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An Electronic Primary Thermometer Based on Thermal
Shot NoiseLafe Spietz
K.W. Lehnert, R.J. Schoelkopf
Department Of Applied Physics, Yale University
Thanks to:
Michel Devoret, Dan Prober, Irfan Siddiqi,
Ryan Held
2ggC V
e0-0.5 0.5
n
300 mK400 mK500 mK600 mK
Coulomb Staircase T>T*
Motivation: Unfilled Need in Milikelvin Thermometry
Mystery kelvins!
OutlineI. Motivation, overview of thermometry
- Limitations of cryogenic thermometry and temperature metrology
II. Thermal-shot noise of tunnel junctions- How it makes a thermometer
III. Fabrication of devices: - Dolan bridge junction fab at Yale
IV. Demonstration of the thermometer from 0.01K to 300 K
V. Future work, possible limitations
Overview of low temperaturethermometry
• Johnson noise: Primary, slow, difficult, very wide range• Resistors: Secondary,can drift, can be field dependent, not good at very
low temperatures, cheap and fast• Nuclear orientation: Primary, expensive, very limited range, doesn’t work in
B field• 3He-4He vapor pressure: Primary, difficult, limited range• diodes: Secondary, not good below 1K• Capacitance: secondary, no B dependence, recalibrate on cycling• Paramagnetic salts: primary, limited range, B dependence
Primary vs. secondary
ITS 90: The Modern Kelvin
Plank radiation law
Platinum resistance thermometer
He gas thermometer
3He 4He vapor pressure
?
.6K
961.78K25K5K3K
Below .6K
undefined!
T90 :
triple point of water = 273.16 K(T90 )
273.16K
Fundamental Noise SourcesJohnson-Nyquist Noise
• Frequency-independent• Temperature-dependent• Used for thermometry
• Frequency-independent • Temperature independent
( ) 2IS f eI
4( ) bI
k TS f
R
2A
Hz
2A
Hz
Shot Noise
Johnson Noise Thermometry
Limited by calibration of gain and bandwidth--very hard, limits bandwidth, and hence speed.
P = GB(SIamp + 4kT/R)
G B PR
Conduction in Tunnel Junctions
Assume: Tunneling amplitudes and D.O.S. independent of Energy
V
I
~ (1 )
~ (1 )
l r l r
r l r l
I f f dE
I f f dE
l r r lI I I Difference gives current:
Thermal-Shot Noise of a Tunnel Junction*
( ) 2 coth2I
b
eVS f eI
k T
Sum gives noise:
( ) 2 ( )I l r r lS f e I I
*D. Rogovin and D.J. Scalpino, Ann Phys. 86,1 (1974)
Thermal-Shot Noise of a Tunnel Junction
( ) 2 coth2I
b
eVS f eI
k T
Self-Calibration Technique
8
~ 10B Hz41
~ 10P
P B
( ( , ))
2,
( , )( , ) (2 )
AmpI IP GB S S V T
e
R
dS V TdP V T d eIIGBdV dVdV
For = 1 second
For eV>>kT
Hence can remove GB.
Thermometer Demonstration
T is measured without reference to unknown system parameters
1/ 20.6126... / bT e k V
1/ 2V
Silicon Substrate
PMMA
PMGI LOR
40 KeV Electrons
.7 m
1 m
E-Beam Lithography onBilayer
Silicon Substrate
PMMA
PMGI LOR
Independent Developers Create Undercut
SEM of Undercut
Silicon Substrate
PMMA
PMGI LOR
Create Suspended Bridges!
Device With Bridge
Silicon Substrate
PMMA
PMGI LOR
AluminumAluminum
Double Angle: 1st Evaporation
Silicon Substrate
PMMA
PMGI LOR
Aluminum +
Aluminum Oxide
Aluminum +
Aluminum Oxide
Oxidize to Create Barrier
Silicon Substrate
PMMA
PMGI LOR
AluminumAluminum
Double Angle:2nd Evaporation
Completed Junction Profile
The Finished Product(AFM)
The Measurement
Linear I-V
Good fit to theory:( ) 2 coth
2Ib
eVS f eI
k T
Calibrate off of shotnoise
Pshot = GB(Samp+2eI)
Comparison of normalized data to functional form
Comparison of normalized data to functional form over
wide range
Fit to extract temperature
Preliminary Results:Comparison to Oxford
Thermometer
Improvements, future work
Improve thermal contact to comparison thermometers
Compare against better thermometers
Investigate self-heating
Investigate precision limits—is this the new Kelvin?
4 wire measurement
Engineer for commercial distribution
Advantages and Disadvantages
*R. J. Schoelkopf et al., Phys Rev. Lett. 80, 2437 (1998)
Advantages
Fast and self-calibrating
Primary
Wide T range
No B-dependence
Measures electron temperature
Possibility to relate T to frequency!*
Disadvantages
Lead heating
Frequency dependence*
I(V) nonlinearities from:
Density of states
Barrier shape
Weak localization, etc
Summary
• Fundamental voltage and temperature dependent noise of a tunnel junction
(thermal-shot noise.)
• Makes fast, accurate thermometer which works over a wide temperature range
• Relates T to V using only e and kb implications for metrology