PTB > Structure > Division 2 > Department 2.4 > Working Group 2.42 > Single-charge Circuits
Deutsche Version
Single-charge-flux Circuits



- Research:
* Single-charge circuits
* Single-flux circuits
- Technology
- Publications



Research:
Single-charge Circuits


SET-circuits for standard of current

Single-electron pump

With the help of an electron pump it is possible to organize a highly-correlated current of single-electrons, forced by the external periodic high-frequency signal and locked to this driving signal. The simplest pump (Fig.1) contains only three small tunnel junctions connected in series and two gates (Gate1 and Gate2), whose capacitive coupling to the intermediate islands makes it possible to control the charging ground state of the pump. When the driving signal is applied to the gates with a relative phase shift of about 90°, the pump enters the regime, even at zero bias voltage V = 0, where electrons are transferred through the pump one by one, one electron per cycle of the driving signal. This gives rise to a current I = ef and the total electric charge Q transferred through the pump amounts to Q = Ne, where N is the number of cycles.

Click for larger image!

Click for larger image!

 

 

Figure 1:
Electric equivalent circuit of a 3-junction pump.

Figure 2:
From 3-junction pump
towards 3-junction R-pump: suppression of unwanted electron cotunneling, the effective process of simultaneous tunneling in the two "passive" junctions.

 

 

The reliability (charging accuracy) of pumping generally depends on the parameter values of the pump as well as on those of the control signal (frequency f, phase difference, amplitude) and at sufficiently low temperatures in the range of mK is mostly limited by the rate of electron cotunneling (Fig.2). This rate can be reduced in two different ways:

  • by means of addition of several extra tunnel junctions [1]; (The additional junctions make the operation of the pump noticeably more complicated, because of correspondingly larger number of control gates necessary.)
  • by using a compact ohmic resistance connected in series to the pump [2] (see Fig.2). We call this new SET-device R-pump.

The effect of pumping of electrons can be observed with the help of the current steps I = ef on the voltage-current characteristics. The width of the steps characterizes the stability of pumping regime against the unwanted cotunneling processes. The results (Fig.3) of our first experiments [3] with the 3-junction R-pump on the basis of the junctions of type Al/AlOx/Al and the on-chip resistors of Cr (Fig.4), fabricated by means of shadow angle evaporation technique, indicate that the metrological level of accuracy of 10 ppb, which otherwise can be realized with the multijunction pump only, is achievable even with the 3- or 4-junction R-Pump.

Current steps: Click to enlarge!

SEM Image: Click to enlarge!

 

 

Figure 3:
Current steps on IV-curve
of an R-pump

Figure 4:
SEM Image of R-pump
(with 4 on-chip Cr resistors)

 

 

The forthcoming applications for the SET-pump of high accuracy involve the closing of the metrological triangle and the standard of electric capacitance.

In the framework of cooperation with Working Group 2.61 towards the development of the single-electron capacitance standard, we developed a 5-junction R-pump to be fabricated on a dielectric quartz glass substrate, due to its substantially smaller dielectric constant. The importance of a low dielectric constant is related to a single-electron resolution of an SET electrometer connected to a 0.1mm-large on-chip needle pad which is used to contact the cryocapacitor. The technological steps (for example, PMMA/Ge/Copolymer-three layer mask, E-beam lithography, three-angle deposition) have been implemented in a similar way as on standard Si-wafer and must be adjusted to the conditions of an insulating substrate. In particular, we could avoid a destructive effect of substrate electrostatics by using a 30nm-thin semiconductor Si layer evaporated on top of the wafer.


TOP


Cooper pair solitons and Bloch oscillations in a long array of small Al/AlOx/Al-junctions


Click to enlarge!

Figure 5:
Equivalent circuit of a long array with high-ohmic resistors
and a shape of a Cooper-pair soliton.

We investigate electric transport properties of a long array (Fig.5) of small Al/AlOx/Al tunnel junctions, biased through high-ohmic on-chip Cr-resistors and driven by an external high-frequency signal using capacitive gates. In order to be able to tune the Josephson coupling strength, we fabricated an array of small-junction SQUIDs (see an SEM-Image in Fig.6). The IV-curves, Fig.7, measured at low temperatures show a region of a negative differential resistance, which, in such structures, indicates the presence and dominance of so-called Bloch-oscillations [4]. Due to a fundamental current-frequency relation I = 2ef, the use of these oscillations can be of metrological relevance, opening a possibility of a quantised current source. As compared to single tunnel junctions [5], the long arrays have an advantage of substantially larger oscillation amplitudes in voltage, and they are featured by similarly wide frequency range up to several GHz. A series connection of small Josephson junctions gives rise to a specific physical problem: the dynamics of charge in form of Cooper pair solitons with variable mass. In the framework of electro-mechanic analogy, the role of the mass is played by the quasicharge-dependent so-called Bloch inductance of the junctions [6].


