andreev reflection at the cecoin 5 heavy fermion superconductor interface wan kyu park and laura h....
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![Page 1: Andreev reflection at the CeCoIn 5 Heavy Fermion Superconductor Interface Wan Kyu Park and Laura H. Greene UIUC John L. Sarrao and Joe D. Thompson LANL](https://reader037.vdocuments.us/reader037/viewer/2022103123/56649d4b5503460f94a2972d/html5/thumbnails/1.jpg)
Andreev reflection at the CeCoIn5 Heavy Fermion Superconductor Interface
Wan Kyu Park and Laura H. Greene UIUCJohn L. Sarrao and Joe D. Thompson LANL
Theoretical support:Justin E. Elenewski UIUC, Greene groupVladimir Lukic UIUC, Leggett groupAnthony J. Leggett UIUCDavid Pines LANL & UIUC
Experimental supportKaren Parkinson UIUC, Undergraduate Thesis StudentCaitlin Jo Ramsey UIUC, UndergraduateB. Florian Wilken UIUC, German exchange student, 03-04Alex N. Thaler UIUC, REU 2003Patrick J. Hentges UIUC, PhD, 2004, now at IntelWilliam L. Feldman UIUC, Lab Tech, retired 2003
Funding support: US DoE, DEFG02-91ER45439 through FSMRL and CMM
RTS Workshop, June 10-11, 2005, Notre Dame, IN
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Conditions ~10ms after Big Bang:
•10 GeV/fm3 or ~1016gm/cm3
•T ~ 170 MeV or ~ 2 x 1012 K
Same physics as superconductivity, (strongly-correlated electron systems) but 1016 different in energy !
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I. Definition of Issues• Andreev reflection between a heavy-fermion
superconductor (HFS) and a normal (N) metal: • Point Contact Spectroscopy (PCS):
II. The HF superconductor CeCoIn5
III. Some Basics of Andreev Reflection and PCS
IV. Experiment: Cantilever-Andreev-Tunneling (CAT)
V. Data & Analysis (extended BTK model)• Known theories cannot explain AR at the
N/HFS interface: • Some analysis consistent with d-wave and
strong-coupling• New data on (110) may show spectroscopic
evidence for d-wave
VI. Conclusions
Outline
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Definition of the issues
1. Understanding charge transport across HF interface Existing models cannot account for
Andreev reflection at the HFS/N interface
2. Spectroscopic studies of CeCoIn5 (OP symmetry, mechanism, etc.,…)
-2.0 -1.0 0.0 1.0 2.0
1.0
1.2
1.4
1.6
1.8
2.0
exp. data s-wave BTK d-wave BTK
Nor
mal
ized
Con
duct
ance
Voltage (mV)
-2 -1 0 1 2
0.9
1.0
1.1
400 mK 2.6K
dI/d
V /
dI/d
V| V
= -
2mV
Voltage (mV)
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The Heavy-Fermion Superconductor CeCoIn5
C. Petrovic et al., J. Phys.: Condens. Matter 13, L337 (2001)
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Tc = 2.3K (record high for HFS) 0
ab = 82Å, 0c = 53Å, ab ~ 1900Å, c ~ 2700Å,
Hc2ab(0) = 12T, Hc2
c(0) = 5T
Superconductivity in clean limit (l >> 0, l = 810Å)
Non-Fermi liquid: ~ T 1.0 ± 0.1, Cen / T ~ -lnT, 1 / T1T ~ T –3/4
Heavy-fermion liquid- n = Cen / T = 0.35J/mol K2, meff = 83m0 “heavy-fermion”
- (0) ~ 10 -2 emu/mol
- ( - 0) / T 2 ~ 0.1cm/K2 (under high pressure)
- Transition from Kondo impurity fluid to coherent heavy electron fluid at T *
TK ~ 1.7K (single ion Kondo temperature)
T * ~ 45K (intersite coupling energy of Kondo lattice) CEF splitting~120K (Nakatsuji, Pines, Fisk, PRL 92, 016401 (2004))
Anisotropic type-II superconductor d-wave pairing symmetry? (Spectroscopic evidence is still lacking) FFLO phase transition? - Power-law dependence: Cen / T ~ T, ~ T 3.37, 1/T1 ~ T 3+, ~ T 1.5
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Layered-tetragonal Crystal Structure Quasi-2D Fermi Surfaces
a = 4.62Å, c = 7.55Å, c/a = 1.63
T = Co, Rh, Ir
H. Shishido et al., JPSJ. 71, 162 (2002)
Ce
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e
N S
h+
N S
Pair Breaking
Probability of finding Cooper Pairs
ANDREEV REFLECTION (no insulator): Normal Metal/Superconductor (N/S)
In N: Electrons retro-reflected as holes
In S: Cooper
Pairs Broken
near interface
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EF (few V)
E
k
Energy Scales for Andreev Reflection
SN
Particle conversion process that conserves charge, energy and
momentum!
