# A model study of present-day Hall-effect circulators

- B Placke
^{1}Email author, - S Bosco
^{1, 2}View ORCID ID profile and - DP DiVincenzo
^{1, 2, 3}

**Received: **10 November 2016

**Accepted: **15 March 2017

**Published: **17 April 2017

The Correction to this article has been published in EPJ Quantum Technology 2018 5:3

## Abstract

Stimulated by the recent implementation of a three-port Hall-effect microwave circulator of Mahoney *et al.* (MEA), we present model studies of the performance of this device. Our calculations are based on the capacitive-coupling model of Viola and DiVincenzo (VD). Based on conductance data from a typical Hall-bar device obtained from a two-dimensional electron gas (2DEG) in a magnetic field, we numerically solve the coupled field-circuit equations to calculate the expected performance of the circulator, as determined by the *S* parameters of the device when coupled to 50Ω ports, as a function of frequency and magnetic field. Above magnetic fields of 1.5 T, for which a typical 2DEG enters the quantum Hall regime (corresponding to a Landau-level filling fraction *ν* of 20), the Hall angle \(\theta_{H}=\tan^{-1}\sigma_{xy}/\sigma_{xx}\) always remains close to 90°, and the *S* parameters are close to the analytic predictions of VD for \(\theta_{H}=\pi/2\). As anticipated by VD, MEA find the device to have rather high (kΩ) impedance, and thus to be extremely mismatched to 50Ω, requiring the use of impedance matching. We incorporate the lumped matching circuits of MEA in our modeling and confirm that they can produce excellent circulation, although confined to a very small bandwidth. We predict that this bandwidth is significantly improved by working at lower magnetic field when the Landau index is high, e.g. \(\nu=20\), and the impedance mismatch is correspondingly less extreme. Our modeling also confirms the observation of MEA that parasitic port-to-port capacitance can produce very interesting countercirculation effects.

## Keywords

## 1 Introduction

*S*) matrices [3]

Recently, Viola and DiVincenzo (VD) proposed an alternative implementation for a passive circulator, which points the way towards better scalability [6]. The main message of their work is that non-reciprocal electrical conduction can lead to well-performing non-reciprocal devices. In particular, ideal circulation at specific frequencies is achieved by reactively coupling electrodes to the edges of a two-dimensional conductor such as a two-dimensional electron gas (2DEG) with a strong Hall effect. By the construction of Carlin [6–8], a 2DEG with three capacitively coupled edge terminals becomes a three-port circulator when the common grounds of the three ports are kept out of contact with the Hall conductor (i.e., the 2DEG should float with respect to the port ground).

The model proposed by VD applies for any values of Hall conductance, requiring the solution of coupled field-circuit equations. However, the results presented by VD were limited to the case when the Hall angle \(\theta_{H}\equiv\tan^{-1}\sigma_{xy}/\sigma_{xx}\) is exactly at its maximal value \(\pi/2\), corresponding to parameter values (magnetic field, carrier density) for which the material conductance is on a quantum Hall plateau and the Landau level filling parameter *ν* is an integer. Under these conditions the VD equations are solvable in closed form; for the more general case considered here, a numerical solution is needed. These solutions, and their consequences for the device *S* parameters, will be presented below.

An experimental realization of a Hall effect microwave circulator has now been reported by Mahoney *et al.* (MEA) [9]. MEA observes that impedance matching and parasitic capacitive coupling between neighboring ports play a key role for the behavior of their circulator. Impedance matching is essential to achieve good circulation, and the appropriate level of parasitic capacitance has the surprising consequence of inverting the direction of circulation in going from one magnetic field or frequency to another. By engineering the coupling between electrodes, this interesting property might be exploited for novel applications, where tiny changes of field could reverse the direction of circulation.