Click to enlarge!
Click to enlarge!
Figure 6:
SEM-Image of an array of ultrasmall SQUIDs
and on-chip high-ohmic resistors.
Figure 7:
IV-characteristics shows a region of the
negative differential resistance (see also Inset)
and indicates a presence of so-called Bloch oscillations.



TOP


Single-electron transport in hybrid SNS Turnstiles

A compact transistor structure, consisting of two small tunnel junctions between the normal conductive and the superconductive electrodes and a capacitive gate to the middle island (see Fig. 8), driven by a high-frequency signal, has been used for quantised charge transport. The transport is cyclic and it involves the excitations of the quasiparticle spectrum of superconductor. Activated by the gate oscillations, the electrons tunnel consecutively through the one or the other tunnel junction. In the island they become quasiparticles of two different polarities, which recombine after a short time. Owing to this operation principle, the device is called "hybrid turnstile" [7]. Our recent studies demonstrated the turnstile behaviour up to the high frequencies of ~1GHz. At the same time, the accuracy of pumping was found to be subject to a few undesirable leak mechanisms. We found that one of these mechanisms related to multiple-tunneling processes (higher-order tunneling) in the bias range below the superconducting gate voltage. The devices of type SNS has shown a lower leakage and the more flat current plateaus than those of type NSN.




Figure 8: SEM Image of a hybrid turnstiles with an on-chip resistor.


We successfully tried to reduce the rate of leakage with the help of compact high-ohmic microstripline resistors of Cr. This improves the turnstile performance at the typical frequencies ~10-100MHz. However, due to the resistor, the current plateaus were found to be shifted to a higher bias-voltage range (see Fig. 9). On the other hand, the high-bias extension of the plateaus was limited by the heating effects, increasing with the driving frequency. Both mentioned effects result in a practical frequency limitation of ~100MHz. The work is supported by the EU through the project SCOPE.



Figure 9: Current plateaus for the two types of devices, SNS und SNS with a Cr-resistor (R-SNS).



References

[1] M. W. Keller, J. M. Martinis, N. M. Zimmerman, and A. H. Steinbach, "Accuracy of electron counting using a 7-junction electron pump", Appl. Phys. Lett. 69, 1804 (1996);
M. W. Keller, J. M. Martinis and R. L. Kautz, "Rare errors in a well-characterized electron pump: comparison of experiment and theory", Phys. Rev. Lett. 80, 4530 (1998).

[2] A. B. Zorin, H. Zangerle, S. V. Lotkhov, and J. Niemeyer, "Coulomb blockade and cotunneling in single electron circuits with on-chip resistors: towards the implementation of R-pump", J. Appl. Phys. 88, 2665 (2000).

[3] S. V. Lotkhov, S. A. Bogoslovsky, A. B. Zorin, and J. Niemeyer, "Operation of a three-junction single-electron pump with on-chip resistors", Appl. Phys. Lett. 78, 946 (2001).

[4] K. K. Likharev and A. B. Zorin, "Theory of the Bloch-wave oscillations in small Josephson junctions", J. Low Temp. Phys. 59, 347-382 (1985).

[5] L. S. Kuzmin and D. B. Haviland, "Observation of the Bloch oscillations in an ultrasmall Josephson junction", Phys. Rev. Lett. 67, 2890-2893 (1991).

[6] A. B. Zorin,"Bloch inductance in small-capacitance Josephson junctions", Phys. Rev. Lett. 96, 167001 (2006).

[7] J. P. Pekola, J. J. Vartiainen, M. Möttönen, O.-P.Saira, M. Meschke, and D. V. Averin, "Hybrid single-electron transistor as a source of quantized electric current," Nature Phys. 4, 120 (2008).



TOP



© Physikalisch-Technische Bundesanstalt
Page created: 04. July 2007, last update: 12. February 2009, Sergey Lotkov