Δ (few mV)
≈≈
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A : Andreev reflectionB : Normal reflectionC : Transmission without branch- crossing (electron-like)D : Transmission with branch- crossing (hole-like)A(E)+B(E)+C(E)+D(E)=1
Probabilities
Blonder-Tinkham-Klapwijk (BTK) Model for charge transport across the N/S interface PRB 25, 4515 (1982)
Assumes (among other things) Ballistic transport
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s-wave BTK Conductance
• Describes transitional behavior from AR to tunneling• Effective barrier strength
22 (1 )
, 4
FNeff
FS
r vZ Z r vr
-4 -2 0 2 40
1
2
E/DE/D
E/D
RNd
I/d
V
Z=0.0
RNd
I/d
V
E/D-4 -2 0 2 4
0
1
2
Z=0.5
-4 -2 0 2 40
2
4
Z=1.5
RNd
I/d
V
RNd
I/d
V
-4 -2 0 2 40
2
4
6
8
Z=5
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S. Kashiwaya et al., PRB 53, 2667 (1996) Extended BTK theory
22
+
, cos 2
, ,
The con
c-axis junction of d-wave superco
ductance is given
the integration over the half space of momentu
ndu
y
m
c
b
tor
T T
E E
2 2
2 2
22
0 0
0
2
1
1
, , k exp
cos = , , sin sin
cos
, c
1
1 1 e
os
xp
S
FS FS
S FSFS S FN N
N FN
N
N NN
N
E a E b E
EE k i
kk k
k
ZZ
i i
Z
0 2
2 2
4
1 4
FN
N
mH
k
Z
' , =E E i
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d-wave BTK Conductance
along c-axis
-4 -2 0 2 40
1
2
E/DE/D
E/D
RNd
I/d
VZ=0.0
RNd
I/d
V
E/D-4 -2 0 2 4
0
1
2
Z=0.5
-4 -2 0 2 40
1
2
Z=1.5R
Nd
I/d
V
RNd
I/d
V
-4 -2 0 2 40
2
Z=5
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BTK model has worked well for a wide range of materials, but NOT for HFS/N interfaces:
22 (1 )
, 4
FNeff
FS
r vZ Z r vr
Recall the effective barrier
strength:
The Fermi velocity mismatch is so great at the HFS/N interface that
Andreev reflection (AR) should never occur
(Z>5, extreme tunneling limit).
However, AR is routinely measured at the N/HFS interface (many reports), albeit
suppressed.
