Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?

Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap...
Ausführliche Beschreibung

Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ . Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Noat, Yves [verfasserIn] Mauger, Alain [verfasserIn] Nohara, Minoru [verfasserIn] Eisaki, Hiroshi [verfasserIn] Ishida, Shigeyuki [verfasserIn] Sacks, William [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity

Übergeordnetes Werk:	Enthalten in: Solid state communications - New York, NY [u.a.] : Elsevier Science, 1963, 348
Übergeordnetes Werk:	volume:348

DOI / URN:	10.1016/j.ssc.2022.114689

Katalog-ID:	ELV057358605

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245	1	0	\|a Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?
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520			\|a Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ .
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allfields	10.1016/j.ssc.2022.114689 doi (DE-627)ELV057358605 (ELSEVIER)S0038-1098(22)00037-0 DE-627 ger DE-627 rda eng 540 530 VZ 33.00 bkl Noat, Yves verfasserin (orcid)0000-0003-1869-7160 aut Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line? 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ . Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity Mauger, Alain verfasserin aut Nohara, Minoru verfasserin (orcid)0000-0003-1931-9903 aut Eisaki, Hiroshi verfasserin aut Ishida, Shigeyuki verfasserin (orcid)0000-0001-9445-8079 aut Sacks, William verfasserin aut Enthalten in Solid state communications New York, NY [u.a.] : Elsevier Science, 1963 348 Online-Ressource (DE-627)266878830 (DE-600)1467698-9 (DE-576)075145502 1879-2766 nnns volume:348 GBV_USEFLAG_U GBV_ELV SYSFLAG_U 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 VZ AR 348
spelling	10.1016/j.ssc.2022.114689 doi (DE-627)ELV057358605 (ELSEVIER)S0038-1098(22)00037-0 DE-627 ger DE-627 rda eng 540 530 VZ 33.00 bkl Noat, Yves verfasserin (orcid)0000-0003-1869-7160 aut Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line? 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ . Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity Mauger, Alain verfasserin aut Nohara, Minoru verfasserin (orcid)0000-0003-1931-9903 aut Eisaki, Hiroshi verfasserin aut Ishida, Shigeyuki verfasserin (orcid)0000-0001-9445-8079 aut Sacks, William verfasserin aut Enthalten in Solid state communications New York, NY [u.a.] : Elsevier Science, 1963 348 Online-Ressource (DE-627)266878830 (DE-600)1467698-9 (DE-576)075145502 1879-2766 nnns volume:348 GBV_USEFLAG_U GBV_ELV SYSFLAG_U 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 VZ AR 348
allfields_unstemmed	10.1016/j.ssc.2022.114689 doi (DE-627)ELV057358605 (ELSEVIER)S0038-1098(22)00037-0 DE-627 ger DE-627 rda eng 540 530 VZ 33.00 bkl Noat, Yves verfasserin (orcid)0000-0003-1869-7160 aut Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line? 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ . Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity Mauger, Alain verfasserin aut Nohara, Minoru verfasserin (orcid)0000-0003-1931-9903 aut Eisaki, Hiroshi verfasserin aut Ishida, Shigeyuki verfasserin (orcid)0000-0001-9445-8079 aut Sacks, William verfasserin aut Enthalten in Solid state communications New York, NY [u.a.] : Elsevier Science, 1963 348 Online-Ressource (DE-627)266878830 (DE-600)1467698-9 (DE-576)075145502 1879-2766 nnns volume:348 GBV_USEFLAG_U GBV_ELV SYSFLAG_U 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 VZ AR 348
allfieldsGer	10.1016/j.ssc.2022.114689 doi (DE-627)ELV057358605 (ELSEVIER)S0038-1098(22)00037-0 DE-627 ger DE-627 rda eng 540 530 VZ 33.00 bkl Noat, Yves verfasserin (orcid)0000-0003-1869-7160 aut Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line? 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ . Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity Mauger, Alain verfasserin aut Nohara, Minoru verfasserin (orcid)0000-0003-1931-9903 aut Eisaki, Hiroshi verfasserin aut Ishida, Shigeyuki verfasserin (orcid)0000-0001-9445-8079 aut Sacks, William verfasserin aut Enthalten in Solid state communications New York, NY [u.a.] : Elsevier Science, 1963 348 Online-Ressource (DE-627)266878830 (DE-600)1467698-9 (DE-576)075145502 1879-2766 nnns volume:348 GBV_USEFLAG_U GBV_ELV SYSFLAG_U 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 VZ AR 348
