<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>0122-7483</journal-id>
<journal-title><![CDATA[Universitas Scientiarum]]></journal-title>
<abbrev-journal-title><![CDATA[Univ. Sci.]]></abbrev-journal-title>
<issn>0122-7483</issn>
<publisher>
<publisher-name><![CDATA[Facultad de Ciencias de la Pontificia Universidad Javeriana de Bogotá.]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0122-74832017000200113</article-id>
<article-id pub-id-type="doi">10.11144/javeriana.sc22-2.vifd</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Variations in ß(T)-function due to addition of LiI-4AgI system]]></article-title>
<article-title xml:lang="es"><![CDATA[Variaciones en la función ß(T) - por la adición del sistema LiI-4AgI]]></article-title>
<article-title xml:lang="pt"><![CDATA[Variações na função ß(T) devido a adição do sistema Lil-4Agl]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Lozano Zapata]]></surname>
<given-names><![CDATA[Carlos Alberto]]></given-names>
</name>
<xref ref-type="aff" rid="Aff"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Peña Lara]]></surname>
<given-names><![CDATA[Diego]]></given-names>
</name>
<xref ref-type="aff" rid="Aff"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Correa Gallego]]></surname>
<given-names><![CDATA[Hernando]]></given-names>
</name>
<xref ref-type="aff" rid="Aff"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Salcedo-Reyes]]></surname>
<given-names><![CDATA[Juan Carlos]]></given-names>
</name>
</contrib>
</contrib-group>
<aff id="Af1">
<institution><![CDATA[,Pontificia Universidad Javeriana  ]]></institution>
<addr-line><![CDATA[Cali ]]></addr-line>
<country>Colombia</country>
</aff>
<aff id="Af2">
<institution><![CDATA[,Universidad del Valle  ]]></institution>
<addr-line><![CDATA[Cali ]]></addr-line>
<country>Colombia</country>
</aff>
<aff id="Af3">
<institution><![CDATA[,Universidad del Quindío  ]]></institution>
<addr-line><![CDATA[Armenia ]]></addr-line>
<country>Colombia</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>08</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>08</month>
<year>2017</year>
</pub-date>
<volume>22</volume>
<numero>2</numero>
<fpage>113</fpage>
<lpage>121</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S0122-74832017000200113&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S0122-74832017000200113&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S0122-74832017000200113&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[Abstract Impedance spectroscopy measurements of the LiI-4AgI samples, in the frequency range 20 Hz-1 MHz, and in the temperature range between 353 K and 378 K were made. Both pure and lithium-doped silver iodide showed blocking phenomena in the electrodes and the grain boundary. The blocking phenomena allowed a change in the transport properties of the pure compound in respect to the doped compound as the temperature varied. The curves of electrical modulus in the LiI-4AgI system show asymmetric peaks corresponding with a weak correlation between mobile ions in the diffusion process. The electrical conductivity in the Agl-Lil system can be described using a stretched relaxation function of the Kohlrausch-Williams-Watts (KWW) type. We speculat e that the phase of lithium dissolved in the silver iodide favors the formation of islands that disperses the conductivity due to the modification of the relationship among the microscopic energies: microscopic energy and migration energy.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[Resumen Se tomaron medidas de espectroscopia de impedancia de muestras de Lil-4Agl en el rango de frecuencia de 20 Hz-1 MHz y en el rango de temperatura entre 353 K y 378 K. Tanto el litio puro como el litio dopado con ioduro de plata mostraron fenómenos de bloqueo en los electrodos y la frontera de grano. Los fenómenos de bloqueo permitieron un cambio en las propiedades de transporte del compuesto puro respecto del compuesto dopado a medida que variaba la temperatura. Las curvas del módulo eléctrico en el sistema LiI-4AgI muestran picos asimétricos correspondientes a una débil correlación entre iones móviles en el proceso de difusión. La conductividad eléctrica en el sistema Agl-Lil se puede describir usando una normalización de la función de relajación del tipo Kohlrausch-Williams-Watts (KWW). Especulamos que la fase de litio disuelto en ioduro de plata favorece la formación de islas que dispersan la conductividad debido a la modificación de la relación entre las energías microscopias: energía microscópica y energía de migración.]]></p></abstract>
<abstract abstract-type="short" xml:lang="pt"><p><![CDATA[Resumo Foram realizadas medidas de espectroscopia de impedancia de amostras de Lil-4Agl na faixa de frequência de 20 Hz - 1 MHz e na faixa de temperatura entre 353 e 378 K. Tanto o litio puro como o litio contaminado com iodeto de prata mostram fenômenos de bloqueio nos eletrodos e nos limites do grão. Os fenômenos de bloqueio permitiram uma mudança nas propriedades de transporte do composto puro em respeito ao composto contaminado, à medida que se variava a temperatura. As curvas do módulo elétrico no sistema Lil-4Agl mostraram picos assimétricos correspondentes a uma correlação débil entre ions móveis no processo de difusão. A condutividade elétrica no sistema AgI-Lil pode ser descrita utilizando uma normalização da função de relaxação do tipo Kohlrausch- Williams-Watts (KWW). Especulamos que a fase de litio dissolvida em iodeto de prata favorece a formação de ilhas que dispersam a condutividade devido a modificação da relação entre as energias microscópicas: energia microscópica e energia de migração.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Electrical modulus]]></kwd>
<kwd lng="en"><![CDATA[Ionic conductivity]]></kwd>
<kwd lng="en"><![CDATA[Silver iodide]]></kwd>
<kwd lng="en"><![CDATA[Lithium iodide]]></kwd>
<kwd lng="en"><![CDATA[KWW function.]]></kwd>
<kwd lng="es"><![CDATA[módulos eléctricos]]></kwd>
<kwd lng="es"><![CDATA[conductividad iónica]]></kwd>
<kwd lng="es"><![CDATA[ioduro de plata]]></kwd>
<kwd lng="es"><![CDATA[ioduro de litio]]></kwd>
<kwd lng="es"><![CDATA[función KWW.]]></kwd>
<kwd lng="pt"><![CDATA[módulos elétricos]]></kwd>
<kwd lng="pt"><![CDATA[condutividade iónica]]></kwd>
<kwd lng="pt"><![CDATA[iodeto de prata]]></kwd>
<kwd lng="pt"><![CDATA[iodeto de litio]]></kwd>
<kwd lng="pt"><![CDATA[função KWW.]]></kwd>
</kwd-group>
</article-meta>
</front><back>
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