Approaching the ultimate superconducting properties of (Ba,K)Fe2As2 by naturally formed low-angle grain boundary networks

The most effective way to enhance the dissipation-free supercurrent in the presence of a magnetic field for type II superconductors is to introduce defects that act as artificial pinning centers (APCs) for vortices. For instance, the in-field critical current density of doped BaFe 2 As 2 (Ba122), on...

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Veröffentlicht in:NPG Asia Materials 2021-10, Vol.13 (1), Article 68
Hauptverfasser: Iida, Kazumasa, Qin, Dongyi, Tarantini, Chiara, Hatano, Takafumi, Wang, Chao, Guo, Zimeng, Gao, Hongye, Saito, Hikaru, Hata, Satoshi, Naito, Michio, Yamamoto, Akiyasu
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creator Iida, Kazumasa
Qin, Dongyi
Tarantini, Chiara
Hatano, Takafumi
Wang, Chao
Guo, Zimeng
Gao, Hongye
Saito, Hikaru
Hata, Satoshi
Naito, Michio
Yamamoto, Akiyasu
description The most effective way to enhance the dissipation-free supercurrent in the presence of a magnetic field for type II superconductors is to introduce defects that act as artificial pinning centers (APCs) for vortices. For instance, the in-field critical current density of doped BaFe 2 As 2 (Ba122), one of the most technologically important Fe-based superconductors, has been improved over the last decade by APCs created by ion irradiation. The technique of ion irradiation has been commonly implemented to determine the ultimate superconducting properties. However, this method is rather complicated and expensive. Here, we report a surprisingly high critical current density and strong pinning efficiency close to the crystallographic c -axis for a K-doped Ba122 epitaxial thin film without APCs, achieving performance comparable to ion-irradiated K-doped Ba122 single crystals. Microstructural analysis reveals that the film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. This study demonstrates that the upper limit of in-field properties reached in ion-irradiated K-doped Ba122 is achievable by grain boundary engineering, which is a simple and industrially scalable manner. Superconductivity: Engineering crytal structure A way to optimize superconductivity by carefully controlling the atomic-level crystal structure has been developed by scientists in Japan and the USA. Superconductivity is a quantum effect, usually only seen at very low temperatures, in which an electrical current can pass through a material without facing any resistance. One approach to increasing the operating temperature is to intentionally introduce atomic-level defects using a technique called ion irradiation but this is technically complicated and expensive. Kazumasa Iida from Nagoya University, Japan, and co-workers have managed to achieve the levels of superconductivity associated with ion irradiation by using so-called grain boundary engineering. Regions of different crystalline orientation are known as grains. The team showed that by controlling the alignment of these grains during synthesis of the superconductor (Ba,K)Fe 2 As 2 , they could maximize the material’s superconductivity. High critical current density and strong pinning efficiency for Fe-based superconductor, K-doped BaFe 2 As 2 , were achieved by natural
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For instance, the in-field critical current density of doped BaFe 2 As 2 (Ba122), one of the most technologically important Fe-based superconductors, has been improved over the last decade by APCs created by ion irradiation. The technique of ion irradiation has been commonly implemented to determine the ultimate superconducting properties. However, this method is rather complicated and expensive. Here, we report a surprisingly high critical current density and strong pinning efficiency close to the crystallographic c -axis for a K-doped Ba122 epitaxial thin film without APCs, achieving performance comparable to ion-irradiated K-doped Ba122 single crystals. Microstructural analysis reveals that the film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. This study demonstrates that the upper limit of in-field properties reached in ion-irradiated K-doped Ba122 is achievable by grain boundary engineering, which is a simple and industrially scalable manner. Superconductivity: Engineering crytal structure A way to optimize superconductivity by carefully controlling the atomic-level crystal structure has been developed by scientists in Japan and the USA. Superconductivity is a quantum effect, usually only seen at very low temperatures, in which an electrical current can pass through a material without facing any resistance. One approach to increasing the operating temperature is to intentionally introduce atomic-level defects using a technique called ion irradiation but this is technically complicated and expensive. Kazumasa Iida from Nagoya University, Japan, and co-workers have managed to achieve the levels of superconductivity associated with ion irradiation by using so-called grain boundary engineering. Regions of different crystalline orientation are known as grains. The team showed that by controlling the alignment of these grains during synthesis of the superconductor (Ba,K)Fe 2 As 2 , they could maximize the material’s superconductivity. High critical current density and strong pinning efficiency for Fe-based superconductor, K-doped BaFe 2 As 2 , were achieved by naturally formed low-angle grain boundary networks. K-doped BaFe 2 As 2 thin film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. 