NickelMaghrebV1, France, Analysis, bibRecord, 000085

Elastic anomalies in BaFe2-xNixAs2 crystals

Identifieur interne : 000085 ( France/Analysis ); précédent : 000084; suivant : 000086

Elastic anomalies in BaFe2-xNixAs2 crystals

Auteurs : M. Saint-Paul [France] ; A. Abbassi [Maroc] ; Zhao-Sheng Wang [France, République populaire de Chine] ; HUINQIAN LUO [République populaire de Chine] ; XINGYE LU [République populaire de Chine] ; CONG REN [République populaire de Chine] ; Hai-Hu Wen [République populaire de Chine] ; K. Hasselbach [France]

Source :

Physica. C. Superconductivity [ 0921-4534 ] ; 2012.

RBID : Pascal:13-0096621

Descripteurs français

Pascal (Inist)
- Anomalie, Méthode ultrasonore, Constante élasticité, Transformation phase, Haute température, Célérité son, Atténuation onde acoustique, Transition supraconductrice, Bande interdite supraconductrice, Chaleur massique, Concentration impureté, Addition nickel, Dopage, Supraconducteur, Pnicture, Baryum Fer Arséniure Mixte, Supraconducteur à base de fer, Arséniure à base de fer.
Wicri :
- topic : Dopage.

English descriptors

KwdEn :
- Acoustical wave attenuation, Anomaly, Barium Iron Arsenides Mixed, Doping, Elastic constants, High temperature, Impurity density, Iron based arsenide, Iron based superconductors, Nickel additions, Phase transformations, Pnictides, Sound velocity, Specific heat, Superconducting energy gap, Superconducting transitions, Superconductors, Ultrasonic method.

Abstract

We present ultrasonic measurements on superconducting BaFe_2-xNi_xAs₂ crystals with x=0.07 and x = 0.15. The elastic constants C₃₃ and C₄₄ for the underdoped crystal (x = 0.07) show a large softening related to the structural phase transition at high temperatures. Anomalies in the sound velocity and the ultrasonic attenuation have been found at the superconducting phase transition T_c = 17 K. Ultrasonic attenuation exhibits a peak at the superconducting transition in contrast with the attenuation in conventional superconductors. In the overdoped crystal (x = 0.15) a minimum of C₆₆ is found at a temperature just above the superconducting temperature T_c = 13 K. Superconducting energy gap values have been tentatively extracted from the longitudinal ultrasonic attenuation. Unconventional behaviour of the ultrasonic attenuation is observed in the superconducting BaFe_2-xNi_xAs₂ crystals.

Affiliations:

