101 years of superconductivity kazimierz conder laboratory for developments and methods, paul...
TRANSCRIPT
PAUL SCHERRER INSTITUTPAUL SCHERRER INSTITUT
101 years of superconductivity
Kazimierz Conder
Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland
2
Temperature
Resi
stiv
ity Kelvin (1902)
Matthiessen (1864)
Dewar (1904)
Electrical resistivity at low temperatures
Kelvin: Electrons will be frozen – resistivity grows till .
Dewar: the lattice will be frozen – the electrons will not be scattered. Resistivity wiil decrese till 0.
Matthiesen: Residual resistivity because of contamination and lattice defects.
Hydrogen was liquefied (boiling point 20.28 K) for the first time by James Dewar in 1898
One of the scientific challenge at the end of 19th and beginning of the 20th century: How to reach temperatures close to 0 K?
Resistivity at low temperatures- pure mercury (could repeatedly distilled producing very pure samples).
•Repeated resistivity measurements indicated zero resistance at the liquid-helium temperatures. Short circuit was assumed!•During one repetitive experimental run, a young technician fall asleep. The helium pressure (kept below atmospheric one) slowly rose and, therefore, the boiling temperature. As it passed above 4.2 K, suddenly resistance appeared.
From: Rudolf de Bruyn Ouboter, “Heike Kamerlingh Onnes’sDiscovery of Superconductivity”, Scientific American March 1997
Hg TC=4.2K
1895 William Ramsay in England discovered helium on the earth 1908 H. Kamerlingh Onnes liquefied helium (boiling point 4.22 K)
Superconductivity- discovery I
4
Superconductivity- discovery II
•Liquid Helium (4K) (1908). Boiling point 4.22K.
•Superconductivity in Hg TC=4.2K (1911)
„Mercury has passed into a new state, which on account of its extraordinary electrical properties may be called the superconducting state“
H. Kamerlingh Onnes 1913 (Nobel preis 1913)
Resistivity R=0 below TC; (R<10-23 cm, 1018 times smaller than for Cu)
5
Further discoveries
1986 (January): High Temperature Superconductivity (LaBa)2 CuO4 TC=35K
K.A. Müller und G. Bednorz (IBM Rüschlikon) (Nobel preis 1987)
1987 (January): YBa2Cu3O7-x TC=93K
1987 (December): Bi-Sr-Ca-Cu-O TC=110K,
1988 (January): Tl-Ba-Ca-Cu-O TC=125K1993: Hg-Ba-Ca-Cu-O TC=133K
(A. Schilling, H. Ott, ETH Zürich)
1911-1986: “Low temperature superconductors” Highest TC=23K for Nb3Ge
6
1920 1940 1960 1980 20000
20
40
60
80
100
120
140
Cs2RbC
60
MgB2
LHe
Liquid nitrogen
HgBa2Ca
2Cu
3O
8
Tl2Sr
2Ca
2Cu
3O
10
Bi2Sr
2Ca
2Cu
3O
10
YBa2Cu
3O
7
La2-x
SrxCuO
4
Ba1-x
KxBiO
3
BaPb1-x
BixO
3
NaxWO
3NbO
Nb3Ge
Nb3SnNbN
NbPbHg
TC [
K]
Year
7
The current can flow 100 000 years!!
Zero resistivity
Low temperatures:LN2 -1960C (77K)
8
A superconductor is a perfect diamagnet. Superconducting material expels magnetic flux from the interior.
W. Meissner, R. Ochsenfeld (1933)On the surface of a superconductor (T<TC) superconducting current will be induced. This creates a magnetic field compensating the outside one.
Meissner-Ochsenfeld-effect
Screening (shielding ) currents
Magnetic levitation
9
Superconducting elements
•Ferromagnetic elements are not superconducting•The best conductors (Ag, Cu, Au..) are not superconducting •Nb has the highest TC = 9.2K from all the elements
10
Classical model of superconductivity
The lattice deformation creates a region of relative positive charge which can attract another electron.
An electron on the way through the lattice interacts with lattice sites (cations). The electron produces phonon.
1957 John Bardeen, Leon Cooper, and John Robert Schrieffer
During one phonon oscillation an electron can cover a distance of ~104Å. The second electron will be attracted without experiencing the repulsing electrostatic force .
John Bardeen, Leon Neil Cooper, John Robert Schrieffer
Nobel Prize in Physics 1972
"for their jointly developed theory of superconductivity, called the BCS-theory”
e-
e-
Phonon
Coherence length
Cooper pair model
12
Fermie und Bose-Statistic
•Total spin of C-P is zero. C-P are bosons. Pauli-Principle doesn’t obey.
•All C-P can have the same quantum state with the same energy.
Cooper-Pairs are created with electrons with opposite spins.
•Fermions- elemental particles with 1/2 spin (e.g. electrons, protons, neutrons..)
•Pauli-Principle –every energy level can be occupied with maximum two electrons with opposite spins.
Energy
Density of states
Energy
Density of states
A movement of the C-P when a supercurrent is flowing, is considered as a movement of a centre of the mass of two electrons creating C-P.
