organic superconductors at extremes of high magnetic field organic superconductors at extremes of...
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Organic SuperconductorsAt Extremes of High Magnetic FieldOrganic SuperconductorsAt Extremes of High Magnetic Field
C. H. MielkeLos Alamos National LaboratoryNational High Magnetic Field Laboratory
Organic SuperconductorsAt Extremes of High Magnetic Field
C. H. MielkeLos Alamos National LaboratoryNational High Magnetic Field Laboratory
NHMFL
NHMFL Magnetic Field Capabilities
• Explosively Driven– 145 T flux compression generator (~3 kg detasheet)– 800-1000 T fcg cylindrical symmetry (~20 kg HMX-9501)– 300 T Capacitor Driven exploding coils
• Controlled Waveform 90 MJ (650 MJ max)– 60T 2 second controlled waveform– 100T CW outsert CD insert 145 MJ (available 2004)
• Capacitor Driven 0.6-1.2 MJ (1.6 MJ max)– 60T “short pulse” 6ms rise 40ms decay– 50T “mid-pulse” 40ms rise 300ms decay
• DC Superconducting Magnets (to 20T)
“Fowler” Flux compressors• Max field of ~180T
• 10mm to 20mm bore
• High homogeneity
• Sample & cryostat are destroyed
• 3 kg of sheet explosive140
120
100
80
60
40
20
0100x10
-6806040200
Time (seconds)
10MT/s
5
0
-5
-10
• Explosively Driven– 145 T flux compression generator (~3 kg detasheet)– 800-1000 T fcg cylindrical symmetry (~20 kg HMX-9505)– 300 T Capacitor Driven exploding coils
• Controlled Waveform 90 MJ (650 MJ max)– 60T 2 second controlled waveform– 100T CW outsert CD insert 145 MJ (available 2004)
• Capacitor Driven 0.6-1.2 MJ (1.6 MJ max)– 60T “short pulse” 6ms rise 40ms decay– 50T “mid-pulse” 40ms rise 300ms decay
• DC Superconducting Magnets (to 20T)
NHMFL Magnetic Field Capabilities
Multi-Stage Flux Compression Generators
• Russian Design “MC1” FCG
• 800 to 1000 tesla
• 20 kg shaped explosive (PBX 9501) 95% HMX 9505 and 5% Plastic bonder
Multi Stage Flux Compression
800
600
400
200
0
Magnetic Field Intensity (tesla)
74x10-6
706866646260
Time (seconds)
First Cascade Accelerates
Second Stage Fuses
Shock Wave Hits
MC-1 Flux Compression GeneratordB/dT ~ 150 MT/sec
• Explosively Driven– 145 T flux compression generator (~3 kg detasheet)– 800-1000 T fcg cylindrical symmetry (~20 kg HMX-9505)– 300 T Capacitor Driven exploding coils
• Controlled Waveform 90 MJ (650 MJ max)– 60T 2 second controlled waveform– 100T CW outsert CD insert 145 MJ (available 2004)
• Capacitor Driven 0.6-1.2 MJ (1.6 MJ max)– 60T “short pulse” 6ms rise 40ms decay– 50T “mid-pulse” 40ms rise 300ms decay
• DC Superconducting Magnets (to 20T)
NHMFL Magnetic Field Capabilities
60
50
40
30
20
10
02.01.51.00.50.0
Time (seconds)
NHMFL 60 tesla controlled waveform magnet
100 ms flat top 200 ms flat top Stepped fiels (Specific Heat Experiments)
Specific Heat in a Kondo InsulatorJaime, et al, Nature 405 (2000) 160
60 minutes between full field shots
1.4 GW motor-generator
1m90 MJ of energy
• Explosively Driven– 145 T flux compression generator (~3 kg detasheet)– 800-1000 T fcg cylindrical symmetry (~20 kg HMX-9505)– 300 T Capacitor Driven (CD) exploding coils