allfieldsSound	10.1016/j.ssc.2022.114689 doi (DE-627)ELV057358605 (ELSEVIER)S0038-1098(22)00037-0 DE-627 ger DE-627 rda eng 540 530 VZ 33.00 bkl Noat, Yves verfasserin (orcid)0000-0003-1869-7160 aut Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line? 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ . Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity Mauger, Alain verfasserin aut Nohara, Minoru verfasserin (orcid)0000-0003-1931-9903 aut Eisaki, Hiroshi verfasserin aut Ishida, Shigeyuki verfasserin (orcid)0000-0001-9445-8079 aut Sacks, William verfasserin aut Enthalten in Solid state communications New York, NY [u.a.] : Elsevier Science, 1963 348 Online-Ressource (DE-627)266878830 (DE-600)1467698-9 (DE-576)075145502 1879-2766 nnns volume:348 GBV_USEFLAG_U GBV_ELV SYSFLAG_U 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 VZ AR 348
language	English
source	Enthalten in Solid state communications 348 volume:348
sourceStr	Enthalten in Solid state communications 348 volume:348
format_phy_str_mv	Article
bklname	Physik: Allgemeines
institution	findex.gbv.de
topic_facet	Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity
dewey-raw	540
isfreeaccess_bool	false
container_title	Solid state communications
authorswithroles_txt_mv	Noat, Yves @@aut@@ Mauger, Alain @@aut@@ Nohara, Minoru @@aut@@ Eisaki, Hiroshi @@aut@@ Ishida, Shigeyuki @@aut@@ Sacks, William @@aut@@
publishDateDaySort_date	2022-01-01T00:00:00Z
hierarchy_top_id	266878830
dewey-sort	3540
id	ELV057358605
language_de	englisch
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author	Noat, Yves
spellingShingle	Noat, Yves ddc 540 bkl 33.00 misc Cuprate superconductors misc Pseudogap misc Magnetic susceptibility misc Unconventional superconductivity Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?
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topic_title	540 530 VZ 33.00 bkl Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line? Cuprate superconductors Pseudogap Magnetic susceptibility Unconventional superconductivity
topic	ddc 540 bkl 33.00 misc Cuprate superconductors misc Pseudogap misc Magnetic susceptibility misc Unconventional superconductivity
topic_unstemmed	ddc 540 bkl 33.00 misc Cuprate superconductors misc Pseudogap misc Magnetic susceptibility misc Unconventional superconductivity
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title	Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?
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title_full	Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?
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title_sort	cuprates phase diagram deduced from magnetic susceptibility: what is the ‘true’ pseudogap line?
title_auth	Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?
abstract	Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ .
abstractGer	Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ .
abstract_unstemmed	Two contradictory phase diagrams have dominated the literature of high- T c cuprate superconductors. Does the pseudogap line cross the superconducting T c -dome or not? To answer, we have revisited the experimental magnetic susceptibility and knight shift of four different compounds, La 1 − x Sr x CuO 4 , Bi 2 Sr 2 Ca 1 − x Y x Cu 2 O 8 , Bi 2 Sr 2 CaCu 2 O 8 + y , YBa 2 Cu 3 O 6 + y , as a function of temperature and doping. The susceptibility can be described by the same function for all materials, having a magnetic and an electronic contributions. The former is the 2D antiferromagnetic (AF) square lattice response, with a characteristic temperature of magnetic correlations T m a x . The latter is the ‘Pauli’ term, revealing the gap opening in the electronic density of states at the pseudogap temperature T ∗ .
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title_short	Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?
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author2	Mauger, Alain Nohara, Minoru Eisaki, Hiroshi Ishida, Shigeyuki Sacks, William
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Cuprates phase diagram deduced from magnetic susceptibility: What is the ‘true’ pseudogap line?

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