Article | Open | Published:

Composite fermion liquid to Wigner solid transition in the lowest Landau level of zinc oxide


Interactions between the constituents of a condensed matter system can drive it through a plethora of different phases due to many-body effects. A prominent platform for it is a dilute two-dimensional electron system in a magnetic field, which evolves intricately through various gaseous, liquid and solid phases governed by Coulomb interaction. Here we report on the experimental observation of a phase transition between the composite fermion liquid and adjacent magnetic field induced phase with a character of Wigner solid. The experiments are performed in the lowest Landau level of a MgZnO/ZnO two-dimensional electron system with attributes of both a liquid and a solid. An in-plane magnetic field component applied on top of the perpendicular magnetic field extends the Wigner-like phase further into the composite fermion liquid phase region. Our observations indicate the direct competition between a composite fermion liquid and a Wigner solid formed either by electrons or composite fermions.


A magnetic field B applied perpendicularly to a two-dimensional charge carrier system modifies its density of states and places the charge carriers on a ladder of discrete Landau levels (LL). The Coulomb interaction between the charged particles acting on the magnetic length scale \(l_{\mathrm{B}} = \sqrt {\hbar /eB}\) can be tuned by varying the magnetic field strength. Thereby, the high mobility carriers evolve through the various correlation phases1. When the electrons occupy half of available states in the lowest LL, e.g., filling factor ν = 1/2, the electrons prefer to reduce their interaction by virtue of capturing two magnetic flux quanta resulting in the emergence of new particles, called composite fermions (CF)2,3. These particles form a Fermi surface at ν = 1/2 and move in an effective field Beff = B − Bν = 1/2 (Fig. 1, middle panel) giving rise to magnetoresistance oscillations. At even lower filling factors a Wigner solid, a crystalline phase of charged particles (electrons or CF) driven by the repulsive Coulomb force and yet another manifestation of many-body correlations, emerges as a ground state of the electron system (Fig. 1).

Fig. 1

Schematic of the phases of a 2DES in a magnetic field: The different phases of a two-dimensional electron system (2DES) in a magnetic field. At zero magnetic field (bottom panel) the electrons are described as a weakly interacting Fermi gas with a well-defined Fermi surface. In the half-filled lowest LL, e.g., at filling factor ν = 1/2, the electrons reduce their mutual interaction by attaching the two magnetic flux quanta, resulting in the emergence of new particles, so-called composite fermions (middle panel)2,3. These particles form a Fermi surface at ν = 1/2 and move in an effective field Beff = B − Bν = 1/2 giving rise to magnetoresistance oscillations known as the fractional quantum Hall effect (Fig. 2). At even lower filling factors, a Wigner solid, a crystalline phase of electrons arranged by the repulsive Coulomb force and another manifestation of many-body correlations, becomes the ground state, which can be formed either by bare electrons (top left) or composite fermions (top right)

Being in the lowest Landau level (LL) the electron system experiences competition between the composite fermion liquid phase and the magnetic field induced Wigner solid phase, which manifests as a large magnetoresistance peak around or below ν = 1/34,6. A liquid-solid transition may follow the Kosterlitz–Thouless model, whereas the particles can form a hexatic phase characterized by bond-oriented nearest-neighbor ordering7,8,9,10,11. An intermediate phase of the liquid-solid transition may also take the form of microemulsion phases associated with a liquid crystalline phase11,12,13. Departing from the liquid phase of CF at ν = 1/2, a formation of both a composite fermion Wigner solid and phase transition to intermediate phases may appear feasible. The idea of realizing a composite fermion Wigner solid was put forward in a number of theoretical works14,15,16,17,18,19. Recent experiments focusing on GaAs-based 2DES have been gradually accumulating evidence pointing towards the realization of CF Wigner solid20,21,22,23,24. Intuitively the CF crystal is stabilized when the CF of nearby liquid states release two of their vortices to stabilize the crystal, whereas the undressed particles retain their energetically favorable correlations18. Thus a two-flux CF crystal borders the four-flux composite fermion liquid phase, whereas an electron crystal phase is embedded in two-flux composite fermion liquid and forms between filling factors ν = 1/3 and ν = 2/5 for a high enough LL mixing19. Thus the transition between the liquid and the solid can be highly non-trivial and is realized in the lowest LL of a two-dimensional charge carrier system by the transformation of the underlying particle type.

