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Huge Upper Critical Field and Electronic Instability in Pressure-induced Superconductor CeIrSi3 without Inversion Symmetry in the Crystal Structure
We measured low-temperature electrical resistivity in a magnetic field as a function of pressure, and studied the superconducting property of CeIrSi3 with a non-centrosymmetric tetragonal structure. CeIrSi3 is an antiferromagnet with a Néel temperature TN=5.0 K at ambient pressure, but the antiferro...
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Published in: | Journal of the Physical Society of Japan 2008-07, Vol.77 (7) |
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creator | SETTAI, Rikio MIYAUCHI, Yuichiro TAKEUCHI, Tetsuya LEVY, Florence SHEIKIN, Ilya ONUKI, Yoshichika |
description | We measured low-temperature electrical resistivity in a magnetic field as a function of pressure, and studied the superconducting property of CeIrSi3 with a non-centrosymmetric tetragonal structure. CeIrSi3 is an antiferromagnet with a Néel temperature TN=5.0 K at ambient pressure, but the antiferromagnetic ordering disappears completely at a pressure Pc=2.25 GPa. Superconductivity appears in a wide pressure region from 1.8 to about 3.5 GPa, with a maximum transition temperature Tsc\\simeq1.6 K at Pc*\\simeq2.63 GPa. At around Pc*, the upper critical field Hc2 for the magnetic field H along the [0 0 1] direction is not destroyed by spin polarization based on Zeeman coupling but possesses an upturn curvature below 1 K, revealing a divergent tendency of Hc2 at Pc*, with a huge Hc2(0)\\simeq450 kOe. On the other hand, the upper critical field for H||[110] indicates the tendency of Pauli paramagnetic suppression, with Hc2(0)=95 kOe at 2.65 GPa. This might be a combined phenomenon between the electronic instability at Pc* and the characteristic superconducting property without inversion symmetry in the tetragonal structure. |
doi_str_mv | 10.1143/jpsj.77.073705 |
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CeIrSi3 is an antiferromagnet with a Néel temperature TN=5.0 K at ambient pressure, but the antiferromagnetic ordering disappears completely at a pressure Pc=2.25 GPa. Superconductivity appears in a wide pressure region from 1.8 to about 3.5 GPa, with a maximum transition temperature Tsc\\simeq1.6 K at Pc*\\simeq2.63 GPa. At around Pc*, the upper critical field Hc2 for the magnetic field H along the [0 0 1] direction is not destroyed by spin polarization based on Zeeman coupling but possesses an upturn curvature below 1 K, revealing a divergent tendency of Hc2 at Pc*, with a huge Hc2(0)\\simeq450 kOe. On the other hand, the upper critical field for H||[110] indicates the tendency of Pauli paramagnetic suppression, with Hc2(0)=95 kOe at 2.65 GPa. This might be a combined phenomenon between the electronic instability at Pc* and the characteristic superconducting property without inversion symmetry in the tetragonal structure.</description><identifier>ISSN: 0031-9015</identifier><identifier>EISSN: 1347-4073</identifier><identifier>DOI: 10.1143/jpsj.77.073705</identifier><identifier>CODEN: JUPSAU</identifier><language>eng</language><publisher>Tokyo: Institute of Pure and Applied Physics</publisher><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Exact sciences and technology ; Heavy-fermion superconductors ; Physics ; Pressure effects ; Superconducting materials (excluding high-tc compounds) ; Superconductivity ; Transition temperature variations</subject><ispartof>Journal of the Physical Society of Japan, 2008-07, Vol.77 (7)</ispartof><rights>2008 INIST-CNRS</rights><rights>Copyright Japan Science and Technology Agency 2008</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c450t-72df8ad52dc3fac416ddec1899ef10ce00c7b58be24f94613bad8f221e3184333</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=20611968$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>SETTAI, Rikio</creatorcontrib><creatorcontrib>MIYAUCHI, Yuichiro</creatorcontrib><creatorcontrib>TAKEUCHI, Tetsuya</creatorcontrib><creatorcontrib>LEVY, Florence</creatorcontrib><creatorcontrib>SHEIKIN, Ilya</creatorcontrib><creatorcontrib>ONUKI, Yoshichika</creatorcontrib><title>Huge Upper Critical Field and Electronic Instability in Pressure-induced Superconductor CeIrSi3 without Inversion Symmetry in the Crystal Structure</title><title>Journal of the Physical Society of Japan</title><description>We measured low-temperature electrical resistivity in a magnetic field as a function of pressure, and studied the superconducting property of CeIrSi3 with a non-centrosymmetric tetragonal structure. CeIrSi3 is an antiferromagnet with a Néel temperature TN=5.0 K at ambient pressure, but the antiferromagnetic ordering disappears completely at a pressure Pc=2.25 GPa. Superconductivity appears in a wide pressure region from 1.8 to about 3.5 GPa, with a maximum transition temperature Tsc\\simeq1.6 K at Pc*\\simeq2.63 GPa. At around Pc*, the upper critical field Hc2 for the magnetic field H along the [0 0 1] direction is not destroyed by spin polarization based on Zeeman coupling but possesses an upturn curvature below 1 K, revealing a divergent tendency of Hc2 at Pc*, with a huge Hc2(0)\\simeq450 kOe. On the other hand, the upper critical field for H||[110] indicates the tendency of Pauli paramagnetic suppression, with Hc2(0)=95 kOe at 2.65 GPa. 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CeIrSi3 is an antiferromagnet with a Néel temperature TN=5.0 K at ambient pressure, but the antiferromagnetic ordering disappears completely at a pressure Pc=2.25 GPa. Superconductivity appears in a wide pressure region from 1.8 to about 3.5 GPa, with a maximum transition temperature Tsc\\simeq1.6 K at Pc*\\simeq2.63 GPa. At around Pc*, the upper critical field Hc2 for the magnetic field H along the [0 0 1] direction is not destroyed by spin polarization based on Zeeman coupling but possesses an upturn curvature below 1 K, revealing a divergent tendency of Hc2 at Pc*, with a huge Hc2(0)\\simeq450 kOe. On the other hand, the upper critical field for H||[110] indicates the tendency of Pauli paramagnetic suppression, with Hc2(0)=95 kOe at 2.65 GPa. This might be a combined phenomenon between the electronic instability at Pc* and the characteristic superconducting property without inversion symmetry in the tetragonal structure.</abstract><cop>Tokyo</cop><pub>Institute of Pure and Applied Physics</pub><doi>10.1143/jpsj.77.073705</doi></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Exact sciences and technology Heavy-fermion superconductors Physics Pressure effects Superconducting materials (excluding high-tc compounds) Superconductivity Transition temperature variations |
title | Huge Upper Critical Field and Electronic Instability in Pressure-induced Superconductor CeIrSi3 without Inversion Symmetry in the Crystal Structure |
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