Superconducting, Fermi surface, and magnetic properties in SrTGe^sub 3^ and EuTGe^sub 3^ (T: transition metal) with the Rashba-type tetragonal structure
We succeeded in growing single crystals of SrTGe3 (T: transition metal) by the In-flux method and measured the electrical resistivity, specific heat, and de Haas-van Alphen (dHvA) effect. We confirmed superconductivity in SrPdGe3 and SrPtGe3, which was previously observed using polycrystal samples,...
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Veröffentlicht in: | Journal of alloys and compounds 2017-02, Vol.694, p.439 |
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creator | Kakihana, Masashi Akamine, Hiromu Tomori, Keisuke Nishimura, Kengo Teruya, Atsushi Nakamura, Ai Honda, Fuminori Aoki, Dai Nakashima, Miho Amako, Yasushi Matsubayashi, Kazuyuki Uwatoko, Yoshiya Takeuchi, Tetsuya Kida, Takanori Hagiwara, Masayuki Haga, Yoshinori Yamamoto, Etsuji Harima, Hisatomo Hedo, Masato Nakama, Takao Ōnuki, Yoshichika |
description | We succeeded in growing single crystals of SrTGe3 (T: transition metal) by the In-flux method and measured the electrical resistivity, specific heat, and de Haas-van Alphen (dHvA) effect. We confirmed superconductivity in SrPdGe3 and SrPtGe3, which was previously observed using polycrystal samples, and also found superconductivity for SrRhGe3, SrIrGe3, and SrNiGe3. Furthermore, from the results of dHvA experiments and energy band calculations, Fermi surfaces of SrIrGe3 are found to split into two similar Fermi surfaces, reflecting the Rashba-type non-centrosymmetric tetragonal structure. We also grew single crystals of EuTGe3 by the same In-flux method and studied magnetic properties, especially focusing on magnetism of EuIrGe3 with a Néel temperature TN=12.2 K and a successive magnetic transition TN=7.3 K. The magnetic phase diagram of EuIrGe3 is found to consist of three antiferromagnetic phases named AF1, AF2, and AF3. A critical field Hc reaching a saturated moment of 7 µB/Eu is determined as Hc≂ 160 kOe from a high-field magnetization curve. We proposed a simple helical magnetic structure based on the Dzyaloshinskii-Moriya interaction. |
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We confirmed superconductivity in SrPdGe3 and SrPtGe3, which was previously observed using polycrystal samples, and also found superconductivity for SrRhGe3, SrIrGe3, and SrNiGe3. Furthermore, from the results of dHvA experiments and energy band calculations, Fermi surfaces of SrIrGe3 are found to split into two similar Fermi surfaces, reflecting the Rashba-type non-centrosymmetric tetragonal structure. We also grew single crystals of EuTGe3 by the same In-flux method and studied magnetic properties, especially focusing on magnetism of EuIrGe3 with a Néel temperature TN=12.2 K and a successive magnetic transition TN=7.3 K. The magnetic phase diagram of EuIrGe3 is found to consist of three antiferromagnetic phases named AF1, AF2, and AF3. A critical field Hc reaching a saturated moment of 7 µB/Eu is determined as Hc≂ 160 kOe from a high-field magnetization curve. We proposed a simple helical magnetic structure based on the Dzyaloshinskii-Moriya interaction.</description><identifier>ISSN: 0925-8388</identifier><identifier>EISSN: 1873-4669</identifier><language>eng</language><publisher>Lausanne: Elsevier BV</publisher><subject>Antiferromagnetism ; Critical field (superconductivity) ; De Haas-Van Alphen effect ; Electrical resistivity ; Fermi surfaces ; Flux ; Magnetic properties ; Magnetic structure ; Magnetism ; Physical properties ; Polycrystals ; Single crystals ; Specific heat ; Superconductivity</subject><ispartof>Journal of alloys and compounds, 2017-02, Vol.694, p.439</ispartof><rights>Copyright Elsevier BV Feb 15, 