Here, we study the magnetotransport in a ZnO heterostructure (see: Methods) in the magnetic field region between the CF liquid phase formed at ν = 1/2 and the high resistivity phase appearing at higher field and exhibiting attributes of a Wigner solid25,26. LL mixing, the ratio between electron–electron interaction energy and the cyclotron energy, is 4.2 at ν = 1/2 in this heterostructure and the magnetotransport in the region of interest features a character of both CF liquid and crystalline phase. The presence of such a region with the interlaced character highlights a non-trivial nature of phase transition, the details of which can further be masked by the inhomogeneous potential landscape arising from inevitable crystallographic disorder. The transition between the two phases can be tuned by the application of an in-plane magnetic field. As a result of the phase intermixture, the state at filling factor ν = 1/2 can be formed by a composite fermion liquid and some intermediate state arising in the course of liquid-solid transition. Owning to a simple band structure of ZnO as compared to p-type GaAs, this oxide material is an attractive platform to access the competition between liquid and solid phases in the fractional quantum Hall regime.


Experiment in perpendicular magnetic field

Figure 2 shows a full scan of the magnetotransport from 0 T to 33 T applied perpendicular to the 2DES plane. Several fractional quantum Hall states are observed around ν = 3/2, consistent with previous results26 and, in addition, developing minima are observed at ν = 9/5, 12/7, 9/7, and 6/5. Furthermore, up to six fractional quantum Hall states are observed on both sides of ν = 1/2. Close inspection of the transport around ν = 1/2 reveals a distinct asymmetry; Rxx maxima between fractional quantum Hall states for ν < 1/2 are much larger than those for ν > 1/2. This increase becomes increasingly dramatic between ν = 2/5, 1/3, and 2/7. Such a high resistance phase between ν = 1/3 and 2/7 has also been observed in GaAs, and was interpreted as the electron Wigner solid pinned by disorder. Two mechanisms have been identified for the appearance of the Wigner solid around these filling factors: one is a large LL mixing, which modifies the ground state energies of fractional quantum Hall states and Wigner solid;4,5,19 the other is short-range disorder4,27,28. Both mechanisms are more pronounced in ZnO-heterostructures than in GaAs25,29.

Fig. 2

Temperature-dependent magnetotransport up to 33 T. a Rxx at T = 60 mK (blue trace). The other colors show Rxx(B) in the fractional quantum Hall regime for higher temperatures. The high resistivity phases HRP1, HRP2, and HRP3 are indicated by the shaded region. b Mass of composite fermions extracted from the temperature dependence of the Rxx oscillation amplitude. c Temperature dependence of Rxx at ν = 1/2. The decreasing resistance with increasing temperatures indicates a residual interaction between composite fermions

In Fig. 2 the apparent high resistance phases are colored and marked as HRP1, HRP2, and HRP3. On the basis of Wigner solid studies in other materials system, the characteristics of HRP1, HRP2, and HRP3 are typical of the Wigner solid. The temperature dependence of Rxx for HRP1, HRP2, and HRP3 resembles the melting of the Wigner solid (Supplementary Fig. 1a). The non-linear current-voltage characteristics are associated with the depinning of the Wigner solid from the disorder, when a certain threshold force is exceeded, and its subsequent sliding along the disorder landscape (Supplementary Fig. 1b). Thus, the trace of a Wigner solid formation appears already in HRP1 between ν = 3/7 and ν = 2/5, whereas a larger Rxx and IV non-linearity at HRP2 and HRP3 indicate a stronger pronounced Wigner solid character.

A non-linear I–V characteristics can also appear in structures with domain boundaries originating from the sample inhomogeneity. To reduce the effect of sample inhomogeneity the structures were being rotated during the molecular epitaxial growth and we used a piece of structure next to the center of the ZnO substrate to ensure a higher sample homogeneity30. Although we cannot exclude the effect of sample inhomogeneity on the sample characteristics, our structure demonstrates magnetotransport of quality comparable with the best GaAs structures. Furthermore, as we will demonstrate later in the paper, the effect of in-plane magnetic field on both the high resistive phases and the transport around ν = 1/2 has a largely intrinsic origin.

HRP1 represents an interesting region. While it shows the features of an emerging Wigner solid, at the same time it can be comprised as a part of the Rxx oscillations caused by the CFs’ orbital motion in Beff, and therefore can also be attributed to the liquid phase. We note that the Rxx amplitude at HRP2 shoots up so high that it can hardly be associated with a gradual increase of the Shibnikov-de Haas oscillations amplitude with an increasing magnetic field. The estimate of the CF mass can be valuable to characterize the CF liquid phase and to elucidate the characteristics of region HRP1. Thus, we now analyze the CF mass mCF around ν = 1/2 from the temperature dependence of the Rxx oscillation amplitude by using the Lifshitz–Kosevitch formalism (Supplementary Note 2). Figure 2b displays mCF around ν = 1/2, which extends the linear dependence of mCF on B (Supplementary Fig. 3) to higher field as mCF/m0 = 0.047B/T25. More noticeable is the increase of mCF over the linear trend when the 2DES approaches the high resistivity phase HRP1.