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Pascal:13-0096621

Le document en format XML

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As<sub>2</sub>
 crystals</title>
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<author><name sortKey="Cong Ren" sort="Cong Ren" uniqKey="Cong Ren" last="Cong Ren">CONG REN</name>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Elastic anomalies in BaFe<sub>2-x</sub>
Ni<sub>x</sub>
As<sub>2</sub>
 crystals</title>
<author><name sortKey="Saint Paul, M" sort="Saint Paul, M" uniqKey="Saint Paul M" first="M." last="Saint-Paul">M. Saint-Paul</name>
<affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Institut Néel, CNRS et Université Joseph Fourier BP 166</s1>
<s2>38042 Grenoble</s2>
<s3>FRA</s3>
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<author><name sortKey="Abbassi, A" sort="Abbassi, A" uniqKey="Abbassi A" first="A." last="Abbassi">A. Abbassi</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Faculté des Sciences et Techniques de Tanger, BP 416 Tanger, Universite Abdelmalek Essaâdi</s1>
<s3>MAR</s3>
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<country>Maroc</country>
<wicri:noRegion>Faculté des Sciences et Techniques de Tanger, BP 416 Tanger, Universite Abdelmalek Essaâdi</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Wang, Zhao Sheng" sort="Wang, Zhao Sheng" uniqKey="Wang Z" first="Zhao-Sheng" last="Wang">Zhao-Sheng Wang</name>
<affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Institut Néel, CNRS et Université Joseph Fourier BP 166</s1>
<s2>38042 Grenoble</s2>
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<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
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</placeName>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, PO Box 603</s1>
<s2>Beijing 100190</s2>
<s3>CHN</s3>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
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</inist:fA14>
<country>République populaire de Chine</country>
<placeName><settlement type="city">Pékin</settlement>
</placeName>
</affiliation>
</author>
<author><name sortKey="Huinqian Luo" sort="Huinqian Luo" uniqKey="Huinqian Luo" last="Huinqian Luo">HUINQIAN LUO</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, PO Box 603</s1>
<s2>Beijing 100190</s2>
<s3>CHN</s3>
<sZ>3 aut.</sZ>
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<country>République populaire de Chine</country>
<placeName><settlement type="city">Pékin</settlement>
</placeName>
</affiliation>
</author>
<author><name sortKey="Xingye Lu" sort="Xingye Lu" uniqKey="Xingye Lu" last="Xingye Lu">XINGYE LU</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, PO Box 603</s1>
<s2>Beijing 100190</s2>
<s3>CHN</s3>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
<placeName><settlement type="city">Pékin</settlement>
</placeName>
</affiliation>
</author>
<author><name sortKey="Cong Ren" sort="Cong Ren" uniqKey="Cong Ren" last="Cong Ren">CONG REN</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, PO Box 603</s1>
<s2>Beijing 100190</s2>
<s3>CHN</s3>
<sZ>3 aut.</sZ>
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<placeName><settlement type="city">Pékin</settlement>
</placeName>
</affiliation>
</author>
<author><name sortKey="Wen, Hai Hu" sort="Wen, Hai Hu" uniqKey="Wen H" first="Hai-Hu" last="Wen">Hai-Hu Wen</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, PO Box 603</s1>
<s2>Beijing 100190</s2>
<s3>CHN</s3>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
<placeName><settlement type="city">Pékin</settlement>
</placeName>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="04"><s1>National Laboratory for Solid State Microstuctures, Department of Physics, Nanjing University</s1>
<s2>210093 Nanjing</s2>
<s3>CHN</s3>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
<wicri:noRegion>210093 Nanjing</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Hasselbach, K" sort="Hasselbach, K" uniqKey="Hasselbach K" first="K." last="Hasselbach">K. Hasselbach</name>
<affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Institut Néel, CNRS et Université Joseph Fourier BP 166</s1>
<s2>38042 Grenoble</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>8 aut.</sZ>
</inist:fA14>
<country>France</country>
<placeName><region type="region" nuts="2">Auvergne-Rhône-Alpes</region>
<region type="old region" nuts="2">Rhône-Alpes</region>
<settlement type="city">Grenoble</settlement>
</placeName>
</affiliation>
</author>
</analytic>
<series><title level="j" type="main">Physica. C. Superconductivity</title>
