NickelMaghrebV1, PascalFrancis, Corpus, bibRecord, 000019

Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe1.93Ni0.07As2 crystals

Identifieur interne : 000019 ( PascalFrancis/Corpus ); précédent : 000018; suivant : 000020

Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe1.93Ni0.07As2 crystals

Auteurs : M. Saint-Paul ; C. Guttin ; A. Abbassi ; Zhao-Sheng Wang ; HUIQIAN LUO ; XINGYE LU ; CONG REN ; Hai-Hu Wen ; K. Hasselbach

Source :

Solid state communications [ 0038-1098 ] ; 2014.

RBID : Pascal:14-0194445

Descripteurs français

Pascal (Inist)
- Impédance surface, Antiferromagnétisme, Supraconductivité, Diffusion électron, Modèle Drude, Quasiparticule, Dopage, Conductivité hyperfréquence, Impureté, Addition nickel, Supraconducteur, Pnicture, Baryum Fer Arséniure Mixte, Supraconducteur à base de fer.

English descriptors

KwdEn :
- Antiferromagnetism, Barium Iron Arsenides Mixed, Doping, Drude model, Electron scattering, Impurities, Iron based superconductors, Microwave conductivity, Nickel additions, Pnictides, Quasiparticles, Superconductivity, Superconductors, Surface impedance.

Abstract

Measurements of the real R and imaginary X parts of the surface impedance were performed in underdoped BaFe_1.93Ni_0.07 As₂ crystals in the frequency range 10 MHz-1.5 GHz. The establishment of the antiferromagnetic order at T_Ñ50 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.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 0038-1098`
A02	`01`			`@0 SSCOA4`
A03		`1`		`@0 Solid state commun.`
A05				`@2 192`
A08	`01`	`1`	`ENG`	`@1 Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe_1.93Ni_0.07As₂ crystals`
A11	`01`	`1`		`@1 SAINT-PAUL (M.)`
A11	`02`	`1`		`@1 GUTTIN (C.)`
A11	`03`	`1`		`@1 ABBASSI (A.)`
A11	`04`	`1`		`@1 WANG (Zhao-Sheng)`
A11	`05`	`1`		`@1 HUIQIAN LUO`
A11	`06`	`1`		`@1 XINGYE LU`
A11	`07`	`1`		`@1 CONG REN`
A11	`08`	`1`		`@1 WEN (Hai-Hu)`
A11	`09`	`1`		`@1 HASSELBACH (K.)`
A14	`01`			`@1 Université Grenoble, CNRS, Institut Néel 166 @2 38042 Grenoble @3 FRA @Z 1 aut. @Z 2 aut. @Z 4 aut. @Z 9 aut.`
A14	`02`			`@1 Faculté des Sciences et Techniques de Tanger, BP 416 Tanger, Université Abdelmalek Essaâdi @3 MAR @Z 3 aut.`
A14	`03`			`@1 Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603 @2 Beijing 100190 @3 CHN @Z 4 aut. @Z 5 aut. @Z 6 aut. @Z 7 aut. @Z 8 aut.`
A14	`04`			`@1 National Laboratory for Solid State Microstuctures, Departement of Physics, Nanjing University @2 210093 Nanjing @3 CHN @Z 8 aut.`
A20				`@1 47-50`
A21				`@1 2014`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 10917 @5 354000150323120110`
A44				`@0 0000 @1 © 2014 INIST-CNRS. All rights reserved.`
A45				`@0 15 ref.`
A47	`01`	`1`		`@0 14-0194445`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Solid state communications`
A66	`01`			`@0 GBR`
C01	`01`		`ENG`	@0 Measurements of the real R and imaginary X parts of the surface impedance were performed in underdoped BaFe_1.93Ni_0.07 As₂ crystals in the frequency range 10 MHz-1.5 GHz. The establishment of the antiferromagnetic order at T_Ñ50 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.
C02	`01`	`3`		`@0 001B70D25N`
C03	`01`	`3`	`FRE`	`@0 Impédance surface @5 02`
C03	`01`	`3`	`ENG`	`@0 Surface impedance @5 02`
C03	`02`	`3`	`FRE`	`@0 Antiferromagnétisme @5 03`
C03	`02`	`3`	`ENG`	`@0 Antiferromagnetism @5 03`
C03	`03`	`3`	`FRE`	`@0 Supraconductivité @5 04`
C03	`03`	`3`	`ENG`	`@0 Superconductivity @5 04`
C03	`04`	`X`	`FRE`	`@0 Diffusion électron @5 05`
C03	`04`	`X`	`ENG`	`@0 Electron scattering @5 05`
C03	`04`	`X`	`SPA`	`@0 Difusión electrón @5 05`
C03	`05`	`3`	`FRE`	`@0 Modèle Drude @5 06`
C03	`05`	`3`	`ENG`	`@0 Drude model @5 06`
C03	`06`	`3`	`FRE`	`@0 Quasiparticule @5 07`
C03	`06`	`3`	`ENG`	`@0 Quasiparticles @5 07`
C03	`07`	`X`	`FRE`	`@0 Dopage @5 08`
C03	`07`	`X`	`ENG`	`@0 Doping @5 08`
C03	`07`	`X`	`SPA`	`@0 Doping @5 08`
C03	`08`	`X`	`FRE`	`@0 Conductivité hyperfréquence @5 09`
C03	`08`	`X`	`ENG`	`@0 Microwave conductivity @5 09`
C03	`08`	`X`	`SPA`	`@0 Conductividad hiperfrecuencia @5 09`
C03	`09`	`3`	`FRE`	`@0 Impureté @5 10`
C03	`09`	`3`	`ENG`	`@0 Impurities @5 10`
C03	`10`	`3`	`FRE`	`@0 Addition nickel @5 11`
C03	`10`	`3`	`ENG`	`@0 Nickel additions @5 11`
C03	`11`	`3`	`FRE`	`@0 Supraconducteur @5 15`
C03	`11`	`3`	`ENG`	`@0 Superconductors @5 15`
C03	`12`	`3`	`FRE`	`@0 Pnicture @2 NA @5 16`
C03	`12`	`3`	`ENG`	`@0 Pnictides @2 NA @5 16`
C03	`13`	`X`	`FRE`	`@0 Baryum Fer Arséniure Mixte @2 NC @2 NA @5 17`
C03	`13`	`X`	`ENG`	`@0 Barium Iron Arsenides Mixed @2 NC @2 NA @5 17`
C03	`13`	`X`	`SPA`	`@0 Mixto @2 NC @2 NA @5 17`
C03	`14`	`3`	`FRE`	`@0 Supraconducteur à base de fer @4 CD @5 96`
C03	`14`	`3`	`ENG`	`@0 Iron based superconductors @4 CD @5 96`
N21				`@1 244`