• Controlled Waveform (CW) 90 MJ (650 MJ max)– 60T 2 second controlled waveform– 100T CW outsert CD insert 145 MJ (available 2004)
• Capacitor Driven 0.6-1.2 MJ (1.6 MJ max)– 60T “short pulse” 6ms rise 40ms decay– 50T “mid-pulse” 40ms rise 300ms decay
• DC Superconducting Magnets (to 20T)
NHMFL Magnetic Field Capabilities
Specifications
Outer Coil (125 MJ peak energy) (Department of Energy)
Coils 1 through 4 AL-60 Conductor 301 SS Sheet Reinforcement wound on Nitronic-40 bobbin
Coils 5 and 6 AL-15 Conductor Nitronic-40 Monolithic Reinforcement
Coil 7 Hard Cu Conductor 304 SS Monolithic Reinforcement
One Meter
Design and Materials
NHMFL’s 100 T Multi-Shot Magnet
100T peak field15mm borePulse every hour
1 msec at 100T peak field
2 secondtotal pulse duration
Insert Coil (2 MJ peak energy) (National Science Foundation) CuNb Conductor MP35N Sheet Zylon Fiber Reinforcement
10 msec above 75T
140 MJ of energy
• Explosively Driven– 145 T flux compression generator (~3 kg detasheet)– 800-1000 T fcg cylindrical symmetry (~20 kg HMX-9505)– 300 T Capacitor Driven exploding coils
• Controlled Waveform 90 MJ (650 MJ max)– 60T 2 second controlled waveform– 100T CW outsert CD insert 145 MJ (available 2004)
• Capacitor Driven 0.6-1.2 MJ (1.6 MJ max)– 60T “short pulse” 6ms rise 40ms decay– 50T “mid-pulse” 40ms rise 300ms decay
• DC Superconducting Magnets (to 20T)
NHMFL Magnetic Field Capabilities
60 tesla “short pulse”
• ~6 milli-seconds to peak field
• Work-horse of the magnet lab
• Life-time of ~500 full field shots
10 cm
30 minutes between full field shots
0.6 MJ of energy
Normal Mode of Failure
• Causes minor damage– He dewar tail– Probe insert– LN2 bucket (igloo cooler)
• Fault on lead end or sometimes in the 3rd layer midplane (due to fatigue of conductor)
• Audible report
Short Pulse Stress Failure
60 tesla magnet destroyed at 72 tesla “confinement failure”
0.8 MJ of energy
Worth the hassle for condensed matter physics
• Extreme fields quantize quasi-particle orbits
• Split Energy Bands
• Suppress Superconductivity
• Drive magnetic transitions
• Reveal new states of matter
• Ect., ect., etc….
5.0x10-8
4.5
4.0
3.5
3.0
6050403020100
Magnetic Field (tesla)
α-( - )BEDT TTF 2 ( )KHg SCN4 = 400 T mK
rf contactless conductivityƒ = 28 MHz
10-4
10-3
10-2
10-1
100
6000500040003000200010000
Frequency (tesla)
β
β−αβ+α
4α
β−α
3α2α
α
Organic Superconductors
• First Organic Superconductor Discovered in 1979
• Initial Tc of ~1K– Q1-D salt
• Various categories– “Bucky Balls”– FET types– Charge transfer salts
TetraMethylTetraSelenaFulvalene
cloride Tc=1K
-BisEthyleneDiThio-TetraThioFulvalene
Copper ThioCynate Tc=10K
-BisEthyleneDiThioTetraThioFulvalene
copper DiCyanidBromide Tc=11.6K
-BisEthelyneDiThioTetraSelenaFulvalene
Gallium TetraClorate Tc= 5K
Charge Transfer Salts begin with organic radicals
BEDT-TTF based (ET for short)
BEDT-TSF based (BETS for short)S
Se
Se
S
Se
S
S
Se
H
HHH
S
S
S
S
S
S
S
S
H
HHH
Effect of the Inorganic Anion
Organic meets Inorganic-(BEDT-TSF)2GaCl4
Half of the unit cell
The Unit Cell