Creation of a C-Pairs diminishes energy of electrons. Breaking a pair (e.g. through interaction with impurity site) means increase of the energy.
All the C-P are in the same quantum state with the same energy. A scattering by a lattice imperfection (impurity) can not change quantum state of all C-P at the same time (collektive behaviour).
e-
e-
Phonon
14
Good electrical conductors are showing no superconductivity
In case of good conductors is the interaction of carriers with the lattice very week. This is, however, important for superconductivity.
BCS Theory: some consequences
Isotope effect
The Cooper-Pairs are created (“glued”) by the electron-phonon interaction. Energy of the phonons (lattice vibrations) depends on the mass of the lattice site . Superconductivity (Tc) should depend on the mass of the ions (atoms) creating the lattice.
TC~M-
For most of the low-temperature
superconductors =0.5
15
What destroys superconductivity?
High temperatures: strong thermal vibration of the lattice predominate over the electron-phonon coupling.
Magnetic field: the spins of the C-P will be directed parallel.
(should be antiparallel in C-P)
A current: produces magnetic field which in turn destroys superconductivity.
Current density
Temperature
Magnetic field
16
Coherence length
Coherence length is the distance between the carriers creating a Cooper-Pair.
GL
Superconductor
Concentration C-PISL SL
x< GL
Coherence length is the largest insulating distance which can be tunneled by Cooper-Pairs.
SC SC
(Xi)
"for his theoretical predictions of the properties of a supercurrent through a tunnel barrier, in particular those phenomena which are generally known as the Josephson effects".
Nobel Prize in Physics 1973
Brian David JosephsonJosephson discovered in 1963 tunnelling effect being 23-years old PhD student
The superconducting tunnel Josephson) junction (superconductor–insulator–superconductor tunnel junction (SIS) — is an electronic device consisting of two superconductors separated by a very thin layer of insulating material
ISL SL
x< GL
SC SC
18
Penetration depth
depicts the distance where B(x) is e-time smaller than on the surface
0
(T)=0*(1-(T/T
C)4)-0.5
TC
Ein
drin
gtie
fe
TemperaturTemperature
Pen
etra
tion
dept
h Superconductor
19
Ginzburg-Landau Parameter =/GL
Tc [nm] [nm]
Al 1.2 16 1600 0.01Sn 3.7 34 230 0.16Pb 7.2 37 83 0.4
<1/2=0.71 Superconductor Type I
Tc [nm] [nm]
Nb 9.3 39 38 1Nb3Sn 18 80 3 27YBa2Cu3O7 93 150 1.5 100Rb3C60 30 247 2.0 124Bi2Sr2Ca2Cu3O10 110 200 1.4 143
>0.71 Superconductor Type II
20
Superconductor type I (/GL<0.71) in a magnetic field
Bi=Ba+0
M
Superconductor Bi=0
Normal conductor Bi=Ba
Negative units !
The field inside the superconductor
The field created on the surface of the superconductor compensating the outside field
Outside field
Outside field BaOutside field Ba
Insi
de fi
eld
Bi
Mag
neti
zati
on
–μ
0M
21
Superconductor type II in a magnetic field
Vortex-lattice in superconductor type II. Magnetic flux of a vortex is quantized: 0=h/2e2.07·10-15Tm2
Bi=Ba+0M
Outside field Ba
Outside field Ba
Mag
neti
zati
on
–μ
0M
Avera
ge insi
de fi
eld
Bi
Meissner phase
Mixed phase
Normal condu-ctor
22
Superconductor type II. B-T-Diagram
Mixed phase
Meissner phase
Normal state
Temperature T
Mag
neti
c in
du
ctio
n B
STM (Scanning Tunneling Microscopy). Abrikosov-lattice in NbSe2
H. Hess, R.B. Robinson, and J.V. Waszczak, Physica B 169 (1991) 422
Alexei A. Abrikosov, Vitaly L. Ginzburg, Anthony J. Leggett
Nobel Prize in Physics 2003
"for pioneering contributions to the theory of superconductors and superfluids".
24
Type IIType I
25
Perovskite ABX3
X=O2-, F-, Cl-)A=alkali, alkali-earth and rare-earth metals, B=transition metals (also Si, Al, Ge, Ga, Bi, Pb…)
Perovskite is named for a Russian mineralogist, Count Lev Aleksevich von Perovski. The mineral (CaTiO3) was discovered and named by Gustav Rose in 1839 from samples found in the Ural Mountains.