The present work is developed in light of MEA’s results. First, we employ the VD model, solving the field problem of a three-port Carlin circulator with realistic values of Hall angle obtained from typical 2DEG magnetoconductance characteristics. These characteristics involve a low magnetic-field regime in which small oscillations in the diagonal and off-diagonal conductances are observed (the Shubnikov-de Haas regime); as these oscillations grow to near 100% amplitude, one enters the quantum Hall regime in which plateaus occur in the off diagonal (\(\sigma_{xy}\)) conductance, and the Hall angle stays very near \(\pi /2\), oscillating slightly away from this value as the conductance passes from plateau to plateau. We see that our numerical calculations of the device performance are to a first approximation given by the analytic results of VD throughout the quantum Hall regime, but with noticeable departures from ideal behavior. We also incorporate in our calculations of the device response a complete circuit description including the impedance matching circuit and parasitic effects as reported by MEA. We find that impedance matching is essential for the realization of circulation; without matching the reflection coefficient of the device is very close to one, making the response very far from the desired behavior. We note, however, the impedance matching limits the versatility of the device: matching can be effectively performed only for specific combinations of parameters, i.e., for specific frequencies or magnetic fields.

Our paper is organized as follows. In Section 2, we compute the *S* parameters of an ideal Carlin circulator, when the device and the external circuit have equal impedance. In Section 3, we incorporate impedance matching circuits optimized for two specific magnetic fields and we study the response in the two cases. In Section 4, we include the parasitic coupling between electrodes: we confirm the magnetic field dependent change in the direction of circulation observed in [9] and we quantitatively analyze this phenomenon.

## 2 Basic analysis

*B*. Three electrodes of equal length

*L*are capacitively coupled to the material and they are symmetrically distributed around its boundary, parametrized by coordinate

*s*. This three-electrode device forms a circulator of the “first Carlin” type [6]. To model this circulator, we follow VD [6]; we assume that the capacitors are much longer than the gaps between them, also corresponding to the geometry of MEA. The VD model neglects any capacitances except for the external electrode capacitors, which should be reasonable for the aspect ratios used here. The work of VD also indicates that for Hall angle \(\theta_{H}\lesssim\pi/2\), the device response should be sensitive only to the edge dimensions and not to the shape of the conductor. Thus, we do not expect any large differences between the square device as modeled here and the circular device of MEA.

*ω*:

*σ*is the magnitude of the Hall conductivity tensor (assumed frequency independent), \(\hat{n}_{H}\) is the unit vector rotated by \(\theta_{H}\) with respect to the direction normal to the boundary and \(\overline{V}(\omega)\) is the Fourier transform of the time-dependent voltages applied at the electrodes. It is assumed that

*ω*is low enough, and the device is small enough that retardation effects are negligible, assuring the applicability of Eq. (2). The phenomenological function \(c(s)\) models the local coupling with the electrodes; it has the dimensions of capacitance per unit length. In our treatment, it takes the form

*i*. The parameter

*c*can be estimated for certain geometries from theory, e.g. [12–15], or directly extracted from experiment. It has contributions from both classical electrostatic coupling and from quantum capacitance due to screening effects [16–18]. A rule of thumb is that quantum capacitance starts to play an important role when the distance between electrodes and quantum Hall droplet is comparable with the electron screening length. In MEA [9], this condition is apparently not met, and we believe that the coupling is strongly dominated by the classical geometric capacitance; this is no problem for the realization of a circulator.

*i*th electrode is related to the boundary potential by [6]

*S*) matrix using the relation [3]

*S*and comparing with Eq. (1), one can establish a criterion [6] to quantify the circulating behavior of the device:

*S*-matrices. From this figure, it appears that even tiny variations of

*Q*from 3 can lead to a significant backward circulation and consequently to a noticeable loss of chirality, e.g. for \(Q_{\circlearrowleft }= 2.8\), \(Q_{\circlearrowright }\) can attain a value as large as 1.

*σ*and \(\theta_{H}\) from the experimental data shown in Figure 3; this data, which is entirely generic for heterostructure 2DEGs, is taken from a device used in the advanced (masters) physics lab course of the second physics institute of Aachen University.

^{1}Figure 4 shows the

*Q*-parameters as a function of frequency and magnetic field for a perfectly matched device (note that perfect matching requires a magnetic field dependent \(Z_{0}\)). From the plot, we confirm that at the frequency in Eq. (8) almost perfect circulation in the anticlockwise direction can be achieved. Comparing with Figure 3, we notice that the highest values of

*Q*are obtained at magnetic fields corresponding to the quantum Hall plateau, but good circulating performances are guaranteed also in the transition regions and in the Shubnikov-de Haas regime. In particular, we observe that in the latter regime the device has a greater bandwidth.