The increase of the composite fermion mass is the signature of an enhanced electron–electron interaction, effectively strengthened by the reduction of kinetic energy, which is brought about by the electron localization by the magnetic field and/or disorder. An enhanced mass can also possibly be anticipated when CFs become more inert due to their localization. Both scenarios for mass increase signal the formation of a solid state, which is consistent with observing the traces of the Wigner solid character at HRP1, and the more strongly pronounced Wigner solid-like character at HRP2. Our transport experiment cannot distinguish whether the high resistance phase HRP2 is formed by the electron or composite fermion. Following the recent theory19 HRP2 should correspond to an electron crystal. Then the transport characteristics described above can be treated as experimental attributes of the intricate phase transition between the composite fermion liquid phase and electron solid. HRP3 can potentially be attributed to a two-flux composite fermion Wigner crystal, as it forms in the LL filling factors attributed to a four-flux composite fermion liquid.

Experiment in tilted magnetic field

The transport properties discussed above change dramatically when the sample is rotated in the magnetic field, that is, when an additional field component is applied parallel to the 2DES. Since the electron spin susceptibility for this structure is about 2, the opposite spin orientation branch of the lowest LL lies energetically high and is not populated31. Thus the spin effects are not anticipated to play a role for the discussion below. Figure 3a depicts Rxx traces at several sample orientations θ obtained at base temperature and shows the asymmetrical impact of the in-plane field on the transport for ν < 1/2 and ν > 1/2 (θ is the tilt angle between the normal of the 2DES plane and the magnetic field direction). Firstly, one notices that Rxx of HRP1, HRP2, and HRP3 increases gradually with an increasing θ, while Rxx minima at ν = 3/7, 2/5, and 1/3 do not change significantly. Thus the insulating phase becomes more pronounced by applying an in-plane field. The temperature dependence of Rxx maxima of the high resistivity phases is depicted for three representative θs in Fig. 3b. Furthermore, Rxx around ν = 1/2 gains a background, which becomes larger with the increasing θ. Since magnetotransport experiments in GaAs demonstrate the extension of the tail of the insulating phase into the ν = 1/2 region with an increasing θ32,33, we may also suppose that the background forming around ν = 1/2 has the same origin and is associated with the development of the insulating phase growing towards ν = 1/2 and above.

Fig. 3

Magnetotransport in tilted magnetic fields. a The resistance of high resistivity phases HRP1, HRP2, and HRP3 increases with the application of in-plane magnetic field. The insulating phase shifts towards higher filling factors with increasing in-plane field, as can be seen from the growing background around ν = 1/2. Inset: mass of composite fermions evaluated from temperature dependence of Rxx oscillation amplitude. b Temperature dependence of high resistivity phases HRP1, HRP2, and HRP3 at several tilt angles


A strong in-plane field couples to the orbital motion and enhances the inter-subband scattering rate34. This will result in an additional LL broadening and should be particularly effective in our ZnO heterostructure, since the subband separation in the confinement potential is of the order of 5 meV and the electron cyclotron energy reaches 3.8 meV at 10 T35. The scenario of scattering rate enhancement at high θ is not consistent with our experimental data. Indeed, for all tilt angles θ the Rxx oscillations are not damped but rather persist on top of an increasing background. Both the field where Rxx oscillations onset and the number of Rxx oscillations do not change with an increasing in-plane field strength, whereas an anticipated broader LL ought to smear out the oscillations and to increase the field where Rxx oscillations set on.

Furthermore, we analyze the temperature dependence of the Rxx oscillation amplitude and estimate mCF around ν = 1/2 for several θs (Supplementary Note 2). The inset of Fig. 3 depicts the result of this analysis. For ν > 1/2, mCF does not show any noticeable change, but it shows a pronounced field and tilt angle dependence for ν < 1/2, that is, for a given perpendicular magnetic field mCF is heavier at a larger tilt angle. The quantum scattering time traced as a fitting parameter in the estimation of mCF does not show a tilt angle dependence around ν = 1/2(Supplementary Fig. 5). This strengthens our concept of negligible change of inter-subband scattering rate due to the application of in-plane magnetic field. The estimation of scattering time becomes more uncertain at approaching the HRP1 phase. This points to an inadequate description of high resistivity phases with Lifschitz–Kosevitch approximation, possibly supporting our point that the HRP1 phase has a mixed character of state of matter. Therefore the experimental finding implies that the change in magnetotransport caused by the in-plane field application has an intrinsic origin.