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Gold tip - sharpened by electrochemical etchingCeCoIn5 single crystal - c-axis oriented - etch-cleaned using H3PO4
Coarse approach - done before inserting probeFine approach - done during cool down - piezo driven by computer control Operation range - Temperature : down to 300mK - Magnetic Field : up to 12T
B e-C u
S c re w(C o a rse a p p ro a c h )
P ie zo e le c tricB im o rp h s(F in e a p p ro a c h )
T ip h o ld e r
G o ld tip
S am p le h o ld e r
S am p le
3 H e pot
Our Experiment: Cantilever-Andreev-Tunneling (CAT) rig
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0
0 2
0 2
Wexler's Formula ( )
, , Knudsen ratio
) 1, ( ) 0.694
4 , Sharvin (Ballistic) limit
3) 0
Proc. Phys. Soc. 89, 927
, 1
,
(196
4 31
3 8
)
2
6
M
e
eSharvin
Maxwell
e K l a
i K K
lR R
aii
lR K
a
K K
Ra
K
R
axwell (Diffusive) limit
2aI I
Basics of PCS: Contact Regimes
Length scales2a: contact sizelel: elastic mean free pathlin: inelastic mean free pathx: coherence length
Therefore, our experiments are in the ballistic, Sharvin Limit, required for good spectroscopy
For our experiment:
* Upper limit of 2a = 46 nm
* lel at Tc= is 81 nm (from thermal conductivity), and
increases with decreasing T, to 4-5 µm at 400mK.
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-2 -1 0 1 2
1.0
1.5
2.0
0.400.600.80
0.981.12
1.311.521.631.751.861.972.07
T(K)
60.050.0
40.0
30.0
20.0
10.0
5.0
2.602.242.15
Nor
mal
ized
Con
duct
ance
Voltage (mV)
DATA: Dynamic Conductance of Au/CeCoIn5
T*
Tc
Background develops an asymmetry at the heavy-fermion liquid coherence temperature, T* ~ 45 K, gradually increasing with decreasing temperature to the onset of superconducting coherence, Tc =2.3 K.
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Normalization by dividing each G-V data by normal state (2.6K) G-V data
-2 -1 0 1 2
0.9
1.0
1.1
2.60
0.40
N
orm
aliz
ed C
ondu
ctan
ce
Voltage (mV)
T (K)
0.60 0.80 0.98 1.12 1.31 1.52 1.63 1.75 1.86 1.97 2.07 2.15 2.24
Background Normalization
-2 -1 0 1 2
1.00
1.05
1.10
1.15
Nor
mal
ized
Con
duct
ance
Voltage (mV)
T(K) 0.40 0.60 0.80 0.98 1.12 1.31 1.52 1.63 1.75 1.86 1.97 2.07 2.15 2.24 2.60
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B
(0) 404μeV
2 (0)4.08
k cT
Strong Coupling
BUT: Decreasing with decreasing T: Not physically meaningful
-2 -1 0 1 2
2.60K
13
.3%
2.24K
2.15K
2.07K
1.97K
1.86K
1.75K
1.63K
1.52K
1.31K
1.12K
0.98K
0.80K
0.60K
0.40K
No
rma
lize
d C
on
du
cta
nce
(a
rb. u
nit)
Voltage (mV)
s-wave fit
0.0 0.5 1.0 1.5 2.0 2.50
100
200
300
400
D (
T),
G (
T)
(m
eV
)
Temperature (K)
D(T)
G(T)
BCS energy gap
G=349(1-t3) meV
Z=0.346
Γ(T)Δ(T)
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s-wave d-wave
Z 0.346 0.215
(eV) 384 460
(eV) 305 220
Fitting Parameters
24.64
B ck T
strong coupling
d-wave fit
-2 -1 0 1 2
1.00
1.04
1.08
1.12 Exp. s-wave d
x2-y2-wave
d-wave vs. s-wave fitting
T=400mKH=0G
G(V
) / G
(-2m
V)
Voltage (mV)
BUT AGAIN, decreasing with decreasing T (like s-wave case): So again, Not physically meaningful
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Zero-bias Conductance Fit (one point)
Constant Γ : Supportive of d-wave pairing symmetry, consistent with literature
218 eV(t) = 0.86(0) x (1-t3/3)
(T, ) =(T)cos(2), (T) = 2.35kBTc x tanh(2.06(Tc/T-1)1/2)
(0) = 349 eV, (T): BCS energy gap
0.3650.346Z
d-waves-wave
Fitting Parameters
0.0 0.2 0.4 0.6 0.8 1.01.00
1.05
1.10
1.15
Nor
mal
ized
ZB
C
T / Tc
exp. data s-wave fit d-wave fit
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Similar AR magnitudes: Common in N/HFS
G. Goll et al., PRL 70, 2008 (1993)
Yu. G. Naidyukv et al., Europhys Lett. 33, 557 (95).