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780</link.rule.ids></links><search><creatorcontrib>Kakihana, Masashi</creatorcontrib><creatorcontrib>Akamine, Hiromu</creatorcontrib><creatorcontrib>Tomori, Keisuke</creatorcontrib><creatorcontrib>Nishimura, Kengo</creatorcontrib><creatorcontrib>Teruya, Atsushi</creatorcontrib><creatorcontrib>Nakamura, Ai</creatorcontrib><creatorcontrib>Honda, Fuminori</creatorcontrib><creatorcontrib>Aoki, Dai</creatorcontrib><creatorcontrib>Nakashima, Miho</creatorcontrib><creatorcontrib>Amako, Yasushi</creatorcontrib><creatorcontrib>Matsubayashi, Kazuyuki</creatorcontrib><creatorcontrib>Uwatoko, Yoshiya</creatorcontrib><creatorcontrib>Takeuchi, Tetsuya</creatorcontrib><creatorcontrib>Kida, Takanori</creatorcontrib><creatorcontrib>Hagiwara, Masayuki</creatorcontrib><creatorcontrib>Haga, Yoshinori</creatorcontrib><creatorcontrib>Yamamoto, Etsuji</creatorcontrib><creatorcontrib>Harima, Hisatomo</creatorcontrib><creatorcontrib>Hedo, Masato</creatorcontrib><creatorcontrib>Nakama, Takao</creatorcontrib><creatorcontrib>Ōnuki, Yoshichika</creatorcontrib><title>Superconducting, Fermi surface, and magnetic properties in SrTGe^sub 3^ and EuTGe^sub 3^ (T: transition metal) with the Rashba-type tetragonal structure</title><title>Journal of alloys and compounds</title><description>We succeeded in growing single crystals of SrTGe3 (T: transition metal) by the In-flux method and measured the electrical resistivity, specific heat, and de Haas-van Alphen (dHvA) effect. We confirmed superconductivity in SrPdGe3 and SrPtGe3, which was previously observed using polycrystal samples, and also found superconductivity for SrRhGe3, SrIrGe3, and SrNiGe3. Furthermore, from the results of dHvA experiments and energy band calculations, Fermi surfaces of SrIrGe3 are found to split into two similar Fermi surfaces, reflecting the Rashba-type non-centrosymmetric tetragonal structure. We also grew single crystals of EuTGe3 by the same In-flux method and studied magnetic properties, especially focusing on magnetism of EuIrGe3 with a Néel temperature TN=12.2 K and a successive magnetic transition TN=7.3 K. The magnetic phase diagram of EuIrGe3 is found to consist of three antiferromagnetic phases named AF1, AF2, and AF3. A critical field Hc reaching a saturated moment of 7 µB/Eu is determined as Hc≂ 160 kOe from a high-field magnetization curve. We proposed a simple helical magnetic structure based on the Dzyaloshinskii-Moriya interaction.</description><subject>Antiferromagnetism</subject><subject>Critical field (superconductivity)</subject><subject>De Haas-Van Alphen effect</subject><subject>Electrical resistivity</subject><subject>Fermi surfaces</subject><subject>Flux</subject><subject>Magnetic properties</subject><subject>Magnetic structure</subject><subject>Magnetism</subject><subject>Physical properties</subject><subject>Polycrystals</subject><subject>Single crystals</subject><subject>Specific heat</subject><subject>Superconductivity</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNqNj81KAzEUhYNYcPx5hwtuFDqQMXWauJVW13bWLen0diZlJhlzbxDfxMc1iAuXrg4cvgPfORNFpZeqXNS1OReFNA-PpVZaX4hLopOUsjKqKsTXJk0Y2-APqWXnuzmsMY4OKMWjbXEO1h9gtJ1Hdi1MMWSaHRI4D5vYvOCW0h7U9odbpT_FXfMEHK0nxy54GJHtcA8fjnvgHuHNUr-3JX9OCIwZ7IK3AxDHLJIiXovZ0Q6EN795JW7Xq-b5tcwO7wmJd6eQYp7QLj9RRtdmKdX_qG-E81oQ</recordid><startdate>20170215</startdate><enddate>20170215</enddate><creator>Kakihana, Masashi</creator><creator>Akamine, Hiromu</creator><creator>Tomori, Keisuke</creator><creator>Nishimura, Kengo</creator><creator>Teruya, Atsushi</creator><creator>Nakamura, Ai</creator><creator>Honda, Fuminori</creator><creator>Aoki, Dai</creator><creator>Nakashima, Miho</creator><creator>Amako, Yasushi</creator><creator>Matsubayashi, Kazuyuki</creator><creator>Uwatoko, Yoshiya</creator><creator>Takeuchi, Tetsuya</creator><creator>Kida, Takanori</creator><creator>Hagiwara, Masayuki</creator><creator>Haga, Yoshinori</creator><creator>Yamamoto, Etsuji</creator><creator>Harima, Hisatomo</creator><creator>Hedo, Masato</creator><creator>Nakama, Takao</creator><creator>Ōnuki, Yoshichika</creator><general>Elsevier BV</general><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20170215</creationdate><title>Superconducting, Fermi surface, and magnetic properties in SrTGe^sub 3^ and EuTGe^sub 3^ (T: transition metal) with the Rashba-type tetragonal structure</title><author>Kakihana, Masashi ; Akamine, Hiromu ; Tomori, Keisuke ; Nishimura, Kengo ; Teruya, Atsushi ; Nakamura, Ai ; Honda, Fuminori ; Aoki, Dai ; Nakashima, Miho ; Amako, Yasushi ; Matsubayashi, Kazuyuki ; Uwatoko, Yoshiya ; Takeuchi, Tetsuya ; Kida, Takanori ; Hagiwara, Masayuki ; Haga, Yoshinori ; Yamamoto, Etsuji ; Harima, Hisatomo ; Hedo, Masato ; Nakama, Takao ; Ōnuki, Yoshichika</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_19339869703</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Antiferromagnetism</topic><topic>Critical