Reduction of low-frequency 1/f noise in Al-AlOx-Al tunnel junctions ...
Reduction of low-frequency 1/f noise in Al-AlOx-Al tunnel junctions ...
Reduction of low-frequency 1/f noise in Al-AlOx-Al tunnel junctions ...
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Juhani Jul<strong>in</strong>, Panu Kopp<strong>in</strong>en, Ilari Maasilta<br />
juhani.jul<strong>in</strong>@phys.jyu.fi<br />
arXiv:1006.3162<br />
<strong>Reduction</strong> <strong>of</strong> <strong>low</strong>-<strong>frequency</strong><br />
1/f <strong>noise</strong> <strong>in</strong> <strong>Al</strong>-<strong>Al</strong>Ox-<strong>Al</strong> <strong>tunnel</strong><br />
<strong>junctions</strong> by thermal anneal<strong>in</strong>g<br />
University <strong>of</strong> Jyväskylä<br />
Department <strong>of</strong> physics<br />
Nanoscience Center<br />
N S C<br />
Nanoscience Center
University Of Jyväskylä
Content<br />
n<br />
<strong>Al</strong>–<strong>Al</strong>Ox–<strong>Al</strong> <strong>tunnel</strong> <strong>junctions</strong><br />
n Fabrication<br />
n Applications<br />
n Us<strong>in</strong>g <strong>in</strong> quantum computation: Qubit<br />
n<br />
Anneal<strong>in</strong>g<br />
n Removes barrier structure defects<br />
n Ceases ag<strong>in</strong>g<br />
n<br />
Noise<br />
n Johnson <strong>noise</strong>, 1/f-<strong>noise</strong><br />
n Measur<strong>in</strong>g the <strong>noise</strong><br />
n AC Bridge modulation setup<br />
n<br />
n<br />
Results<br />
Conclusion
<strong>Al</strong>–<strong>Al</strong>Ox–<strong>Al</strong> <strong>tunnel</strong> junction<br />
n Insulat<strong>in</strong>g layer between conduct<strong>in</strong>g<br />
metal (~1-2 nm thick) thus electrons<br />
can <strong>tunnel</strong> through the barrier<br />
n Fabricated us<strong>in</strong>g nan<strong>of</strong>abrication<br />
methods on Silicon oxide or silicon<br />
nitride substrate<br />
n L<strong>in</strong>e width 200-400 nm<br />
First evaporation at 65 deg<br />
Second evaporation at 0 deg<br />
PMMA<br />
Copolymer<br />
Substrate
Applications<br />
n Low temperature thermometers<br />
n Electron coolers<br />
n Radiation detectors<br />
n SQUIDs<br />
n S<strong>in</strong>gle electron transistor<br />
n Memory devices<br />
n Quantum computation
Realization <strong>of</strong> a qubit<br />
n Coherent state, isolated from the environment<br />
n Absence <strong>of</strong> dissipation (superconduct<strong>in</strong>g)<br />
n ET
Anneal<strong>in</strong>g treatment<br />
n<br />
n<br />
After fabrication the barrier structure<br />
is imperfect<br />
Spontaneous relaxation to equilibrium<br />
n Resistance <strong>in</strong>creases <strong>in</strong> time; ag<strong>in</strong>g<br />
n<br />
Anneal<strong>in</strong>g: heat<strong>in</strong>g sample to 400 C<br />
n S<strong>low</strong> cool down; barrier will relax<br />
through the equilibrium states<br />
n Ceases ag<strong>in</strong>g (*)<br />
n Reduces the 1/f <strong>noise</strong><br />
(*) P. J. Kopp<strong>in</strong>en, L. M. Väisto, and I. J. Maasilta.<br />
Applied Physics Letters, 90:053503 (2007)
Ag<strong>in</strong>g
Conductance at 4K
Johnson <strong>noise</strong>:<br />
n Orig<strong>in</strong>ates from charge<br />
movements<br />
n Voltage <strong>noise</strong><br />
n White <strong>noise</strong><br />
n Depends only on<br />
temperature and resistance<br />
Noise<br />
1/f-<strong>noise</strong>:<br />
n Ensemble <strong>of</strong> charge traps<br />
or dislocations <strong>in</strong> barrier<br />
n Resistance fluctuations<br />
while current through the<br />
sample
Measur<strong>in</strong>g the <strong>noise</strong><br />
n Must get rid <strong>of</strong> the <strong>noise</strong> from the measurement setup<br />
(preamplifiers etc…)<br />
n Low-freq. measurements are difficult, time-consum<strong>in</strong>g,<br />
1/f-<strong>noise</strong> from preamplifiers dom<strong>in</strong>ate.<br />
n Requires a sensitive technique s<strong>in</strong>ce <strong>tunnel</strong> <strong>junctions</strong> are<br />
destroyed by large currents<br />
Noise from the preamplifiers<br />
Noise from the sample
n<br />
n<br />
AC Bridge modulation setup<br />
Solution: shift the <strong>noise</strong> measurement <strong>in</strong>to the region where<br />
m<strong>in</strong>imal preamplifier <strong>noise</strong><br />
Resistance fluctuations modulate the carrier signal
AC Bridge modulation setup<br />
n Phase selectivity, <strong>frequency</strong> dependent 1/f-<strong>noise</strong> <strong>in</strong><br />
phase with carrier signal<br />
n Out-<strong>of</strong> phase signal white Johnson <strong>noise</strong><br />
In phase<br />
Out-<strong>of</strong> phase
2kΩ carbon resistor at 4K<br />
S<strong>in</strong>gle amplifier measurement<br />
Bridge measurement:<br />
Blue is without and red is with crosscorrelation
Results<br />
Room temperature 1/f <strong>noise</strong><br />
spectrum <strong>of</strong> <strong>tunnel</strong> <strong>junctions</strong><br />
fabricated <strong>in</strong> HV and UHV<br />
Temperature dependence<br />
<strong>of</strong> the 1/f <strong>noise</strong> <strong>in</strong> nonannealed<br />
<strong>tunnel</strong> <strong>junctions</strong><br />
Noise normalized by <strong>tunnel</strong><strong>in</strong>g resistance<br />
Noise levels (at 10Hz) as<br />
a function <strong>of</strong> temperature.<br />
Solid circles represent<br />
non-annealed and open<br />
circles (different)<br />
annealed samples
Conclusion<br />
n Actually not 1/f <strong>noise</strong>,<br />
SR/R=1.6799.10-8f -1.13 for UHV-samples<br />
n 1/f <strong>noise</strong> is <strong>in</strong>dependent on used substrate<br />
n Samples fabricated <strong>in</strong> higher vacuum<br />
-> <strong>low</strong>er <strong>noise</strong><br />
n After anneal<strong>in</strong>g -> equal 1/f <strong>noise</strong> levels<br />
n Percentage drop is 80% <strong>in</strong> UHV samples<br />
and even 90% <strong>in</strong> HV samples (300K).<br />
q The critical current 1/f <strong>noise</strong> is related to the<br />
resistance <strong>noise</strong>
Thank you