Application of µSR Superconductors · • Superconductors – Meissner effect: magnetic field...
Transcript of Application of µSR Superconductors · • Superconductors – Meissner effect: magnetic field...
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17/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Application of µSRSuperconductors
Roberto De Renzi
Dept. SMFI, University of Parma
ITER
Persistent eddy currents:screening
Levitation
KamerlinghOnnes 1911Hg zero resistance
N
S
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17/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
µSR in superconductors
Q0: who did not have any superconductivity in their Syllabus?
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317/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Outline
• Superconductors– Meissner effect: magnetic field expulsion– London penetration of the field– Pairs and free energy– The gap and the coherence length– Type I and type II – Abrikosov flux lattice
• Experimental examples– bulk isotropic case– anisotropic superconductors– LE muons– gap fits– Uemura plot– phase diagrams
TC
Year of discovery
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417/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Meissner - Ochsenfeld effect
Shielding
http://www.superconductors.org/Type1.htm
t
B
Field expulsion: cool a sample below Tc
Meissner-Ochsenfeld effect
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517/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
London model: the penetration depth
A first lengthscale
Ampere Maxwell law
Guess the solution
Right!
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617/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Imagine
Q1: Implant muons in a Meissner state superconductor. What do you detect?
µSµ
Above Tc a precession
When cooling below Tc the precessiondisappears
cooling
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717/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Summary of superconductor facts
• Only for T < TC (pretty low)
• Only below a critical field (H < HC)
• Zero electrical resistance
• Magnetic field expulsion, requires a lenghtscale
How can this be explained?
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817/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Microscopic modelPrototype: BCS
Attraction
Cooper pair, compound bosoncondensation energy (binding) Δ
k
-k
normal metal
Δ
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917/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Mean free energy
Ginzburg-Landau
order parameter
magnetic free energy easy to add
supercurrents
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1017/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
The gap:a second lengthscale
k
-k Coherence length ξ
● how far can you pull a pair apart?
Cooper pair
Inject an electron in a superconductor
● how far from the surface does it starts
to pair (feel the attraction)?
● Ginzburg Landau definition
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1117/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Type I and Type II superconductors
Ginzburg Landau parameter
-M
H
Type I:
Hc
-M
H
Type II:
Hc
Hc1
Hc2
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1217/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Abrikosov flux lattice
H
Hc1
Hc2
-M
H > Hc1
partial field penetration
H = Hc1
magnetic flux quantum
for
periodic solution
of GL equations
H > Hc1
flux lattice
H = Hc2
ΔF = 0
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1317/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Imagine
µ
B
Sµ
µ
B
Sµ
Q2: Homogeneously implant muons in a bulk FL. What do you expect to measure?
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1417/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Field distribution in the FL
• the Flux Lattice is incommensurate to the crystal lattice
• whereas muons are interstitials in the crystal lattice
→ dense random sampling
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1517/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Field distribution in the FL
• GL equations predict
a
bB maxima
B minima
saddle point
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1617/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Experimental caseVanadium
p(B
) arb
. un
its
0.16 T
0.20 T
0.24 T
0.29 T
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1717/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Quck and dirtymultigaussian fit
Comparison with polycrystal data Second moment
is it worth while?
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1817/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Anisotropic penetrationYBa2Cu3O6.9
E.M. Forgan et al. Hyperfine Interactions 63, 71
B
θ
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1917/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
La1.83
Sr0.17
CuO4 crystal
s-wave ns
σ(T): gap fits
YBCO6.95
crystal
Field cool, then shift field down(pinned flux lattice)
d-wave: lines of nodes
PRB42 8019 (1990)
YBCO6.95
powders (!)
0.05 T
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2017/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
LaO0.5F0.5BiS
La Mura et al. Phys. Rev. B 88, 180509(R)
BiS2 ≈ CuO
2: conventional or unconventional superconductor?
s-wave, not d-wave
gap, i.e cost to break a Cooper pair
s-wave gap
p-wave gap
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2117/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Low Energy muonsLondon penetration depth
B=Be−rλ z
µ0H
Field parallel to the surfacedecays exponentially witha penetration depth λ
R. Kiefl et al. PRB 81 180502 (2010)
Single crystal YBa2Cu
3O
6.92
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2217/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
MgB2: two gaps
Two gaps, two fluids,with different effective B
c2
PRB42 8019 (1990)
S. Serventi Phys. Rev. Lett. 93 217003
YBa2Cu
3O
7
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2317/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Uemura plot
σμ=γμ(⟨B2⟩−⟨B ⟩2)
12 ∝
1
λ2∝nsm∗
unconventional
conventional
σ ns T
F
At T=0:
Y.J Uemura et al. Phys Rev Lett. 62, 2317 (1989) 500 cit.
Y.J Uemura et al. Phys Rev Lett. 66, 2665 (1991) 300 cit.
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2417/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Phase diagrams
S. Sanna Phys Rev Lett. 93 207001 (2004) Y.J. Uemura Nature Materials 8 253 (2009)
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2517/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Imagine
Q3: How do we subtract the nuclear relaxation rate σn?
Tc
σn
σ(T)
In quadrature:
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2617/3/2016 RDR - µSR in superconductorsDEPARTMENT OF MATHEMATICAL, PHYSICALAND COMPUTER SCIENCES
Recap
• Muons map the internal field distribution
• Two length scales, λ (currents, fields) and ξ (gap, wave function)
• Refined model (full distribution) for single crystal studies
• Rough model (second moment) for comparative studies
• σ(T) µ λ-2(T): gap(s), symmetries
• coexistence with magnetism
That's it ...