URu2Si2-Pt
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-4 -2 0 2 40.21
0.22
0.23
0.24
0.25
0.26
0.27
0.28
T = 0.41 KH = 0 G
Conductance of [110]CeCoIn5-Au point contact
d
I/dV
(-1
)
Voltage (mV)
VERY NEW DATA: PCS on 110-orientation: Spectroscopic proof of d-wave ??? (work in progress):
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-4 -2 0 2 4
0.9
1.0
1.1
1.2
1.3
1.4
1.5
1.6
2.58 K
2.16 K
2.03 K
1.93 K
1.76 K
1.57 K
1.38 K
1.17 K
1.02 K
0.88 K
0.65 K
0.41 K
Normalized conductance of [110]CeCoIn5-Au point contact
G(V
) / G
(-5
mV
)
Voltage (mV)
-4 -2 0 2 4
1.0
1.1
1.2
1.3
1.4
1.5
1.6
2.58 K
2.16 K
2.03 K
1.93 K
1.76 K
1.57 K
1.38 K
1.17 K
1.02 K
0.88 K
0.65 K
0.41 K
Normalized conductance of [110]CeCoIn5-Au point contact
G(V
) / G
(-5
mV
)
Voltage (mV)
Temperature Dependence: Can normalize as the c-axis data
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-4 -2 0 2 40.98
1.00
1.02
1.04
1.06
1.08
1.10
1.12
T = 0.41 KH = 0 G
Normalized conductance of [110]CeCoIn5-Au point contact
N
orm
aliz
ed
Co
nd
uct
an
ce
Voltage (mV)
Note magnitude of Andreev signal is the SAME as for the (001) PCS!
This supports:A) Intrinsic property (reproducibility indicates not a “barrier” effect)
B) Sharvin limit
Shape supports d-wave: May be 1st spectroscopic evidence.
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BTK Conductance: s-wave vs. d-wave
work in progress…
-4.0 -2.0 0.0 2.0 4.00
1
2
3
4
5
RNd
I/dV
E /
Z=0 Z=0.5 Z=1 Z=5
d-wave: ab-plane
-4 -2 0 2 4
0
1
2
E/E/
E/
RNdI
/dVZ=0.0
RNdI
/dV
E/-4 -2 0 2 4
0
1
2
Z=0.5
-4 -2 0 2 40
1
2
Z=1.5
RNdI
/dV
RNdI
/dV
-4 -2 0 2 40
2
Z=5
d-wave: c-axis
-4 -2 0 2 40
1
2
E/E/
E/
RNdI
/dVZ=0.0
RNdI
/dV
E/-4 -2 0 2 4
0
1
2
Z=0.5
-4 -2 0 2 40
2
4
Z=1.5
RNdI
/dV
RNdI
/dV
-4 -2 0 2 40
2
4
6
8
Z=5
s-wave
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Models which address the observation of AR at HFS/N Interface
1. Deutscher and Nozières, PRB 50, 13577 (1994)
From PCS of N/HFS, it has been common to obtain conductance curves corresponding to low Zeff value.
Deutscher and Nozières’ argument: “The boundary condition at the interface involves Fermi velocities without mass-enhancement factors.”
2. N. A. Mortensen et al., PRB 59, 10176 (2000)
Mismatch of Fermi Momenta combined with the two-fluid model of Nakatsuji, Pines & Fisk causes strong effect on tunneling cone. Zeff must be calculated for each component.
This effect can explain ZBC normalized to normal state conductance, but not to high-bias conductance.
3-Dimensional System
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Breakdown of the Andreev Approximation
Retro-reflection whenever D << EF (Andreev approximation).
If D/EF is non-negligible, the hole does not trace back the electron trajectory exactly (breakdown of Andreev approx.).
