Combined breakdown of a dielectric nanolayer to form a Josephson bridge A.V. Krevsun S.I. Bondarenko V.P. Koverya B. Verkin Institute for Low Temperature Physics and Engineering of the National Academy of

2025-04-27 0 0 271.56KB 10 页 10玖币
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Combined breakdown of a dielectric nanolayer to form a Josephson bridge
A.V. Krevsun, S.I. Bondarenko, V.P. Koverya
B. Verkin Institute for Low Temperature Physics and Engineering of the National Academy of
Sciences of Ukraine, Kharkiv 61103, Ukraine
E-mail: bondarenko@ilt.kharkov.ua
Electrical breakdown of a dielectric nanolayer between film electrodes under the combined
action of direct current and capacitor discharge current makes it possible to form Josephson bridges
with a reproducible resistance exceeding 1 Ω. A new feature of the formation of a bridge during
electrical breakdown, which is preceded by a series of preliminary breakdowns (auto breakdowns) of a
dielectric nanolayer, has been discovered. The mechanism of the process and the role of the thickness
of the cathode film in the formation of the bridge are discussed.
Keywords: electrical breakdown, Josephson bridge, dielectric nanolayer.
1. Introduction
It is known [1-7] that as a result of electrical breakdown of a thin dielectric layer between two metal
electrodes, a conducting channel is formed in it in the form of a metal bridge. Almost all numerous
studies of the formation of such bridges were previously carried out using non-superconducting
massive electrodes. For the first time, studies of some properties of bridges made of superconducting
materials formed as a result of electrical breakdown were carried out in 1970-1976 in B.I. Verkin
Institute for Low temperature Physics and Engineering (ILTPE) [8, 9, 10]. At the same time, the use of
film electrodes was also new. The purpose of these studies was to elucidate the possibility of using
electrical breakdown to create a superconducting weak link between films with Josephson properties.
In particular, three methods were tested to achieve the breakdown of a dielectric: a smooth increase in
the electric voltage across it from a direct voltage source, a discharge of an electric capacitor through
it, and a single rectangular voltage pulse [10]. The material of the bridges formed by the electrical
breakdown was lead or a lead-tin compound, from which a thin cathode film was made. The features
of the cathode metal film transfer through the dielectric during breakdown are an important and little
studied issue. The result of the initial studies of the formation of superconducting bridges during the
electrical breakdown of a dielectric was an experimental proof of the fundamental possibility of
creating such Josephson weak links [9, 10]. In the future, based on these film bridges, it was planned to
develop miniature film superconducting direct current (DC) quantum interferometer with high
sensitivity and stability of parameters even under significant external mechanical influences.
At the same time, a number of questions concerning the patterns of bridge formation remained
unexplained. The answer to some of them was obtained by us in a recent work [11], in which an
electrical breakdown of the dielectric oxide layer of a niobium film with a thickness of 30 nm was
carried out using a 50% indium50% tin alloy film with a thickness of 100 nm as a cathode. In
particular, for the first time it was found that with a smooth (less than 1 V/s) increase in voltage up to
breakdown, the minimal and reproducible total value of the bridge resistance (RΣ 3 Ω), consisting of
the intrinsic resistance of the bridge Rb and the resistance of the contact conductor, was achieved at a
breakdown current of 10 mA. In this case, the indicated resistance values at a temperature of T=300K
were reproducible on dozens of bridges. The diameter (about 25 nm) of the bridge itself with a
resistance of Rb 1 Ω was determined by calculation. It was experimentally proved that the bridge
material is identical to the indium-tin alloy of a cathode film. At the same time, the manufacture of
Josephson bridges (JB) by the electrical breakdown method is much simpler than by known traditional
methods.
It was also shown that in the temperature range of 300-77K, the dependence of the resistance of
the cathode film and bridges on temperature with its decrease is linearly decreasing, and their
temperature coefficients of resistance (TCR) are within (2.0 ± 0.3)×10 -3 K-1. Note that the TCR of
massive indium and tin are (4.9 and 4.4) × 10-3 K-1, respectively.
The importance of determining the resistance value of the bridge at T=300K is that it correlates
with the value of its normal resistance (NR) near the superconducting transition and the critical current
of the JB in the superconducting state, which determines its Josephson properties [12].
At present, there are a number of unresolved issues in the technology of manufacturing JB
using breakdown. These include questions about the possibility to form a reproducible JB with Rb ˃ 1
Ohm, about influence of the thickness of the cathode film on the formation of JB, as well as the use of
alternative methods of electrical breakdown of the dielectric and their influence on the NR value of the
resulting JB. In particular, such a method can be the breakdown of niobium oxide using the combined
electrical action on the oxide of direct current and the current of a capacitor connected in parallel and
charged to the breakdown voltage.
The purpose of this work was to find answers to these questions through experimental studies.
2. Setting up the experiment.
Figure 1 shows the electrical circuit of the device for the combined breakdown of niobium oxide in
order to form JB.
摘要:

CombinedbreakdownofadielectricnanolayertoformaJosephsonbridgeA.V.Krevsun,S.I.Bondarenko,V.P.KoveryaB.VerkinInstituteforLowTemperaturePhysicsandEngineeringoftheNationalAcademyofSciencesofUkraine,Kharkiv61103,UkraineE-mail:bondarenko@ilt.kharkov.uaElectricalbreakdownofadielectricnanolayerbetweenfilmel...

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