X
A
B
26
La, Sr
Cu
O
0.0 0.1 0.2 0.310
100
La2-x
SrxCuO
4
Insu
lato
r
Met
al
An
tife
rro
ma
gn
et
Superconductor
TN
TC
Tem
pera
ture
[K]
Sr-content x, (holes per CuO2-layer)
2SrO 2Sr‘La + 2Ox
O + VO
VO+ 0.5O2 Ox
O+ 2h
(LaBa)2 CuO4 TC=35K K.A. Müller und G. Bednorz (IBM Rüschlikon 1986 )
High Temperature Superconductor. La2-
xSrxCuO4
27
CuO2 –layer
5-fold Cu coordination
CuO-chain
4-fold Cu coordination
BaO
Y
Perovskite
“YBa2Cu3O9
”
High Temperature Superconductor: YBa2Cu3O7-x
28
Oxygen doping in YBa2Cu3O7-x
6.0 6.2 6.4 6.6 6.8 7.00
20
40
60
80
100
Superconductor
YBa2Cu
3O
7-
Te
mp
era
ture
[K]
Oxygen content (7-)
TC
200 400 600 800 100098.5
99.0
99.5
100.0
YBa2Cu
3O
6.985
Oxy
gen
inde
x
Wei
ght
[%
]
Temperature [oC]
6.4
6.6
6.8
7.0
Thermogavimetry
Oxygen content depends on temperature and oxygen partial pressure
29
Layered structure of YBa2Cu3O7-x
Conducting CuO2 layers
Charge reservoir
holes
electrons
holes
2Cu2+ + 0.5O2 2Cu3+ +O2-
2CuxCu + V
O +0.5O2 2CuCu +
OxO
2CuCu 2Cux
Cu + 2h
Y
BaO
CuO
CuO2
Conducting CuO2 layers
30
YBa2Cu3O7 TC=93
ab [Å] c [Å] ab [Å] c [Å]
1500 6000 15 4
8.3Å
3.4Å
Bi2Sr2Ca2 Cu3O10 TC=110
ab [Å] c [Å] ab [Å] c [Å]
2000 10 000 13 2
Cooper-pairs can not tunnel through the charge reservoir!
For YBa2Cu3O7 single crystals at 4.2Kjc(ab)~107A/cm2, jc(c)~105A/cm2
Un
it c
ell
Layered structure of YBa2Cu3O7-x. Anisotropy
31
C a
C a
C a
C a
C a
C a
Bi2Sr2Ca2Cu3O10 2223TC=110K
Bi2Sr2CaCu2O8
2212 TC=95KBi2Sr2CuO6 2201TC=20K
Bi-Sr-Ca-Cu-O
BiO
SrOCuO2 Ca
BiO
32
HgBa2Can-1CunO2n+2 “Hg-12(n-1)n”
1 2 3 4 5 6 7
90
100
110
120
130
140
Te
mp
era
ture
[K
]
Number of CuO2-layers in the unit cell
TC für HgBa2Can-1CunO2n+2
Hg-12(n-1)n
CuO2-layers
World record 133K !!!ETH Zürich - A.Schilling, M.Cantoni, J.D. Guo, H.R.Ott, Nature, 362(1993)226
33
Sm TC=55K
April, 2008
Magnetic ion in the structure
Cs0.8(FeSe0.98)2
FeSe
CsIntercalation
K0.8(FeSe0.98)2
Cs0.8(FeSe0.98)2
Crystal growth in Cs (or K)- vapour in quartz ampoules at 1050oC
New superconductor Lix(C5H5N)yFe2-zSe2
arXiv:1206.7022
Synthesis of a new alkali metal-organic solvent intercalated iron selenide superconductor with Tc≈45K
A. Krzton-Maziopa, E. V. Pomjakushina, V. Yu. Pomjakushin, F. von Rohr, A. Schilling, K. Conder
Synthesized via intercalation of dissolved alkaline metal (Li) in anhydrous pyridine at room temperature.
C5H5N
36
USOUS
OUnidentified Superconducting
Object
37American Superconductor
Extrusion
Abfüllen in Silberröhrchen und Schweissen
Extrusion
Walzen und Erhitzen bei800-900oC
c ab
Applications. Wires and bands.
38
Applications. Wires and bands.
Cross section of HTC
band
American Superconductor Corporation
HTC Cable
39
Application. Industry.
MagLev – train (magnetic levitation)
SMES: Superconducting Magnetic Energy StorageSaves energy in form of magnetic field produced by a superconducting coil.
Magnetic bearing
A flywheel in a vacuum chamber – energy accumulator.
Summary
•History of discovery and farther development•How it works (still open problem for HTc)•What are the materials•Potential applications
A spin of a Cooper pair is:
1/21
2 0
Most of the HTc superconductors are:
Cuprates Nickelates
Cobaltates Manganates
Superconductors type II in comparison to type I:
have shorter coherence length and longer penetration depth
have shorter coherence length and shorter penetration depth
are cuprates (all other superconductors are type I)
have longer coherence length and shorter penetration depth
In the BCS theory it is assumed that the interaction between electrons in Cooper pairs is mediated by:
photons Coulomb force
phonons magnetic interaction
Vortex phase is observed:
For all superconductors type I Only in cuprates
For all superconductors above Tc
For all superconductors type II
Isotope effect (Tc dependence on lattice mass) is:
a proof of BCS theory (electron-phonon interaction)
a proof that superconductor is of type II
only observed for hole doped superconductors
not observed in superconductors
In case of many High Temperature superconductors in order to achieve temperatures below Tc one can use:
Ice+water Liquid nitrogen
Dry ice (solid CO2-
sublimation at −78.5 C)
No cooling is necessary