field (superconductivity)</topic><topic>De Haas-Van Alphen effect</topic><topic>Electrical resistivity</topic><topic>Fermi surfaces</topic><topic>Flux</topic><topic>Magnetic properties</topic><topic>Magnetic structure</topic><topic>Magnetism</topic><topic>Physical properties</topic><topic>Polycrystals</topic><topic>Single crystals</topic><topic>Specific heat</topic><topic>Superconductivity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kakihana, Masashi</creatorcontrib><creatorcontrib>Akamine, Hiromu</creatorcontrib><creatorcontrib>Tomori, Keisuke</creatorcontrib><creatorcontrib>Nishimura, Kengo</creatorcontrib><creatorcontrib>Teruya, Atsushi</creatorcontrib><creatorcontrib>Nakamura, Ai</creatorcontrib><creatorcontrib>Honda, Fuminori</creatorcontrib><creatorcontrib>Aoki, Dai</creatorcontrib><creatorcontrib>Nakashima, Miho</creatorcontrib><creatorcontrib>Amako, Yasushi</creatorcontrib><creatorcontrib>Matsubayashi, Kazuyuki</creatorcontrib><creatorcontrib>Uwatoko, Yoshiya</creatorcontrib><creatorcontrib>Takeuchi, Tetsuya</creatorcontrib><creatorcontrib>Kida, Takanori</creatorcontrib><creatorcontrib>Hagiwara, Masayuki</creatorcontrib><creatorcontrib>Haga, Yoshinori</creatorcontrib><creatorcontrib>Yamamoto, Etsuji</creatorcontrib><creatorcontrib>Harima, Hisatomo</creatorcontrib><creatorcontrib>Hedo, Masato</creatorcontrib><creatorcontrib>Nakama, Takao</creatorcontrib><creatorcontrib>Ōnuki, Yoshichika</creatorcontrib><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of alloys and compounds</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kakihana, Masashi</au><au>Akamine, Hiromu</au><au>Tomori, Keisuke</au><au>Nishimura, Kengo</au><au>Teruya, Atsushi</au><au>Nakamura, Ai</au><au>Honda, Fuminori</au><au>Aoki, Dai</au><au>Nakashima, Miho</au><au>Amako, Yasushi</au><au>Matsubayashi, Kazuyuki</au><au>Uwatoko, Yoshiya</au><au>Takeuchi, Tetsuya</au><au>Kida, Takanori</au><au>Hagiwara, Masayuki</au><au>Haga, Yoshinori</au><au>Yamamoto, Etsuji</au><au>Harima, Hisatomo</au><au>Hedo, Masato</au><au>Nakama, Takao</au><au>Ōnuki, Yoshichika</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Superconducting, Fermi surface, and magnetic properties in SrTGe^sub 3^ and EuTGe^sub 3^ (T: transition metal) with the Rashba-type tetragonal structure</atitle><jtitle>Journal of alloys and compounds</jtitle><date>2017-02-15</date><risdate>2017</risdate><volume>694</volume><spage>439</spage><pages>439-</pages><issn>0925-8388</issn><eissn>1873-4669</eissn><abstract>We succeeded in growing single crystals of SrTGe3 (T: transition metal) by the In-flux method and measured the electrical resistivity, specific heat, and de Haas-van Alphen (dHvA) effect. We confirmed superconductivity in SrPdGe3 and SrPtGe3, which was previously observed using polycrystal samples, and also found superconductivity for SrRhGe3, SrIrGe3, and SrNiGe3. Furthermore, from the results of dHvA experiments and energy band calculations, Fermi surfaces of SrIrGe3 are found to split into two similar Fermi surfaces, reflecting the Rashba-type non-centrosymmetric tetragonal structure. We also grew single crystals of EuTGe3 by the same In-flux method and studied magnetic properties, especially focusing on magnetism of EuIrGe3 with a Néel temperature TN=12.2 K and a successive magnetic transition TN=7.3 K. The magnetic phase diagram of EuIrGe3 is found to consist of three antiferromagnetic phases named AF1, AF2, and AF3. A critical field Hc reaching a saturated moment of 7 µB/Eu is determined as Hc≂ 160 kOe from a high-field magnetization curve. We proposed a simple helical magnetic structure based on the Dzyaloshinskii-Moriya interaction.</abstract><cop>Lausanne</cop><pub>Elsevier BV</pub></addata></record> |
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subjects | Antiferromagnetism Critical field (superconductivity) De Haas-Van Alphen effect Electrical resistivity Fermi surfaces Flux Magnetic properties Magnetic structure Magnetism Physical properties Polycrystals Single crystals Specific heat Superconductivity |
title | Superconducting, Fermi surface, and magnetic properties in SrTGe^sub 3^ and EuTGe^sub 3^ (T: transition metal) with the Rashba-type tetragonal structure |
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