Format Inist (serveur)

NO :	PASCAL 14-0194445 INIST
ET :	Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe_1.93Ni_0.07As₂ crystals
AU :	SAINT-PAUL (M.); GUTTIN (C.); ABBASSI (A.); WANG (Zhao-Sheng); HUIQIAN LUO; XINGYE LU; CONG REN; WEN (Hai-Hu); HASSELBACH (K.)
AF :	Université Grenoble, CNRS, Institut Néel 166/38042 Grenoble/France (1 aut., 2 aut., 4 aut., 9 aut.); Faculté des Sciences et Techniques de Tanger, BP 416 Tanger, Université Abdelmalek Essaâdi/Maroc (3 aut.); Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603/Beijing 100190/Chine (4 aut., 5 aut., 6 aut., 7 aut., 8 aut.); National Laboratory for Solid State Microstuctures, Departement of Physics, Nanjing University/210093 Nanjing/Chine (8 aut.)
DT :	Publication en série; Niveau analytique
SO :	Solid state communications; ISSN 0038-1098; Coden SSCOA4; Royaume-Uni; Da. 2014; Vol. 192; Pp. 47-50; Bibl. 15 ref.
LA :	Anglais
EA :	Measurements of the real R and imaginary X parts of the surface impedance were performed in underdoped BaFe_1.93Ni_0.07 As₂ crystals in the frequency range 10 MHz-1.5 GHz. The establishment of the antiferromagnetic order at T_Ñ50 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.
CC :	001B70D25N
FD :	Impédance surface; Antiferromagnétisme; Supraconductivité; Diffusion électron; Modèle Drude; Quasiparticule; Dopage; Conductivité hyperfréquence; Impureté; Addition nickel; Supraconducteur; Pnicture; Baryum Fer Arséniure Mixte; Supraconducteur à base de fer
ED :	Surface impedance; Antiferromagnetism; Superconductivity; Electron scattering; Drude model; Quasiparticles; Doping; Microwave conductivity; Impurities; Nickel additions; Superconductors; Pnictides; Barium Iron Arsenides Mixed; Iron based superconductors
SD :	Difusión electrón; Doping; Conductividad hiperfrecuencia; Mixto
LO :	INIST-10917.354000150323120110
ID :	14-0194445

