<i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor

We report the finding of a novel pairing state in a newly discovered superconductor Na<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semant...

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Main Authors: Amitava Bhattacharyya, Devashibhai Adroja, Yu Feng, Debarchan Das, Pabitra Kumar Biswas, Tanmoy Das, Jun Zhao
Format: Article
Language:English
Published: MDPI AG 2023-02-01
Series:Magnetochemistry
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Online Access:https://www.mdpi.com/2312-7481/9/3/70
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author Amitava Bhattacharyya
Devashibhai Adroja
Yu Feng
Debarchan Das
Pabitra Kumar Biswas
Tanmoy Das
Jun Zhao
author_facet Amitava Bhattacharyya
Devashibhai Adroja
Yu Feng
Debarchan Das
Pabitra Kumar Biswas
Tanmoy Das
Jun Zhao
author_sort Amitava Bhattacharyya
collection DOAJ
description We report the finding of a novel pairing state in a newly discovered superconductor Na<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Cr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>As<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>. This material has a non-centrosymmetric quasi-one-dimensional crystal structure and is superconducting at <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>T</mi><mi mathvariant="normal">C</mi></msub><mo>∼</mo></mrow></semantics></math></inline-formula> 8.0 K. We find that the magnetic penetration depth data suggests the presence of a nodal line <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>p</mi><mi>z</mi></msub></semantics></math></inline-formula>-wave pairing state with zero magnetic moment using transverse-field muon-spin rotation (TF-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>μ</mi></semantics></math></inline-formula>SR) measurements. The nodal gap observed in Na<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Cr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>As<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> compound is consistent with that observed in isostructural (K,Cs)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Cr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>As<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> compounds using TF-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>μ</mi></semantics></math></inline-formula>SR measurements. The observed pairing state is consistent with a three-band model spin-fluctuation calculation, which reveals the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>S</mi><mi>z</mi></msub><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula> spin-triplet pairing state with the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo form="prefix">sin</mo><msub><mi>k</mi><mi>z</mi></msub></mrow></semantics></math></inline-formula> pairing symmetry. The long-sought search for chiral superconductivity with topological applications could be aided by such a novel triplet <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>S</mi><mi>z</mi></msub><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula><i>p</i>-wave pairing state.
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spelling doaj.art-b6601fc72cee48b5af06bfc74069194c2023-11-17T12:16:30ZengMDPI AGMagnetochemistry2312-74812023-02-01937010.3390/magnetochemistry9030070<i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> SuperconductorAmitava Bhattacharyya0Devashibhai Adroja1Yu Feng2Debarchan Das3Pabitra Kumar Biswas4Tanmoy Das5Jun Zhao6Department of Physics, Ramakrishna Mission Vivekananda Educational and Research Institute, Belur Math, Howrah 711202, IndiaISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire OX11 0QX, UKState Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, ChinaLaboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, SwitzerlandISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire OX11 0QX, UKDepartment of Physics, Indian Institute of Science, Bangalore 560012, IndiaState Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, ChinaWe report the finding of a novel pairing state in a newly discovered superconductor Na<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Cr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>As<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>. This material has a non-centrosymmetric quasi-one-dimensional crystal structure and is superconducting at <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>T</mi><mi mathvariant="normal">C</mi></msub><mo>∼</mo></mrow></semantics></math></inline-formula> 8.0 K. We find that the magnetic penetration depth data suggests the presence of a nodal line <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>p</mi><mi>z</mi></msub></semantics></math></inline-formula>-wave pairing state with zero magnetic moment using transverse-field muon-spin rotation (TF-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>μ</mi></semantics></math></inline-formula>SR) measurements. The nodal gap observed in Na<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Cr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>As<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> compound is consistent with that observed in isostructural (K,Cs)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Cr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>As<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> compounds using TF-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>μ</mi></semantics></math></inline-formula>SR measurements. The observed pairing state is consistent with a three-band model spin-fluctuation calculation, which reveals the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>S</mi><mi>z</mi></msub><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula> spin-triplet pairing state with the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo form="prefix">sin</mo><msub><mi>k</mi><mi>z</mi></msub></mrow></semantics></math></inline-formula> pairing symmetry. The long-sought search for chiral superconductivity with topological applications could be aided by such a novel triplet <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>S</mi><mi>z</mi></msub><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula><i>p</i>-wave pairing state.https://www.mdpi.com/2312-7481/9/3/70low dimensional systemssuperconducting gap structuremuon spin spectroscopy
spellingShingle Amitava Bhattacharyya
Devashibhai Adroja
Yu Feng
Debarchan Das
Pabitra Kumar Biswas
Tanmoy Das
Jun Zhao
<i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor
Magnetochemistry
low dimensional systems
superconducting gap structure
muon spin spectroscopy
title <i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor
title_full <i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor
title_fullStr <i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor
title_full_unstemmed <i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor
title_short <i>μ</i>SR Study of Unconventional Pairing Symmetry in the Quasi-1D Na<sub>2</sub>Cr<sub>3</sub>As<sub>3</sub> Superconductor
title_sort i μ i sr study of unconventional pairing symmetry in the quasi 1d na sub 2 sub cr sub 3 sub as sub 3 sub superconductor
topic low dimensional systems
superconducting gap structure
muon spin spectroscopy
url https://www.mdpi.com/2312-7481/9/3/70
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