<p>This study presents an analysis of the dielectric and thermal properties in the vicinity of the second-order ferroelectric phase transition, with a specific emphasis on lithium-sodium tetragermanate, LiNaGe<sub>4</sub>O<sub>9</sub>. The power-law equation is employed by modifying the Kouvel-Fisher (KF) technique, which articulates the magnetization (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:M\)</EquationSource> </InlineEquation>) and magnetic susceptibility <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:\left({\chi\:}_{M}\right)\)</EquationSource> </InlineEquation> in relation to the spontaneous polarization (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:{P}_{S}\)</EquationSource> </InlineEquation>) and the dielectric constant (<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon\)</EquationSource> </InlineEquation>) within ferroelectric frameworks. A parallel methodology is adopted to elucidate the heat capacity (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:{C}_{P}\)</EquationSource> </InlineEquation>) and thermal expansivity (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:{\propto\:}_{P}\)</EquationSource> </InlineEquation>) in the vicinity of phase transitions occurring in LiNaGe<sub>4</sub>O<sub>9</sub>. We demonstrate that the continuous fluctuations in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:{P}_{S}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon\)</EquationSource> </InlineEquation> with temperature nearing the Curie point (T<sub>C</sub> <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq9.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:\sim\)</EquationSource> </InlineEquation>108&#xa0;K) as an indication of a second-order transition in LiNaGe<sub>4</sub>O<sub>9</sub>. Furthermore, a linear correlation is also established between <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:{C}_{P}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43994_2025_260_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(\:{\propto\:}_{P}\)</EquationSource> </InlineEquation> with temperature approaching the Curie point T<sub>C</sub> for this crystal structure. Experimental data are used from the literature for our analysis. Our findings show that the critical behavior of one dielectric or thermal property near the transition temperature in LiNaGe<sub>4</sub>O<sub>9</sub> can be predicted from the other through these linear relationships. The methodology articulated herein for delineating the dielectric and thermal characteristics of LiNaGe<sub>4</sub>O<sub>9</sub> close to the Curie point is extendable to various other ferroelectric materials.</p>

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Phenomenological study of lithium-sodium tetragermanate close to the phase transition

  • A. Kiraci

摘要

This study presents an analysis of the dielectric and thermal properties in the vicinity of the second-order ferroelectric phase transition, with a specific emphasis on lithium-sodium tetragermanate, LiNaGe4O9. The power-law equation is employed by modifying the Kouvel-Fisher (KF) technique, which articulates the magnetization ( \(\:M\) ) and magnetic susceptibility \(\:\left({\chi\:}_{M}\right)\) in relation to the spontaneous polarization ( \(\:{P}_{S}\) ) and the dielectric constant ( \(\epsilon\) ) within ferroelectric frameworks. A parallel methodology is adopted to elucidate the heat capacity ( \(\:{C}_{P}\) ) and thermal expansivity ( \(\:{\propto\:}_{P}\) ) in the vicinity of phase transitions occurring in LiNaGe4O9. We demonstrate that the continuous fluctuations in \(\:{P}_{S}\) and \(\epsilon\) with temperature nearing the Curie point (TC \(\:\sim\) 108 K) as an indication of a second-order transition in LiNaGe4O9. Furthermore, a linear correlation is also established between \(\:{C}_{P}\) and \(\:{\propto\:}_{P}\) with temperature approaching the Curie point TC for this crystal structure. Experimental data are used from the literature for our analysis. Our findings show that the critical behavior of one dielectric or thermal property near the transition temperature in LiNaGe4O9 can be predicted from the other through these linear relationships. The methodology articulated herein for delineating the dielectric and thermal characteristics of LiNaGe4O9 close to the Curie point is extendable to various other ferroelectric materials.