3. A. Golubov and F. Tafuri, PRB 62, 15200 (2000)
2 2, , 1 in N 1 in S e h FN F FS Fk k k Ek E EE
0 1 2 3 45
6 A
B CD
N S
-q - q -
Dq +-q + k +k --k --k +
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Energy-Dependent QP Lifetime
4. F. B. Anders and K. Gloos, Physica B 230-232 437 (1997)
Causes a reduction in gap energy (renormalization due to the strongly reduced QP spectral weight) Causes asymmetry: with the emergence of coherent heavy quasi-particles
2eV
N S
HL HR
HT
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1. Clean dynamic conductance data are measured between 60 K and 400 mK across HFS/N (CeCoIn5/Au) nano-scale junctions
2. Careful investigations show the contact is in the Sharvin limit.
3. Existing models cannot adequately describe the particle-hole Andreev conversion process at the HFS/N interface.
4. The low-temperature (400mK) conductance curve is consistent with strong coupling and the temperature-dependence of a single point, the zero-bias conductance, is consistent with a d-wave order parameter symmetry, both conclusions consistent with the literature for CeCoIn5.
5. We propose that systematic corrections to the BTK model that go beyond the breakdown of the Andreev approximation and re-normalized Fermi momenta may provide a framework for our future understanding of Andreev reflection at the N/HFS interface.
6. Recent (110) data may be spectroscopic evidence for d-wave
Conclusions
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Biscuits
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2
2
/
n
F
TT
Tl v
l T
Is the Contact in Sharvin Limit?
Thermal Conductivity
R. Movshovich et al., PRL 86, 5152 (2001)
• Contact Size, d O ~ 500 Å using Wexler’s formula with RN=R0(1+Z2), RN ~ 1 , Z ~ 0.35, Tc ~ 3.1 cm• 0 ~ 82Å• lel ~ 4-5 mm, lin ~0.65 mm @400mK• 0 < d << lel, lin Contact is ballistic, even if considering reduced l in point contact
Scattering Rate from Microwave Conductivity
R. Ormeno et al., PRL 88, 047005 (2002)
/ ~ 0.6 @45 μ 00 mKm inelasticl
0 1 2
0.1
1
10
Mea
n F
ree
Pat
h (m
m)
Temperature (K)
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How can we explain the background conductance?
Nakatsuji, Pines, Fisk, PRL 92, 016401 (2004)
Relative weight of HF fluid f(T) = f(0)(1-T/T*), T* ~ 45 K Kondo impurity fluid Coherent heavy-fermion fluid Saturating to 0.9 below ~ 2K
Enhanced asymmetry due to DOS change (shift of spectral weight toward Fermi energy) with increasing HF fluid?
Particle-hole asymmetry due to different kinetic energies in HFL?
“The pseudo-gap at T*, arising from the formation of the heavy quasi-particles in the coherent state, asymmetrically increases the resistance of the contact.” (K. Gloos et al., JLTP 105,37 (1996))
2q m E
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-4 -2 0 2 4
0.85
0.90
0.95
1.00
1.05
1.10
1.15 0.41 K0.65 K0.88 K1.02 K1.17 K1.38 K1.57 K1.76 K1.93 K2.03 K2.16 K2.58 K
Normalized conductance of [110]CeCoIn5-Au point contact
G(V
) / G
(-5
mV
)
Voltage (mV)
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-4 -2 0 2 4
0.9
1.0
1.1
1.2
1.3
1.4
1.5
T = 0.42 K
9 T
8 T
7 T
6 T
5 T
4 T
3 T
2 T
1 T
0 T
Field dependence of normalized conductance in [110] CeCoIn
5-Au point contact
G(V
) / G
(-m
V)
Voltage (mV)
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0 1 2 3 4
0.160
0.165
0.170
0.175
0.180
Zero-bias conductance of [110]CeCoIn5-Au point contact
Ze
ro-b
ias
Co
nd
uct
an
ce
Temperature (K)
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0.0 0.2 0.4 0.6 0.8 1.01.00
1.02
1.04
1.06
1.08
1.10
1.12
Normalized zero-bias conductance of [110]CeCoIn5-Au point contact
No
rma
lize
d Z
BC
T / Tc
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Heating Effect?