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For instance, the in-field critical current density of doped BaFe 2 As 2 (Ba122), one of the most technologically important Fe-based superconductors, has been improved over the last decade by APCs created by ion irradiation. The technique of ion irradiation has been commonly implemented to determine the ultimate superconducting properties. However, this method is rather complicated and expensive. Here, we report a surprisingly high critical current density and strong pinning efficiency close to the crystallographic c -axis for a K-doped Ba122 epitaxial thin film without APCs, achieving performance comparable to ion-irradiated K-doped Ba122 single crystals. Microstructural analysis reveals that the film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. This study demonstrates that the upper limit of in-field properties reached in ion-irradiated K-doped Ba122 is achievable by grain boundary engineering, which is a simple and industrially scalable manner. Superconductivity: Engineering crytal structure A way to optimize superconductivity by carefully controlling the atomic-level crystal structure has been developed by scientists in Japan and the USA. Superconductivity is a quantum effect, usually only seen at very low temperatures, in which an electrical current can pass through a material without facing any resistance. One approach to increasing the operating temperature is to intentionally introduce atomic-level defects using a technique called ion irradiation but this is technically complicated and expensive. Kazumasa Iida from Nagoya University, Japan, and co-workers have managed to achieve the levels of superconductivity associated with ion irradiation by using so-called grain boundary engineering. Regions of different crystalline orientation are known as grains. The team showed that by controlling the alignment of these grains during synthesis of the superconductor (Ba,K)Fe 2 As 2 , they could maximize the material’s superconductivity. High critical current density and strong pinning efficiency for Fe-based superconductor, K-doped BaFe 2 As 2 , were achieved by naturally formed low-angle grain boundary networks. K-doped BaFe 2 As 2 thin film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. The achieving superconducting properties are almost 10 times as high as the K-doped BaFe 2 As 2 single crystal and comparable to ion-irradiated single crystal.</description><subject>639/301/119/1003</subject><subject>639/301/299</subject><subject>Atomic structure</subject><subject>Biomaterials</subject><subject>Chemistry and Materials Science</subject><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</subject><subject>critical current</subject><subject>Critical current density</subject><subject>Crystal defects</subject><subject>Crystal structure</subject><subject>Crystallography</subject><subject>Energy Systems</subject><subject>Fe-based superconductors</subject><subject>Grain boundaries</subject><subject>Hc2</subject><subject>Ion irradiation</subject><subject>Jc</subject><subject>Low temperature</subject><subject>low-angle grain boundary</subject><subject>materials for energy and catalysis</subject><subject>MATERIALS SCIENCE</subject><subject>Microstructural analysis</subject><subject>Operating temperature</subject><subject>Optical and Electronic Materials</subject><subject>Pinning</subject><subject>Single crystals</subject><subject>Structural Materials</subject><subject>superconducting properties and materials</subject><subject>Superconductivity</subject><subject>Superconductors</subject><subject>Surface and Interface Science</subject><subject>Thin Films</subject><subject>upper critical field</subject><issn>1884-4049</issn><issn>1884-4057</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>BENPR</sourceid><recordid>eNp9kUFPxCAQhRujiWb1D3gietHEKlBo4bhuXDVu4kXPhNLpbrULK9CY_fey1ujN07wM35sw87LslOBrggtxExhhtMoxJTnGRVHlfC87IkKwnGFe7f9qJg-zkxDeMMakLJng7CjbTjcb77RZdXaJ4grQ0MdurSOgMGzAG2ebwcTdY8JSI3YQkGvRxa2-erqcA50GiuotsjoOXvf9FrXOr6FBvfvMtV32gJZedxbVbrCN9omE-On8ezjODlrdBzj5qZPsdX73MnvIF8_3j7PpIjeMlzE3FS9rUWtZGN7IBsuGMQoVGCM4gC5pkrUgGFdlxSU3RrakpQ0kDTVIVkyys3GuC7FTwXQRzCrtZcFERQSVrJIJOh-htOXHACGqNzd4m_6lKBfpvmVJRKLoSBnvQvDQqo1Px_JbRbDaRaHGKFSKQn1HoXgyFaMpJNguwf-N_sf1BYnBjT0</recordid><startdate>20211022</startdate><enddate>20211022</enddate><creator>Iida, Kazumasa</creator><creator>Qin, Dongyi</creator><creator>Tarantini, Chiara</creator><creator>Hatano, Takafumi</creator><creator>Wang, Chao</creator><creator>Guo, Zimeng</creator><creator>Gao, Hongye</creator><creator>Saito, Hikaru</creator><creator>Hata, Satoshi</creator><creator>Naito, Michio</creator><creator>Yamamoto, Akiyasu</creator><general>Nature