Physica C 235-240 (1994)3339-3340 PHYSICA
North-Holland
Barriers formed by a plasma discharge process in all YBCO Josephson edge junctions
E. Aharoni and G. Koren
Physics Department and the Crown Center for Superconductivi~',
Technion - Israel Institute of Technology, Haifa 32000, Israel
All YBCO Josephson edge junctions were prepared with a barrier formed by an rf plasma discharge under
different conditions. The structure of the barrier and the transport properties of these junctions, have been
investigated. Under typical plasma conditions of 30-60 s plasma of 50-80 W at 100 mTorr of CF4 gas, and
500-600 °C, we found that the junctions behaved like weak links. The normal resistance was of the order of a
few ~2, with a minimum at around 50 K, .typical to localization versus temperature. The temperature
dependence of the critical current. I c, was found to be I c oc (T~ - T) 15. This reflects the asymmetric structure of
these junctions, in which only the base electrode is exposed to the plasma. To learn about the thickness of the
barriers a separate experiment was carried out on ultra thin YBCO films of various thicknesses that were
exposed to the plasma. It was found that under the above plasma conditions films thinner than 100 A have lost
their superconductivity. This determines an upper limit on the thickness of the barrier in our junctions. The
composition of the barriers was investigated by Auger spectroscopy performed on thicker films that were also
exposed to the same plasma. It was found that the surface layer down to about 50 A has lost its 1-2-3
stoichiometry, and contained a significant amount of carbon. This indicates a barrier thickness of about 50 A,
in agreement with the result obtained from the ultra thin films.
All YBCO Josephson edge junctions were
prepared in-situ using laser ablation deposition and
metallic masks, and the barrier was formed by
applying plasma discharge in CF 4 gas to modify
the edge of the base electrode [1,2]. The structure
of the barrier and the transport properties of the
junctions were characterized.
Under typical plasma conditions of 30-60 s
plasma of 50-80 W at 100 mTorr of CF 4 gas, and
500-600 °C, we found that the junctions behaved
like weak links. The normal resistance was of the
order of a few ~, with a minimum at 40-60 K,
typical to localization versus temperature.
Generally, the resistance normalized to the junction
area RcvA, increased with increasing sample
temperature, pressure, rf power, or discharge
duration. The critical current density decreased
correspondingly. Oxygen addition to the gas
flowing through the cell during the discharge,
caused stronger links. The normalized resistances
of three junctions prepared with different plasma
parameters are given in Fig. 1 as a fnnction of
temperature. The normalized resistance of the first
junction (a), created with the the above mentioned
plasma parameters, is localized in temperature at
about 60 K. The barrier in the second junction (b)
has been created with 200 mTorr flowing CF 4
during the discharge. R~A, in this case increases
with temperature. In the third exampl~e (c), the
addition of 20% oxygen during the discharge
created a strong link with normal resistance
decreasing with temperature. The critical currents,
below 40 K, were too high and prevented from
measuring the normal resistance.
The temperature dependence of the critical
current, I c, was found to be I c oc (T c - T) 15. This is
similar to the I c (T) dependence of SNIS junctions
[3] and reflects the asymmetric structure of these
junctions, in which only the base electrode is
exposed to the plasma. To learn about the thickness
of the barriers a separate experiment was carried
out on ultra thin YBCO films of various thicknesses
that were exposed to the plasma. The films were
covered with an insulating YBCO layer deposited at
500 °C to protect from room environment. The
resistivity vs. temperature of YBCO ultra thin films
exposed to 50 W plasma in CF 4 gas at 600 °C for
60 s and annealed in oxygen at 750 °C, is given in
Fig. 2. The thickness of the thinnest film
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