Links to Exploration step

Pascal:14-0194445

Le document en format XML

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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="Wang, Zhao Sheng" sort="Wang, Zhao Sheng" uniqKey="Wang Z" first="Zhao-Sheng" last="Wang">Zhao-Sheng Wang</name>
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<author><name sortKey="Huiqian Luo" sort="Huiqian Luo" uniqKey="Huiqian Luo" last="Huiqian Luo">HUIQIAN LUO</name>
<affiliation><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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<author><name sortKey="Cong Ren" sort="Cong Ren" uniqKey="Cong Ren" last="Cong Ren">CONG REN</name>
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<affiliation><inist:fA14 i1="04"><s1>National Laboratory for Solid State Microstuctures, Departement of Physics, Nanjing University</s1>
<s2>210093 Nanjing</s2>
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<sZ>8 aut.</sZ>
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<author><name sortKey="Hasselbach, K" sort="Hasselbach, K" uniqKey="Hasselbach K" first="K." last="Hasselbach">K. Hasselbach</name>
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<series><title level="j" type="main">Solid state communications</title>
<title level="j" type="abbreviated">Solid state commun.</title>
<idno type="ISSN">0038-1098</idno>
<imprint><date when="2014">2014</date>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Antiferromagnetism</term>
<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>
<term>Baryum Fer Arséniure Mixte</term>
<term>Supraconducteur à base de fer</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>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0038-1098</s0>
</fA01>
<fA02 i1="01"><s0>SSCOA4</s0>
</fA02>
<fA03 i2="1"><s0>Solid state commun.</s0>
</fA03>
<fA05><s2>192</s2>
</fA05>
<fA08 i1="01" i2="1" l="ENG"><s1>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</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>SAINT-PAUL (M.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>GUTTIN (C.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>ABBASSI (A.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>WANG (Zhao-Sheng)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>HUIQIAN LUO</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>XINGYE LU</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>CONG REN</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>WEN (Hai-Hu)</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>HASSELBACH (K.)</s1>
</fA11>
<fA14 i1="01"><s1>Université Grenoble, CNRS, Institut Néel 166</s1>
<s2>38042 Grenoble</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Faculté des Sciences et Techniques de Tanger, BP 416 Tanger, Université Abdelmalek Essaâdi</s1>
<s3>MAR</s3>
<sZ>3 aut.</sZ>
</fA14>
<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>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>National Laboratory for Solid State Microstuctures, Departement of Physics, Nanjing University</s1>
<s2>210093 Nanjing</s2>
<s3>CHN</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA20><s1>47-50</s1>
</fA20>
<fA21><s1>2014</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>10917</s2>
<s5>354000150323120110</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2014 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>15 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>14-0194445</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Solid state communications</s0>
</fA64>
<fA66 i1="01"><s0>GBR</s0>
</fA66>
<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>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70D25N</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Impédance surface</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Surface impedance</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Antiferromagnétisme</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Antiferromagnetism</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Supraconductivité</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Superconductivity</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Diffusion électron</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Electron scattering</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Difusión electrón</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Modèle Drude</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Drude model</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Quasiparticule</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Quasiparticles</s0>
<s5>07</s5>
</fC03>
<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>
<server><NO>PASCAL 14-0194445 INIST</NO>
<ET>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</ET>
<AU>SAINT-PAUL (M.); GUTTIN (C.); ABBASSI (A.); WANG (Zhao-Sheng); HUIQIAN LUO; XINGYE LU; CONG REN; WEN (Hai-Hu); HASSELBACH (K.)</AU>
<AF>Université Grenoble, CNRS, Institut Néel 166/38042 Grenoble/France (1 aut., 2 aut., 4 aut., 9 aut.); Faculté des Sciences et Techniques de Tanger, BP 416 Tanger, Université Abdelmalek Essaâdi/Maroc (3 aut.); Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603/Beijing 100190/Chine (4 aut., 5 aut., 6 aut., 7 aut., 8 aut.); National Laboratory for Solid State Microstuctures, Departement of Physics, Nanjing University/210093 Nanjing/Chine (8 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Solid state communications; ISSN 0038-1098; Coden SSCOA4; Royaume-Uni; Da. 2014; Vol. 192; Pp. 47-50; Bibl. 15 ref.</SO>
<LA>Anglais</LA>
<EA>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.</EA>
<CC>001B70D25N</CC>
<FD>Impédance surface; Antiferromagnétisme; Supraconductivité; Diffusion électron; Modèle Drude; Quasiparticule; Dopage; Conductivité hyperfréquence; Impureté; Addition nickel; Supraconducteur; Pnicture; Baryum Fer Arséniure Mixte; Supraconducteur à base de fer</FD>
<ED>Surface impedance; Antiferromagnetism; Superconductivity; Electron scattering; Drude model; Quasiparticles; Doping; Microwave conductivity; Impurities; Nickel additions; Superconductors; Pnictides; Barium Iron Arsenides Mixed; Iron based superconductors</ED>
<SD>Difusión electrón; Doping; Conductividad hiperfrecuencia; Mixto</SD>
<LO>INIST-10917.354000150323120110</LO>
<ID>14-0194445</ID>
</server>
</inist>
</record>

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	Serveur d'exploration sur le nickel au Maghreb
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Serveur d'exploration sur le nickel au Maghreb

Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe1.93Ni0.07As2 crystals

Surface impedance in the antiferromagnetic and superconducting states of underdoped BaFe1.93Ni0.07As2 crystals

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