Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe1.93Ni0.07As2 crystals
Identifieur interne : 000422 ( PascalFrancis/Curation ); précédent : 000421; suivant : 000423Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe1.93Ni0.07As2 crystals
Auteurs : M. Saint-Paul [France] ; C. Guttin [France] ; A. Abbassi [Maroc] ; Zhao-Sheng Wang [France, République populaire de Chine] ; HUIQIAN 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 :
- Solid state communications [ 0038-1098 ] ; 2014.
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- topic : Dopage.
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Abstract
Measurements of the real R and imaginary X parts of the surface impedance were performed in underdoped BaFe1.93Ni0.07 As2 crystals in the frequency range 10 MHz-1.5 GHz. The establishment of the antiferromagnetic order at TÑ50 K gives rise to anomalous increase of electron scattering time. Drude type conductivity yields X and R differ from each other. The increase of the real conductivity σ1 in the superconducting state is attributed to a rapid decrease of the quasiparticle scattering time. This result gives evidence of coexistence of superconductivity and antiferromagnetism.
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Ni<sub>0.07</sub>
As<sub>2</sub>
crystals</title>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe<sub>1.93</sub>
Ni<sub>0.07</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>
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<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, P.O. Box 603</s1>
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<sZ>8 aut.</sZ>
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<term>Barium Iron Arsenides Mixed</term>
<term>Doping</term>
<term>Drude model</term>
<term>Electron scattering</term>
<term>Impurities</term>
<term>Iron based superconductors</term>
<term>Microwave conductivity</term>
<term>Nickel additions</term>
<term>Pnictides</term>
<term>Quasiparticles</term>
<term>Superconductivity</term>
<term>Superconductors</term>
<term>Surface impedance</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Impédance surface</term>
<term>Antiferromagnétisme</term>
<term>Supraconductivité</term>
<term>Diffusion électron</term>
<term>Modèle Drude</term>
<term>Quasiparticule</term>
<term>Dopage</term>
<term>Conductivité hyperfréquence</term>
<term>Impureté</term>
<term>Addition nickel</term>
<term>Supraconducteur</term>
<term>Pnicture</term>
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<front><div type="abstract" xml:lang="en">Measurements of the real R and imaginary X parts of the surface impedance were performed in underdoped BaFe<sub>1.93</sub>
Ni<sub>0.07</sub>
As<sub>2</sub>
crystals in the frequency range 10 MHz-1.5 GHz. The establishment of the antiferromagnetic order at T<sub>Ñ</sub>
50 K gives rise to anomalous increase of electron scattering time. Drude type conductivity yields X and R differ from each other. The increase of the real conductivity σ<sub>1</sub>
in the superconducting state is attributed to a rapid decrease of the quasiparticle scattering time. This result gives evidence of coexistence of superconductivity and antiferromagnetism.</div>
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Ni<sub>0.07</sub>
As<sub>2</sub>
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<sZ>3 aut.</sZ>
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<fA14 i1="03"><s1>Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603</s1>
<s2>Beijing 100190</s2>
<s3>CHN</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
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<fA14 i1="04"><s1>National Laboratory for Solid State Microstuctures, Departement of Physics, Nanjing University</s1>
<s2>210093 Nanjing</s2>
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<fC01 i1="01" l="ENG"><s0>Measurements of the real R and imaginary X parts of the surface impedance were performed in underdoped BaFe<sub>1.93</sub>
Ni<sub>0.07</sub>
As<sub>2</sub>
crystals in the frequency range 10 MHz-1.5 GHz. The establishment of the antiferromagnetic order at T<sub>Ñ</sub>
50 K gives rise to anomalous increase of electron scattering time. Drude type conductivity yields X and R differ from each other. The increase of the real conductivity σ<sub>1</sub>
in the superconducting state is attributed to a rapid decrease of the quasiparticle scattering time. This result gives evidence of coexistence of superconductivity and antiferromagnetism.</s0>
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<fC03 i1="06" i2="3" l="FRE"><s0>Quasiparticule</s0>
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<fC03 i1="06" i2="3" l="ENG"><s0>Quasiparticles</s0>
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<fC03 i1="07" i2="X" l="FRE"><s0>Dopage</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Doping</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Doping</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Conductivité hyperfréquence</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Microwave conductivity</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Conductividad hiperfrecuencia</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Impureté</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Impurities</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Addition nickel</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Nickel additions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Supraconducteur</s0>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Superconductors</s0>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Pnicture</s0>
<s2>NA</s2>
<s5>16</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Pnictides</s0>
<s2>NA</s2>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Baryum Fer Arséniure Mixte</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>17</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Barium Iron Arsenides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>17</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Mixto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>17</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Supraconducteur à base de fer</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Iron based superconductors</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>244</s1>
</fN21>
</pA>
</standard>
</inist>
</record>
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