Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2

Recently Li et al. (2019 Nature 572 624) discovered a new type of oxide superconductor Nd0.8Sr0.2NiO2 with Tc = 14 K. To classify superconductivity in this infinite-layer nickelate experimental upper critical field, Bc2(T), and the self-field critical current densities, Jc(sf,T), reported by Li et a...

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Main Author: E.F. Talantsev
Format: Article
Language:English
Published: Elsevier 2020-06-01
Series:Results in Physics
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2211379720306057
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spelling doaj-bc57cb4ccc4547c195c44b3df9c6d2f72020-11-25T03:33:04ZengElsevierResults in Physics2211-37972020-06-0117103118Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2E.F. Talantsev0M.N. Mikheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, 18, S. Kovalevskoy St., Ekaterinburg 620108, Russia; NANOTECH Centre, Ural Federal University, 19 Mira St., Ekaterinburg 620002, Russia; Address: M.N. Mikheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, 18, S. Kovalevskoy St., Ekaterinburg 620108, Russia.Recently Li et al. (2019 Nature 572 624) discovered a new type of oxide superconductor Nd0.8Sr0.2NiO2 with Tc = 14 K. To classify superconductivity in this infinite-layer nickelate experimental upper critical field, Bc2(T), and the self-field critical current densities, Jc(sf,T), reported by Li et al. (2019 Nature 572 624), are analysed in assumption of s-, d-, and p-wave pairing symmetries and single- and multiple-band superconductivity. Based on deduced the ground-state superconducting energy gap, Δ(0), the London penetration depth, λ(0), the relative jump in electronic specific heat at Tc, ΔC/C, and the ratio of 2Δ(0)/kBTc, we conclude that Nd0.8Sr0.2NiO2 is type-II high-κ weak-coupled single-band s-wave superconductor.http://www.sciencedirect.com/science/article/pii/S2211379720306057SuperconductivityInfinite-layer nickelateUpper critical fieldSelf-field critical current densitySuperconducting energy gapLondon penetration depth
collection DOAJ
language English
format Article
sources DOAJ
author E.F. Talantsev
spellingShingle E.F. Talantsev
Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2
Results in Physics
Superconductivity
Infinite-layer nickelate
Upper critical field
Self-field critical current density
Superconducting energy gap
London penetration depth
author_facet E.F. Talantsev
author_sort E.F. Talantsev
title Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2
title_short Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2
title_full Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2
title_fullStr Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2
title_full_unstemmed Classifying superconductivity in an infinite-layer nickelate Nd0.8Sr0.2NiO2
title_sort classifying superconductivity in an infinite-layer nickelate nd0.8sr0.2nio2
publisher Elsevier
series Results in Physics
issn 2211-3797
publishDate 2020-06-01
description Recently Li et al. (2019 Nature 572 624) discovered a new type of oxide superconductor Nd0.8Sr0.2NiO2 with Tc = 14 K. To classify superconductivity in this infinite-layer nickelate experimental upper critical field, Bc2(T), and the self-field critical current densities, Jc(sf,T), reported by Li et al. (2019 Nature 572 624), are analysed in assumption of s-, d-, and p-wave pairing symmetries and single- and multiple-band superconductivity. Based on deduced the ground-state superconducting energy gap, Δ(0), the London penetration depth, λ(0), the relative jump in electronic specific heat at Tc, ΔC/C, and the ratio of 2Δ(0)/kBTc, we conclude that Nd0.8Sr0.2NiO2 is type-II high-κ weak-coupled single-band s-wave superconductor.
topic Superconductivity
Infinite-layer nickelate
Upper critical field
Self-field critical current density
Superconducting energy gap
London penetration depth
url http://www.sciencedirect.com/science/article/pii/S2211379720306057
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