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![Page 1: Kondo problem to heavy fermions and local ... - pks.mpg.deqimp11/Slides/Steglich_Kondo_HF_Experiment_I.pdf · Kondo problem to heavy fermions and local quantum criticality (Experiment](https://reader030.fdocuments.us/reader030/viewer/2022041205/5d57910288c993f9568b5afd/html5/thumbnails/1.jpg)
Kondo problem to heavy fermions and local quantum criticality (Experiment I)
F. SteglichMPI for Chemical Physics of Solids, 01187 Dresden, Germany
outline:
Kondo effect
Superconductivity vs. magnetism
Heavy fermions
Heavy-fermion superconductors
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1930: T- dependence of the electrical resistivity in pure metals?
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≤ 1970: Noble metals with transition-metal impurities
Kondo effect:
(J. Kondo 1964)
D.K.C. MacDonald et al., Proc. Roy. Soc. A266, 161 (1962)resistivity susceptibility
Curie Weiss law
χ(T) ~ (T + θ)-1, θ = f (TK) > 0
effective moment µeff(T):
(T)/T
T 0 µeff(T) 0
2effμχ(T) ~
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2 CrFe[J/K -mole ]
γ
1.0
CuFe
16
CuCr
T = TK: local Fermi liquid (P. Nozières 1974)
Incremental specific heat of Cu1-xMx (M: Cr, Fe):
ΔC(T) = C(T) – CCu(T)
per mole M: ΔC(T)/x = γT
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> 1970: Rare earth impuritiesJ. Moeser, F. Steglich, G.v. MinnigerodeJ. Low Temp. Phys. 15, 9 (1974)giant thermoelectric power
K. Winzer, Z. Phys. 265, 139 (1973)resistivity
x = 0.00626re-entrant superconductivity ( ) [ ( ) ( )]
( )ce La
cece
T S T T SST
ρ ρ ρρ
− −=
Gorter-Nordheim:
(La1-xCex)Al2
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outline:
Kondo effect
Superconductivity vs. magnetism
Heavy fermions
Heavy-fermion superconductors
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Superconductivity vs. magnetism
IA VIIIA1
H1.008 IIA IIIA IVA VA VIA VIIA
2
He4.003
3
Li6.941
4
Be9.012
5
B10.81
6
C12.01
7
N14.01
8
O16.00
9
F19.00
10
Ne20.18
11
Na22.99
12
Mg24.31 IIIB IVB VB VIB VIIB VIIIB IB IIB
13
Al26.98
14
Si28.09
15
P30.97
16
S32.07
17
Cl35.45
18
Ar39.95
19
K39.10
20
Ca40.08
21
Sc44.96
22
Ti47.87
23
V50.94
24
Cr52.00
25
Mn54.94
26
Fe55.85
27
Co58.93
28
Ni58.69
29
Cu63.55
30
Zn65.39
31
Ga69.72
32
Ge72.61
33
As74.92
34
Se78.96
35
Br79.90
36
Kr83.80
37
Rb85.47
38
Sr87.62
39
Y88.91
40
Zr91.22
41
Nb92.91
42
Mo95.94
43
Tc(98)
44
Ru101.1
45
Rh102.9
46
Pd106.4
47
Ag107.9
48
Cd112.4
49
In114.8
50
Sn118.7
51
Sb121.8
52
Te127.6
53
I126.9
54
Xe131.3
55
Cs132.9
56
Ba137.3
57
La138.9
72
Hf178.5
73
Ta180.9
74
W183.8
75
Re186.2
76
Os190.2
77
Ir192.2
78
Pt195.1
79
Au197.0
80
Hg200.6
81
Tl204.4
82
Pb207.2
83
Bi209.0
84
Po(209)
85
At(210)
86
Rn(222)
87
Fr(223)
88
Ra(226)
89
Ac(227)
104
Rf(261)
105
Db(262)
106
Sg(266)
107
Bh(264)
108
Hs(269)
109
Mt(268)
58
Ce140.1
59
Pr140.9
60
Nd144.2
61
Pm(145)
62
Sm150.4
63
Eu152.0
64
Gd157.3
65
Tb158.9
66
Dy162.5
67
Ho164.9
68
Er167.3
69
Tm168.9
70
Yb173.0
71
Lu175.0
