Orbital driven two-dome superconducting phases in multiorbital superconductors

We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes. Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Liu, Jing [verfasserIn] Wang, Qing-Wei [verfasserIn] Zou, Liang-Jian [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2020

Schlagwörter:	Unconventional superconductor Phase diagram Theory Orbital degeneracy

Übergeordnetes Werk:	Enthalten in: Physics letters / A - Amsterdam : North-Holland Publ., 1967, 391
Übergeordnetes Werk:	volume:391

DOI / URN:	10.1016/j.physleta.2020.127118

Katalog-ID:	ELV005419220

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520			\|a We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes.
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allfields	10.1016/j.physleta.2020.127118 doi (DE-627)ELV005419220 (ELSEVIER)S0375-9601(20)30985-3 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Liu, Jing verfasserin aut Orbital driven two-dome superconducting phases in multiorbital superconductors 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes. Unconventional superconductor Phase diagram Theory Orbital degeneracy Wang, Qing-Wei verfasserin aut Zou, Liang-Jian verfasserin aut Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 391 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:391 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 391
spelling	10.1016/j.physleta.2020.127118 doi (DE-627)ELV005419220 (ELSEVIER)S0375-9601(20)30985-3 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Liu, Jing verfasserin aut Orbital driven two-dome superconducting phases in multiorbital superconductors 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes. Unconventional superconductor Phase diagram Theory Orbital degeneracy Wang, Qing-Wei verfasserin aut Zou, Liang-Jian verfasserin aut Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 391 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:391 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 391
allfields_unstemmed	10.1016/j.physleta.2020.127118 doi (DE-627)ELV005419220 (ELSEVIER)S0375-9601(20)30985-3 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Liu, Jing verfasserin aut Orbital driven two-dome superconducting phases in multiorbital superconductors 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes. Unconventional superconductor Phase diagram Theory Orbital degeneracy Wang, Qing-Wei verfasserin aut Zou, Liang-Jian verfasserin aut Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 391 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:391 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 391
allfieldsGer	10.1016/j.physleta.2020.127118 doi (DE-627)ELV005419220 (ELSEVIER)S0375-9601(20)30985-3 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Liu, Jing verfasserin aut Orbital driven two-dome superconducting phases in multiorbital superconductors 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes. Unconventional superconductor Phase diagram Theory Orbital degeneracy Wang, Qing-Wei verfasserin aut Zou, Liang-Jian verfasserin aut Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 391 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:391 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 391
allfieldsSound	10.1016/j.physleta.2020.127118 doi (DE-627)ELV005419220 (ELSEVIER)S0375-9601(20)30985-3 DE-627 ger DE-627 rda eng 530 DE-600 33.00 bkl Liu, Jing verfasserin aut Orbital driven two-dome superconducting phases in multiorbital superconductors 2020 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes. Unconventional superconductor Phase diagram Theory Orbital degeneracy Wang, Qing-Wei verfasserin aut Zou, Liang-Jian verfasserin aut Enthalten in Physics letters / A Amsterdam : North-Holland Publ., 1967 391 Online-Ressource (DE-627)266015298 (DE-600)1466603-0 (DE-576)074959905 1873-2429 nnns volume:391 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.00 Physik: Allgemeines AR 391
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author	Liu, Jing
spellingShingle	Liu, Jing ddc 530 bkl 33.00 misc Unconventional superconductor misc Phase diagram misc Theory misc Orbital degeneracy Orbital driven two-dome superconducting phases in multiorbital superconductors
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topic_title	530 DE-600 33.00 bkl Orbital driven two-dome superconducting phases in multiorbital superconductors Unconventional superconductor Phase diagram Theory Orbital degeneracy
topic	ddc 530 bkl 33.00 misc Unconventional superconductor misc Phase diagram misc Theory misc Orbital degeneracy
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title	Orbital driven two-dome superconducting phases in multiorbital superconductors
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title_full	Orbital driven two-dome superconducting phases in multiorbital superconductors
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title_sort	orbital driven two-dome superconducting phases in multiorbital superconductors
title_auth	Orbital driven two-dome superconducting phases in multiorbital superconductors
abstract	We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes.
abstractGer	We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes.
abstract_unstemmed	We theoretically study the superconductivity in multiorbital superconductors based on a three-orbital tight-banding model. With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. We find that the competition between different orbital pairing leads to two-dome SC phase diagrams in multiorbital superconductors, and different matrix elements of J 1 and J 2 considerably affect the boundary of two SC domes.
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title_short	Orbital driven two-dome superconducting phases in multiorbital superconductors
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doi_str	10.1016/j.physleta.2020.127118
up_date	2024-07-06T17:54:25.750Z
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With appropriate values of the nearest-neighbor exchange J 1 α β and the next-nearest-neighbor exchange J 2 α β , we find a two-dome structure in the T c − n phase diagram: one dome in the doping range n < 3.9 where the superconducting (SC) state is mainly s x 2 y 2 component contributed by inter-orbital pairing, the other dome in the doping range 3.9 < n < 4.46 where the SC state is mainly s x 2 y 2 + s x 2 + y 2 components contributed by intra-orbital pairing. 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Orbital driven two-dome superconducting phases in multiorbital superconductors

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