-2 -1 0 1 2
0.9
1.0
1.1
-1 0 1 2
after normalizationbefore normalization
400 mK 2.6K
Nor
ma
lized
Co
ndu
cta
nce
Voltage (mV)
400 mK 2.6K
• Local minima not intrinsic but caused due to incomplete match of BC
• No minima in un-normalized data
• No heating effect due to non-ballistic contact Sharvin contact!
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Non-Ballistic Point Contact
K. Gloos et al., JLTP 105, 37 (1996)
R = RA + RMAX
In N/HFS point contact, Maxwell resistance dominates since the resistivity of HFS is large.
CeCoIn5 has relatively small resistivity ( ~ 3.1 cm) and extremely long electron mean free path at low temperatures. Sharvin(ballistic) point contact could be formed
82//a,b 53//c
90
77
190
120//a,b 140//c
95
75//a, 130//c
(Å)
~ 10
3
~ 10
~ 2
~ 13
~ 2
~ 6
l/
810
270
720
470
1600
165
440
l (Å)
2.3
0.5
2
1
0.48
0.87
1.20
Tc(K)
3.5, 36.366UPd2Al3
1.5-65380CeCu2Si2
3.183CeCoIn5
3048UNi2Al3
0.27//c 0.45//b
180UPt3
43260UBe13
11140URu2Si2
0 (cm)m*/m0HFS
Properties of Heavy-Fermion Superconductors
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The Four Questions
1. Is the contact ballistic, diffusive, or thermal? (A: Ballistic: we have shown the Sharvin Limit)
2. How can we explain the background conductance shape? We observe a change in asymmetry at T*
3. What is the Pairing symmetry? (s-wave or d-wave) fit the data using extended BTK models
4. Why is the enhancement of sub-gap conductance so small? (~13.3% @ 400mK, NOT 100% as in conventional SCs) explore various possibilities…
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Models to account for observaion of AR at HFS/’N Interface
50
7
0
9.74 10 , 83
1 8.08 1083,
1.
1 1, , (1 )
73
1
0.28
F F ef
F eff
F
F
FS
f
N
f
ef
v cm s m m
z v cm s
vr
v v zz
v
m m
Z
: effective
:
qu
ve
asip
loci
article velocity
: renormalization fact
t
or
y
F F
F
F
v v z
v
z
v
Deutscher and Nozières, PRB 50, 13577 (1994)
2 2 1/ 2
8
55
,
[ (1 ) / 4 ] , /
1.40 10 / , for Au
9.7
Ac
4 10 / , for CeCoIn
.
cording to BTK model
6, tunneling regi
No AR expected to be observed in N/HFS contacts
meeff
eff FN FS
FN
FS
Z
Z Z r r r v v
v cm s
v cm s
From PCS of N/HFS, it has been common to obtain conductance curves corresponding to low Zeff value.
Deutscher and Nozières’ argument: “The boundary condition at the interface involves Fermi velocities without mass-enhancement factors.”
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Quantum Critical Point & Phase Diagram
V. A. Sidorov et al., PRL 89, 157004 (2002)
P. G. Pagliuso et al., Physica B 312-313, 129 (2002)
• Coexistence of AFM & SC
• Similar to cuprates
Ce(Co,Rh,Ir)In5
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PCS in Sharvin limit
- contact resistance independent of materials’ resistivities
- in practical situation, heterogeneous contact
d l1, l2
2
2
16 31
16
3
3
8e
e
PC
lR K
d K
l
d d
Yu. G. Naidyuk and I. K. Yanson, J. Phys.: Condens. Matter 10, 8905 (1998)
Calculated Resistance of Point-Contact
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2
2
/
n
F
TT
Tl v
l T
Is the Contact in Sharvin Limit?