90
Th232.0
91
Pa(231)
92
U238.0
93
Np(237)
94
Pu(244)
95
Am(243)
96
Cm(247)
97
Bk(247)
98
Cf(251)
99
Es(252)
100
Fm(257)
101
Md(258)
102
No(259)
103
Lr(262)
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Tc of La0.99RE0.01
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Pairbreaking by magnetic impurities (theory)
Hint = 2 J S . s
α ~ x S(S + 1)
J > 0
TK ~ TFexp (-1/NFJ)
)1S(S()T/T(ln)1S(Sx~
2
K
2
2
+π++π
α
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Pairbreaking by magnetic impurities (experiment)
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outline:
Kondo effect
Superconductivity vs. magnetism
Heavy fermions
Heavy-fermion superconductors
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TK increases by a factor of 250CeAl2 (x = 1): ≈ 0.3
⇒ TK ≈ 5 K
Volume dependence of Kondo effect, cf.[(La1-zYz)1-xCex]Al2
F.S. et al., Physica 86-88B, 503 (1977). F.S., Adv. Solid State Phys. (1977), Vol. XVII, p.319.
T<< TK : Δρ = ρ0 (1-AT2)
A = π2/(4 )(M. Larsen '75)
)V/()VV(=v22 YAlLaAl 2LaAlV --
v2
KT
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Specific heat of CeAl2
γ = 0.135 J/K2mole
F. S. et al., J. Phys. (Paris) 40, C5-301 (1979).
C.D. Bredl et al., Z. Phys. B 29, 327 (1978).
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γ = 1.62 J/K2mole A = 35 µΩcm/K2
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Superconductivity in CeCu2Si2
100 at% Ce3+ ions necessaryfor superconductivity
(LaCu2Si2 is not a superconductor)
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Heavy-Fermion metals
T >> TK (10 ... 100 K)
T << TK: Heavy electrons ("composite fermions")
→ m* ≈ 1000 mel: "strongly correlated electron system"
Groundstate properties - Heavy Landau Fermi liquid (LFL) : CeCu6- Non-Fermi liquid (NFL) : YbRh2Si2- Magnetic order : NpBe13- Superconductivity : UPd2Al3
vF ≈ 106sm
vF* ≈ 103sm
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outline:
Kondo effect
Superconductivity vs. magnetism
Heavy fermions
Heavy-fermion superconductors
![Page 19: Kondo problem to heavy fermions and local ... - pks.mpg.deqimp11/Slides/Steglich_Kondo_HF_Experiment_I.pdf · Kondo problem to heavy fermions and local quantum criticality (Experiment](https://reader030.fdocuments.us/reader030/viewer/2022041205/5d57910288c993f9568b5afd/html5/thumbnails/19.jpg)
Superconductivity in CeCu2Si2
100 at% Ce3+ ions necessaryfor superconductivity
(LaCu2Si2 is not a superconductor)
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Heavy-fermion superconductivity in CeCu2Si2
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Heavy-fermion superconductivity in UBe13
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Heavy-fermion superconductivity in UPt3
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Heavy-fermion superconductivity in URu2Si2[W. Schlabitz et al., Poster ICVF, Cologne 1984 (unpublished)]
cf. also, T.T.M. Palstra et al., PRL 55, 2727 (1985)M.B. Maple et al., PRL 56, 185 (1986).