-(BEDT-TSF)2GaCl4 -(BEDT-TTF)2Cu(NCS)2
a = 18 Åb = 16 Åc = 8 Å
a = 16 Åb = 8 Åc = 13 Å
Layer spacing is the important dimension
packing motif packing motif
The Fermi Surfaces
β
α
Γ
M
k
kc
b
Y
-(BEDT-TSF)2GaCl4 -(BEDT-TTF)2Cu(NCS)2
Anisotropy of the Electronic System
-(BEDT-TTF)2Cu(NCS)2-(BEDT-TTF)2Cu(NCS)2
Molecular Corridor-(BEDT-TSF)2GaCl4
4
3
2
1
06050403020100
Field (tesla)
1.0
0.8
0.6
0.4
0.2
0.0800040000
Frequency (tesla)
αƒ=670 T
βƒ=4060 T
0.10
0.05
0.00
-0.05
-0.1026 10x -324222018
1/μ0 (H T-1)
-( - )BEDT TSF2GaCl4 = 430 T mK
Magnetic Breakdown in -(BEDT-TSF)2GaCl4
Magnetic Breakdown in -(BEDT-TTF)2Cu(NCS)2
1.0
0.5
0.0
-0.5
36x10-3
34323028262422
Inverse Magnetic Field (T-1
)
T = 40 mK
T = 650 mK
Magnetic Breakdown1.0
0.8
0.6
0.4
0.2
0.01000080006000400020000
Frequency (tesla)
α = 600 T
β = 3990 Tβ − α
Pippard Magnetic Breakdownβ
α
Γ
M
k
kc
b
Y
Exponential Growth of Breakdown Amplitude
4x10-3
2
0
-2
-4
42x10-3
4038363432302826
Inverse Magnetic Field ( T-1
)
-( - )BEDT TTF 2 ( )Cu NCS4 Breakdown orbit digitally filtered = 40T mK
Forbidden Trajectories0.25
0.20
0.15
0.10
0.05
0.001000080006000400020000
Frequency (tesla)
β
β + α
β − α
β + 3αβ − 2α
-( - )BEDT TTF 2 ( )Cu NCS4
β − α α
Γ
Mk
k
Y
Anomalous Trajectories are due toStark Quantum Interference
β
α
Γ
M
k
kc
b
Y
Angular Dependent Magnetoresistance
Field Lines
PlatformSample
Rotation Axis
-(BEDT-TSF)2GaCl4
-(BEDT-TTF)2Cu(NCS)2
B = 42T (DC)
B
Belly orbits show salt to be more 3-D than
Quasi 2-D region w/B || layersPeak width is determinedby the interlayer transfer integral (t )
β
α
Γ
M
k
kc
b
Y
J. Singleton, et. al. PRL, 88 (2002).
t⊥λ ≈0.21meV
t⊥κ ≈0.04meV
C. Mielke, et. al. J. Phys. Cond. Mat., 13 (2001) 8325.
Tight-binding dispersion relation added to the effective dimer model
Using G-L theory to estimate z
302520151050
Magnetic Field (tesla)
H c2 c2H
H || planes
-( )ET 2 ( )Cu NCS4 -( )BETS 2GaCl4
Hc2⊥z =φ0
2πξxyξz
z ≈ 5Å
z ≈ 16Å
At T* ≈ 18 Å for -(BEDT-TSF)2GaCl4
10
2
3
4
5
6
7
89
100
43210
Temperature (K)
( ) ~ T (0)/(1 - )t1/2
4
5
6
7
89
10
2
3
4
5
Coherence Length (Å)
86420
Temperature (K)
-(BEDT-TTF)2Cu(NCS)2 appears to be in the 2-D limit so close to Tc we can’t resolve it
Superconducting Properties of -(BEDT-TSF)2GaCl4
and -(BEDT-TTF)2Cu(NCS)2
C. H. Mielke, J. Singleton, M-S Nam, N. Harrison, C.C. Agosta, B. Fravel, and L.K. Montgomery, J. Phys.: Condens. Matter, 13 (2001)8325.
6
5
4
3
2
1
01086420
Temperature (K)
-( )ET 2 ( )Cu NCS2
(Fit to Tc- )Tβ
β =0.73
λ-(BEDT-TSF)2GaCl4 Fit to (Tc-T)
β
β = 0.5 G-L theory 3D linear fit
Conclusions
• Creating very high magnetic fields can be exciting!
• By tuning the organic molecules the effective dimensionality of the system is readily changed
• Dimensionality is closely related to the superconducting properties
John Singleton (Oxford U. joining LANL in July)Ross McDonald (LANL Postdoctoral Fellow 3-D Fermi surfaces)Greg Boebinger, Dwight Rickel, Neil Harrison (LANL)Mike (L. K.) Montgomery (Indiana U. synthesis of organic SC) Department of Energy and the National Science Foundation