*ν*being the filling factor [19], far greater than the characteristic impedance of standard microwave circuits \(Z_{0}=50\Omega\). Thus, use of impedance matching techniques is essential.

## 3 Augmented network for impedance matching

*LC*-circuits at each port are used to match the impedance of the device with the external circuit. This network, like any impedance-matching circuit, has the drawback of working only at specific frequencies \(\omega_{m}\), limiting the versatility of the circulator. Figure 5 also shows parasitic capacitances coupling each pair of neighboring electrodes, as suggested by MEA. We will neglect these for the time being, returning to their analysis in the following section. From standard circuit theory (see Chapter 3 of [20]), one can write the admittance matrix of the augmented device

*ν*. Hence, the impedance matching circuit works only for specific filling factors, setting an additional constraint on the regime of parameters which guarantees good circulation.

*Q*-parameters when the matching is optimized for filling factor \(\nu =8\) and for the first circulation frequency, i.e. \(\omega_{m}=\omega _{c}(n=0)\). As expected, the device behaves as the theoretical perfectly matched device, in Figure 4, only near the filling factor and frequency at which the matching is performed. For the parameters needed for good impedance matching, the effective bandwidth of the device is limited, as expected given the very large mismatch to be overcome.

*Q*-parameter decreases. Hence, when engineering the device there is a trade-off between bandwidth and circulation performance to be accounted for.

## 4 Effect of parasitic capacitances

*Q*-parameters for the realistic parasitic coupling value \(C_{p}=120~\mbox{fF}\). The surprising effect of the additional capacitive channels is to introduce significant circulation in the reverse direction, as experimentally observed in [9]. The direction of circulation becomes magnetic-field dependent and is seen to change in the vicinity of the curve defined by \(\omega=\omega_{c}(n=0)\). Interestingly, for the parameters chosen, both circulators behave almost equally well, with a maximum of \(Q_{\circlearrowleft }^{\max}=2.75\) and \(Q_{\circlearrowright }^{\max}=2.88\). Finally, for significantly larger values of the parasitic capacitances, they dominate the device response and circulation in both directions is suppressed, as shown in Figure 10.

*Q*-parameters on \(C_{p}\). Figure 11 shows the maximum value of

*Q*for the two directions of circulation as a function of the parasitic coupling. Strikingly, reverse circulation can be more effective (larger

*Q*) than the direct one, and it degrades more slowly as \(C_{p}\) increases. Finally, we observe that for certain coupling values, e.g. \(C_{p}\approx 40~\mbox{fF}\), almost perfect circulation can be achieved in both directions (at different frequencies, of course). This phenomenon might be exploited for novel applications, where tiny changes of magnetic field can reverse the direction of circulation.

## 5 Conclusion

We have investigated an implementation of a quantum Hall effect circulator. We proved that realistic variations of Hall angle occurring once the quantum Hall regime has been entered (at around 1.5 T for the 2DEG considered) do not alter significantly the fundamental behavior of the device investigated in [6], even for a large Landau-level index (\(\nu=20\)). Moreover, we addressed two important microwave-engineering issues, impedance matching and parasitic capacitances. Although the presence of an impedance matching circuit decreases the versatility of the device, we proved that the performance of the circulator can be optimized either to have a large bandwidth or to operate in a large range of magnetic field. Finally, analyzing the effect of parasitic capacitances, we observed a reverse circulation phenomenon, expected from recent experiments [9]. Interestingly, we found that depending on the coupling strength the reverse circulation is comparable and for certain parameters even better than the direct one, opening up to new possible applications.

## Notes

## Declarations

### Acknowledgements

The authors would like to thank D Reilly, A Mahoney, AC Doherty, and T Leonhardt for useful discussions. This work was supported by the Alexander von Humboldt foundation.

**Open Access** This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

## Authors’ Affiliations

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