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Heavy-fermion superconductorsTc(K)
CeCu2Si2 0.6 ('79 DA/K)[p = 2.9 GPa: 2.3 ('84 GE/GR)]CeNi2Ge2 0.2 ('97 DA, '98 CA/GR) CeIrIn5 0.4 ('00 LANL)CeCoIn5 2.3 ('00 LANL)Ce2CoIn8 0.4 ('02 NA)Ce2PdIn8 0.7 ('09 WR)CePt3Si 0.7 ('03 VI)p > 0CeCu2Ge2 0.6 ('92 GE)CePd2Si2 0.4 ('94 CA) CeRh2Si2 0.4 ('95 LANL)CeCu2 0.15 ('97 GE/KA)CeIn3 0.2 ('98 CA)CeRhIn5 2.1 ('00 LANL)Ce2RhIn8 1.1 ('03 LANL)CeRhSi3 0.8 ('05 SE)CeIrSi3 1.6 ('06 OS)CeCoGe3 0.7 ('06 OS)Ce2Ni3Ge5 0.26 ('06 OS)CeNiGe3 0.4 ('06 OS)CePd5Al2 0,57 (‘08 OS)CeRhGe2 0.45 ('09 OS)CePt2In7 2.1 (‘10 LANL)CeIrGe3 1.5 (’10 OS)
UBe13 0.9 ('83 Z/LANL)UPt3 0.5 ('84 LANL)URu2Si2 1.4 ('84 K/DA)UNi2Al3 1.2 ('91 DA)UPd2Al3 2.0 ('91 DA)URhGe 0.3 ('01 GR)UCoGe 3.0 ('07 AM/KA)p > 0UGe2 0.7 ('00 CA/GR)UIr 0.14 ('04 OS)
NpPd5Al2 5.0 ('07 OS)
PuCoGa5 18.5 ('02 LANL)PuRhGa5 8.7 ('03 KA)
p > 0Am metal 2.2 ('05 KA)
Tc(K) PrOs4Sb12 1.85 ('01 UCSD)
β-YbAlB4 0.08 ('08 TO/IR)
p > 0Eu metal 1.8-2.8 (’09 SL, OS)
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Magnetic Cooper pairing in UPd2Al3
C. Geibel et. al., 1991
Tmagn ≈ 14 Kµs ≈ 0.85 µB
γ ≈ 140 mJ/K2molTc ≈ 2 K2∆0/kBTc ≈ 6 (Kyougaku
et al., 1993)
•Two more localized ("core") electrons: magnetism• one less localized ("heavy" itinerant) electron:
heavy LFL state (Tc< T < TN)heavy-fermion SC (T < Tc)
U3+ (5f3)coexisting with local AF
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Quasiparticle tunneling[M. Jourdan et. al., Nature 398, 47 (1999)]
tunnel diode UPd2Al3 - AlOx - Pb (Pb normal conducting : B = 0.3 T)
dI/dV
(T = 0.15 K)
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Inelastic neutron scattering[N.K. Sato et al., Nature 410, 340 (2001)]
acoustic magnon ("magnetic exciton")
= = (0, 0, 1/2)Tc = 1.8 K
Cooper pairs formed by heavy electrons ("itinerant" 5f electrons)
superconducting glue provided by magnetic excitons in the system of
"localized" 5f electrons
Q 0Q
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Non-Fermi-liquid superconductor UBe13[F. Kromer et al., PRL 81, 4476 (1998); N. Oeschler et al., Acta Phys. Pol. 34, 255 (2003)]
ΔCT vs T C vs T
TL 0 at B* ≈ 4.2 T: QCP
4T ≤ B ≤ 10 T : ρ/ρ(1K) vs T universal
ΔC/T = γ0-βT0.5 (B = 12 T)
P. Gegenwart et al. (2004)
(α =l-1 δl/δT)
α vs T
T 0 : Δρ ~ T1.5
(3D-SDW)
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Double transition in (U1-xThx)Be13 0.019 < x < 0.046 [H.R. Ott et al., Phys. Rev. B 31, 1651 (1985)]
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Phase diagram of U1-xThxBe13[F. Kromer et al., PRB 62, 12477 (2000); JLTP 126, 815 (2002)]
α vs T
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Kondo problem to heavy fermions and local quantum criticality (Experiment II):
Interplay of incipient magnetism and superconductivity in heavy-fermion metals