Publishing Group UK</general><general>Nature Publishing Group</general><general>Nature Publishing Group Asia</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>OIOZB</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0003-1038-9630</orcidid><orcidid>https://orcid.org/0000-0002-3314-5906</orcidid><orcidid>https://orcid.org/0000-0003-1332-2589</orcidid><orcidid>https://orcid.org/0000000233145906</orcidid><orcidid>https://orcid.org/0000000310389630</orcidid><orcidid>https://orcid.org/0000000313322589</orcidid></search><sort><creationdate>20211022</creationdate><title>Approaching the ultimate superconducting properties of (Ba,K)Fe2As2 by naturally formed low-angle grain boundary networks</title><author>Iida, Kazumasa ; 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For instance, the in-field critical current density of doped BaFe 2 As 2 (Ba122), one of the most technologically important Fe-based superconductors, has been improved over the last decade by APCs created by ion irradiation. The technique of ion irradiation has been commonly implemented to determine the ultimate superconducting properties. However, this method is rather complicated and expensive. Here, we report a surprisingly high critical current density and strong pinning efficiency close to the crystallographic c -axis for a K-doped Ba122 epitaxial thin film without APCs, achieving performance comparable to ion-irradiated K-doped Ba122 single crystals. Microstructural analysis reveals that the film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. This study demonstrates that the upper limit of in-field properties reached in ion-irradiated K-doped Ba122 is achievable by grain boundary engineering, which is a simple and industrially scalable manner. Superconductivity: Engineering crytal structure A way to optimize superconductivity by carefully controlling the atomic-level crystal structure has been developed by scientists in Japan and the USA. Superconductivity is a quantum effect, usually only seen at very low temperatures, in which an electrical current can pass through a material without facing any resistance. One approach to increasing the operating temperature is to intentionally introduce atomic-level defects using a technique called ion irradiation but this is technically complicated and expensive. Kazumasa Iida from Nagoya University, Japan, and co-workers have managed to achieve the levels of superconductivity associated with ion irradiation by using so-called grain boundary engineering. Regions of different crystalline orientation are known as grains. The team showed that by controlling the alignment of these grains during synthesis of the superconductor (Ba,K)Fe 2 As 2 , they could maximize the material’s superconductivity. High critical current density and strong pinning efficiency for Fe-based superconductor, K-doped BaFe 2 As 2 , were achieved by naturally formed low-angle grain boundary networks. K-doped BaFe 2 As 2 thin film is composed of columnar grains with widths of approximately 30–60 nm. The grains are rotated around the b - (or a -) axis by 1.5° and around the c -axis by −1°, resulting in the formation of low-angle grain boundary networks. The achieving superconducting properties are almost 10 times as high as the K-doped BaFe 2 As 2 single crystal and comparable to ion-irradiated single crystal.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><doi>10.1038/s41427-021-00337-5</doi><orcidid>https://orcid.org/0000-0003-1038-9630</orcidid><orcidid>https://orcid.org/0000-0002-3314-5906</orcidid><orcidid>https://orcid.org/0000-0003-1332-2589</orcidid><orcidid>https://orcid.org/0000000233145906</orcidid><orcidid>https://orcid.org/0000000310389630</orcidid><orcidid>https://orcid.org/0000000313322589</orcidid><oa>free_for_read</oa></addata></record>
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subjects 639/301/119/1003
639/301/299
Atomic structure
Biomaterials
Chemistry and Materials Science
CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
critical current
Critical current density
Crystal defects
Crystal structure
Crystallography
Energy Systems
Fe-based superconductors
Grain boundaries
Hc2
Ion irradiation
Jc
Low temperature
low-angle grain boundary
materials for energy and catalysis
MATERIALS SCIENCE
Microstructural analysis
Operating temperature
Optical and Electronic Materials
Pinning
Single crystals
Structural Materials
superconducting properties and materials
Superconductivity
Superconductors
Surface and Interface Science
Thin Films
upper critical field
title Approaching the ultimate superconducting properties of (Ba,K)Fe2As2 by naturally formed low-angle grain boundary networks
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