic conductivity from its characteristic linear frequency dependence to a quadratic one at low frequencies?
New answers
to our two questions can now be given, both of them in the affirmative. In particular, the crossover in the frequency dependence has been identified as an implication of the localization of the non-activated ionic motion.</abstract><cop>Boston</cop><pub>Springer US</pub><doi>10.1007/s10832-014-9898-0</doi><tpages>11</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Ceramics Characterization and Evaluation of Materials Chemistry and Materials Science Composites Constants Coulomb friction Crossovers Crystallography and Scattering Methods Electrochemistry Glass Ionic conductivity Journeys Low frequencies Materials Science Mathematical analysis Mathematical models Natural Materials Optical and Electronic Materials |
title | Toward understanding the second universality—A journey inspired by Arthur Stanley Nowick |
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