Thermal Conductivity
R. Movshovich et al., PRL 86, 5152 (2001)
• Contact Size, d O ~ 500 Å using Wexler’s formula with RN=R0(1+Z2), RN ~ 1 , Z ~ 0.35, Tc ~ 3.1 cm• 0 ~ 82Å• lel ~ 4-5 mm, lin ~0.65 mm @400mK• 0 < d << lel, lin Contact is ballistic, even if considering reduced l in point contact
Scattering Rate from Microwave Conductivity
R. Ormeno et al., PRL 88, 047005 (2002)
/ ~ 0.6 @45 μ 00 mKm inelasticl
0 1 2
0.1
1
10
Mea
n F
ree
Pat
h (m
m)
Temperature (K)
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Andreev Reflection
A. F. Andreev, Sov. Phys. JETP 19, 1228 (1964)
0 0
2
2
ˆ ˆ
For energies of the order of , the medium is
compl with an accuracyetely homogeneous ( )
Then, set
,
w
( / 2 ) ( ) ,
( / 2 ) ( )
( ), (
e
h re
)
F
ip n r i t ip r
F
n i t
i f t m f i r
i t m i r f
f e
E
E
r e r
0
1 2
1 2 30 0
1
0
ˆ
2
is the Fermi momentum and and are slowly
varing functions compared with .
, ( ) 0
,
where
(2 )
1 0
0 1
ˆ ˆ,
(
)
ik r ik r
ip n r
p
e
z r
R
A e B e
k n v k n v
f p T d e
,
where 2 1.
T
cH H
Thermal resistance of Sn in intermediate state
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/
/
ikx iEt
ikx iEt
f ue
g ve
Assume x)=V(x)=0, D(x)=D
Plane wave solutions
2 2
2 2
2
2
k
m u uE
v vk
m
Bogoliubov-de Gennes Equations
2 for N ( =0)q m E
22 22 2
2
kE
m
2 2
2 1E
k m
Solving for E, u, v
2 22 21
1 12
Eu v
E
2 22 20 0
11 1
2
Eu v
E
(u0 > v0)
22
22
( ) ( ) ( , ) ( ) ( , )2
( ) ( ) ( , ) ( ) ( , )2
fi x V x f x t x g x t
t m
gi x V x g x t x f x t
t m
Excitations in a superconductor
Four types of QP waves for given E
0 0
0 0
( )Defining ,
( )
, ik x ik x
k k
f x
g x
u ve e
v u
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Suggestions For Theoretical Study
The following issues need to be investigated carefully.
Mismatch in Fermi parameters: effective mass, momentum, velocity
Anisotropy: order parameter, layered structure, Fermi surface
Emergent heavy quasiparticles, two fluid model
Quasiparticle scattering rate in AR process across N/HFS interface
Length scales for electrostatic potential, order parameter, effective mass, etc., in terms of coherence lengths both in a normal metal and in a superconductor
Successful model should explain the following experimental features.
Concomitance of asymmetry in background conductance with emergent heavy-fermion liquid
Suppressed Andreev reflection to quantify the full conductance curve
Possible shrinking(?) of the conductance curve
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2
2 22
2 2
2
2 2
2
cos1
1 sincos4coscos1
( 1), original BTK thoery
4
sin1 sin
v
keff
k v
k
veff
v
rZ Z
r
rrZ
Zr r
r
S1
conserv. of parallel momenta
,
sin sin ,
, 2
1sin , critical angle
FN FNk v
FS FS
FN N FS S
N ck
k vr r
k v
k k
ifr
Mismatch of Fermi Momenta
N. A. Mortensen et al., PRB 59, 10176 (2000)
3-Dimensional System
This effect can explain the suppression of ZBC normalized to normal state conductance, but not to high-bias conductance.
If the superconductor is inhomogeneous as in the two-fluid model (Nakatsuji, Pines & Fisk), we can define different Zeff for each component. We’re exploring this possibility.
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Breakdown of Andreev Approximation
Retroreflection whenever << EF (Andreev approximation).
If /EF is non-negligible, the hole does not trace back the electron trajectory exactly (breakdown of Andreev approx.).
This happens in layered structures, too.