<title level="j" type="abbreviated">Phys., C Supercond.</title>
<idno type="ISSN">0921-4534</idno>
<imprint><date when="2012">2012</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Physica. C. Superconductivity</title>
<title level="j" type="abbreviated">Phys., C Supercond.</title>
<idno type="ISSN">0921-4534</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Acoustical wave attenuation</term>
<term>Anomaly</term>
<term>Barium Iron Arsenides Mixed</term>
<term>Doping</term>
<term>Elastic constants</term>
<term>High temperature</term>
<term>Impurity density</term>
<term>Iron based arsenide</term>
<term>Iron based superconductors</term>
<term>Nickel additions</term>
<term>Phase transformations</term>
<term>Pnictides</term>
<term>Sound velocity</term>
<term>Specific heat</term>
<term>Superconducting energy gap</term>
<term>Superconducting transitions</term>
<term>Superconductors</term>
<term>Ultrasonic method</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Anomalie</term>
<term>Méthode ultrasonore</term>
<term>Constante élasticité</term>
<term>Transformation phase</term>
<term>Haute température</term>
<term>Célérité son</term>
<term>Atténuation onde acoustique</term>
<term>Transition supraconductrice</term>
<term>Bande interdite supraconductrice</term>
<term>Chaleur massique</term>
<term>Concentration impureté</term>
<term>Addition nickel</term>
<term>Dopage</term>
<term>Supraconducteur</term>
<term>Pnicture</term>
<term>Baryum Fer Arséniure Mixte</term>
<term>Supraconducteur à base de fer</term>
<term>Arséniure à base de fer</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Dopage</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">We present ultrasonic measurements on superconducting BaFe<sub>2-x</sub>
Ni<sub>x</sub>
As<sub>2</sub>
 crystals with x=0.07 and x = 0.15. The elastic constants C<sub>33</sub>
 and C<sub>44</sub>
 for the underdoped crystal (x = 0.07) show a large softening related to the structural phase transition at high temperatures. Anomalies in the sound velocity and the ultrasonic attenuation have been found at the superconducting phase transition T<sub>c</sub>
 = 17 K. Ultrasonic attenuation exhibits a peak at the superconducting transition in contrast with the attenuation in conventional superconductors. In the overdoped crystal (x = 0.15) a minimum of C<sub>66</sub>
 is found at a temperature just above the superconducting temperature T<sub>c</sub>
 = 13 K. Superconducting energy gap values have been tentatively extracted from the longitudinal ultrasonic attenuation. Unconventional behaviour of the ultrasonic attenuation is observed in the superconducting BaFe<sub>2-x</sub>
Ni<sub>x</sub>
As<sub>2</sub>
 crystals.</div>
</front>
</TEI>
<affiliations><list><country><li>France</li>
<li>Maroc</li>
<li>République populaire de Chine</li>
</country>
<region><li>Auvergne-Rhône-Alpes</li>
<li>Rhône-Alpes</li>
</region>
<settlement><li>Grenoble</li>
<li>Pékin</li>
</settlement>
</list>
<tree><country name="France"><region name="Auvergne-Rhône-Alpes"><name sortKey="Saint Paul, M" sort="Saint Paul, M" uniqKey="Saint Paul M" first="M." last="Saint-Paul">M. Saint-Paul</name>
</region>
<name sortKey="Hasselbach, K" sort="Hasselbach, K" uniqKey="Hasselbach K" first="K." last="Hasselbach">K. Hasselbach</name>
<name sortKey="Wang, Zhao Sheng" sort="Wang, Zhao Sheng" uniqKey="Wang Z" first="Zhao-Sheng" last="Wang">Zhao-Sheng Wang</name>
</country>
<country name="Maroc"><noRegion><name sortKey="Abbassi, A" sort="Abbassi, A" uniqKey="Abbassi A" first="A." last="Abbassi">A. Abbassi</name>
</noRegion>
</country>
<country name="République populaire de Chine"><noRegion><name sortKey="Wang, Zhao Sheng" sort="Wang, Zhao Sheng" uniqKey="Wang Z" first="Zhao-Sheng" last="Wang">Zhao-Sheng Wang</name>
</noRegion>
<name sortKey="Cong Ren" sort="Cong Ren" uniqKey="Cong Ren" last="Cong Ren">CONG REN</name>
<name sortKey="Huinqian Luo" sort="Huinqian Luo" uniqKey="Huinqian Luo" last="Huinqian Luo">HUINQIAN LUO</name>
<name sortKey="Wen, Hai Hu" sort="Wen, Hai Hu" uniqKey="Wen H" first="Hai-Hu" last="Wen">Hai-Hu Wen</name>
<name sortKey="Wen, Hai Hu" sort="Wen, Hai Hu" uniqKey="Wen H" first="Hai-Hu" last="Wen">Hai-Hu Wen</name>
<name sortKey="Xingye Lu" sort="Xingye Lu" uniqKey="Xingye Lu" last="Xingye Lu">XINGYE LU</name>
</country>
</tree>
</affiliations>
</record>

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Elastic anomalies in BaFe2-xNixAs2 crystals

Elastic anomalies in BaFe2-xNixAs2 crystals

Source :

Descripteurs français

English descriptors

Abstract

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