Odd-parity superconductors with two-component order parameters: Nematic and chiral, full gap, and Majorana node
Motivated by the recent experiment indicating that superconductivity in the doped topological insulator CuxBi2Se3 has an odd-parity pairing symmetry with rotational symmetry breaking, we study the general class of odd-parity superconductors with two-component order parameters in trigonal and hexagon...
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Veröffentlicht in: | Physical review. B 2016-11, Vol.94 (18), Article 180504 |
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description | Motivated by the recent experiment indicating that superconductivity in the doped topological insulator CuxBi2Se3 has an odd-parity pairing symmetry with rotational symmetry breaking, we study the general class of odd-parity superconductors with two-component order parameters in trigonal and hexagonal crystal systems. In the presence of strong spin-orbit interaction, we find two possible superconducting phases below Tc, a time-reversal-breaking (i.e., chiral) phase and an anisotropic (i.e., nematic) phase, and determine their relative energetics from the gap function in momentum space. The nematic superconductor generally has a full quasiparticle gap, whereas the chiral superconductor with a three-dimensional (3D) Fermi surface has point nodes with lifted spin degeneracy, resulting in itinerant Majorana fermions in the bulk and topological Majorana arcs on the surface. |
doi_str_mv | 10.1103/PhysRevB.94.180504 |
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The nematic superconductor generally has a full quasiparticle gap, whereas the chiral superconductor with a three-dimensional (3D) Fermi surface has point nodes with lifted spin degeneracy, resulting in itinerant Majorana fermions in the bulk and topological Majorana arcs on the surface.</description><subject>Broken symmetry</subject><subject>Fermi surfaces</subject><subject>Fermions</subject><subject>Order parameters</subject><subject>Parity</subject><subject>Spin-orbit interactions</subject><subject>Superconductivity</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNo9kF1LwzAUhosoOHR_wKuAt-s8SZN28U6HXzCdiF6HNDl1HV1Tk9Sxf2916rk5h8PD-8KTJGcUppRCdvG82oUX_LyeSj6lMxDAD5IR47lMpczl4f8t4DgZh7AGAJqDLECOEre0Nu20r-OOhL5Db1xrexOdD2RbxxWJW5cat-lci20kzlv0ZOD1BiP6cEmecKNjbYhuLTGr2utmQqq-aci77iY_30e9dl63mrTO4mlyVOkm4Ph3nyRvtzev8_t0sbx7mF8tUpNRGdOSSsZngleitMMwwNxWAIxLk9uScpTCWg1WYCEgm7FClshLwTEvKMuRZyfJ-T638-6jxxDV2vW-HSoVGwjJJIAcKLanjHcheKxU5-uN9jtFQX27VX9uleRq7zb7Anu5b38</recordid><startdate>20161101</startdate><enddate>20161101</enddate><creator>Venderbos, Jörn W. 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B</jtitle><date>2016-11-01</date><risdate>2016</risdate><volume>94</volume><issue>18</issue><artnum>180504</artnum><issn>2469-9950</issn><eissn>2469-9969</eissn><abstract>Motivated by the recent experiment indicating that superconductivity in the doped topological insulator CuxBi2Se3 has an odd-parity pairing symmetry with rotational symmetry breaking, we study the general class of odd-parity superconductors with two-component order parameters in trigonal and hexagonal crystal systems. In the presence of strong spin-orbit interaction, we find two possible superconducting phases below Tc, a time-reversal-breaking (i.e., chiral) phase and an anisotropic (i.e., nematic) phase, and determine their relative energetics from the gap function in momentum space. 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subjects | Broken symmetry Fermi surfaces Fermions Order parameters Parity Spin-orbit interactions Superconductivity |
title | Odd-parity superconductors with two-component order parameters: Nematic and chiral, full gap, and Majorana node |
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