A. Golubov and F. Tafuri, PRB 62, 15200 (2000)
2 2, , 1 in N 1 in S e h FN F FS Fk k k Ek E EE
0 1 2 3 45
6 A
B CD
N S
-q - q -
Dq +-q + k +k --k --k +
0.285.321.59.25Nb
~ 2.0~ 12090YBCOCuprate
2.3
39
7.20
1.18
Tc(K)
0.5
1.2 – 1.8
5
0.4-0.62.4
7.0
MgB2
Two-band
0.149.471.35Pb
~ 2.1~ 0.0220.46CeCoIn5HFS
0.01511.70.175AlElemental
/EF (%)EF(eV)(meV)ExampleSC type
Ratio of Gap Energy to Fermi Energy of Superconductors
Layered N / isotropic S
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d-wave BTK Conductance
along c-axis
-4 -2 0 2 40
1
2
E/DE/D
E/D
RNdI
/dVZ=0.0
RNdI
/dV
E/D-4 -2 0 2 4
0
1
2
Z=0.5
-4 -2 0 2 40
1
2
Z=1.5
RNdI
/dV
RNdI
/dV
-4 -2 0 2 40
2
Z=5
-4.0 -2.0 0.0 2.0 4.00
1
2
3
4
5
RNdI
/dV
E / D
Z=0 Z=0.5 Z=1 Z=5
along ab-plane
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MgB2 PCS
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-25 -20 -15 -10 -5 0 5 10 15 20 250.25
0.30
0.35
0.40
0.45
0.50
0.55
T = 1.52 K
MgB2- #9 (ASU)-3rd contact
M04020 (STI)
Conductance of ion-irradiated MgB2-Au point contact
May 25, 2005
dI/d
V (-1
)
Voltage (mV)
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-25 -20 -15 -10 -5 0 5 10 15 20 250.9
1.0
1.1
1.2
1.3
1.4
1.5
1.6
1.7
1.8
T = 1.52 K
MgB2- #9 (ASU)-3rd contact
M04020 (STI)
Normalized conductance of ion-irradiated MgB2-Au point contact
May 25, 2005
G(V
) / G
(-2
5m
V)
Voltage (mV)
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-10 -5 0 5 10 150.00
0.05
0.10
0.15
0.20
0.25
T = 1.50 K
MgB2-9 (ASU)-5th contact (initial)
M04020 (STI)
Conductance of ion-irradiated MgB2-Au point contact
May 25, 2005
dI /
dV
(-1
)
Voltage (mV)
![Page 55: Andreev reflection at the CeCoIn 5 Heavy Fermion Superconductor Interface Wan Kyu Park and Laura H. Greene UIUC John L. Sarrao and Joe D. Thompson LANL](https://reader037.vdocuments.us/reader037/viewer/2022103123/56649d4b5503460f94a2972d/html5/thumbnails/55.jpg)
-20 -15 -10 -5 0 5 10 15 200.09
0.10
0.11
0.12
0.13
T = 1.51 K
MgB2- #9 (ASU)-5th contact (final)
M04020 (STI)
Conductance of ion-irradiated MgB2-Au point contact
May 25, 2005
G(V
) / G
(-2
0m
V)
Voltage (mV)
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-20 -15 -10 -5 0 5 10 15 20
1.0
1.1
1.2
1.3
1.4
T = 1.51 K
MgB2- #9 (ASU)-5th contact (final)
M04020 (STI)
Normalized conductance of ion-irradiated MgB2-Au point contact
May 25, 2005
G(V
) /
G(-
20
mV
)
Voltage (mV)
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-20 -15 -10 -5 0 5 10 15 20
1.0
1.1
1.2
1.3
1.4 MgB2- #9 (ASU)-5th contact (final)
M04020 (STI)
1.51 K 6.41 K 11.10 K 16.49 K 21.67 K 26.69 K 31.72 K 36.70 K 39.30 K
Normalized conductance of ion-irradiated MgB2-Au point contact
May 25, 2005
G(V
) / G
(-2
0m
V)
Voltage (mV)
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0 5 10 15 20 25 30 35 400.085
0.090
0.095
0.100
0.105
0.110
0.115
Zero-bias conductance of MgB2-Au point contact
MgB2- #9 (ASU)-5th contact (final)
M04020 (STI)May 25, 2005
Ze
ro-b
ias
con
du
cta
nce
(
)
Temperature (K)