The application of an in-plane field can significantly disturb the electron/CF Fermi contour making it elliptic shaped36,37,38,39,40. The effective particle mass is now given by \(m \ast = \sqrt {m_t \times m_l}\), where mt and ml are the masses along two prime axises of the ellipse. Such anisotropy might be responsible for the CF mass enhancement beyond the mass estimated at zero tilt angle. An enhanced mass can also signal that the electron–electron interaction becomes stronger, which brings the system closer to the condition to form a crystalline phase.

In order to further address the in-plane field induced stabilization of the Wigner solid-like phase we now analyze how much the in-plane field squeezes the electron wavefunction width, as it effectively enhances the Coulomb interaction and can affect the transport properties41,42,43. In zero in-plane field the wavefunction width of the heterostructure is about 10 nm wide31,35. At θ = 50° it is squeezed down to 2.6 nm at B = 12 T, representing the region ν > 1/2, and down to 2.2 nm at B = 17 T, representing the region ν < 1/2 (Supplementary Note 3). Since the wavefunction width reduces significantly with in-plane field on both sides of ν = 1/2 compared with zero in-plane field, the Coulomb interaction should also be commensurately enhanced around ν = 1/2. Nonetheless, mCF defined by the interaction effects remains almost unchanged for ν > 1/2 and no large effect of in-plane field on transport characteristics is seen in this region. Consequently, the increase of mCF for ν < 1/2 is not mainly caused by the reduced wavefunction width. However, a smaller width of the wavefunction favors the solid phase over the liquid phase19. This can explain an increased resistivity of HRP1, HRP2, and HRP3 phases and the gradual shift of insulating phase towards higher filling factors. In this scenario, the mCF increase in ν < 1/2 region is consistent with our observation that mCF is larger the closer the electron system approaches the high resistivity phase, which may be interpreted as an effective localization of the CF.

Finally, we discuss the filling factor ν = 1/2, which is originally thought to have a Fermi surface of CF (Fig. 1). Figure 4 depicts the temperature dependence of Rxx at several θ’s. At θ = 0, considering the presence of only CF Fermi surface, the logarithmic temperature dependence of Rxx points toward a residual CF interaction2,25,44. At larger θ the slope of logarithmic Rxx temperature dependence increases, pointing to an increased CF residual interaction. On the other hand, our experiment demonstrates the shift of the insulating phase towards higher filling factors with an increasing θ. Consequently, the state at ν = 1/2 is formed by both a CF Fermi liquid with a Fermi surface and tail of the insulating phase forming in the course of liquid-solid phase transition. Then the Rxx temperature dependence at each θ in Fig. 4 reflects not only the CF residual interaction but also the melting of the intermediate liquid-solid phase growing towards ν = 1/2. Giving a small Rxx increase between θ = 0 and θ = 40 the intermediate phase is absent or its contribution is small at ν = 1/2 for θ = 0. Our consideration raises questions about the stability of a CF Fermi surface exposed to a strong in-plane magnetic field, whereas the 2DES characteristics in a tilted magnetic field can likely be the attributes of the precursor for the new insulating state in a strong in-plane magnetic field proposed by Piot et al.33.

Fig. 4

Rxx temperature dependence at ν = 1/2. The resistance decreases with increasing temperature indicating a residual interaction between the composite fermions at zero tilt angle. The slope becomes more pronounced at higher tilt angles, i.e., a stronger in-plane field, and points towards a more robust Wigner solid phase

Our experimental data show that the electron system enters a correlation regime, which reflects the character of both solid and liquid phases for ν < 1/2 and can likely be the features of a non-trivial phase transition in the electron system occupying the lowest LL. Our experimental results are interpreted within the CF approach, which has recently attracted renewed attention from theory predicting that the CF can be Dirac particles45,46,47,48. This also introduces an exciting perspective for ZnO studies. Our experimental results display the composite fermion paradigm in a system distinct from conventional semiconductor systems and address the question on how the charge carrier system translates between liquid and solid phases.



The sample under study is a MgZnO/ZnO heterostructure (a sequence of about 500-nm thick epitaxial ZnO film (buffer layer) and 250-nm thick MgZnO (capping layer) grown on ZnO substrate) with a charge carrier density n = 1.7 × 1011 cm−2 and a mobility μ = 600,000 cm2V−1s−1 at the base temperature of our dilution refrigerator T = 60 mK. The LL mixing for this charger carrier density is κ = 4.2 at ν = 1/2.

Magnetotransport in tilted magnetic field

The sample is mounted on a rotating stage allowing in-situ sample rotation in the magnetic field. The tilt angle θ is determined from the shift of Rxx resistance minima of the well-known fractional quantum Hall states.

Data availability

The data that support the findings of this study are available from the corresponding author upon request.

Additional information

Publisher's note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.


  1. 1.

    Das Sarma, S. & Pinczuk, A. Perspective in quantum Hall effects (John Wiley, New Jersey, 1997).

  2. 2.

    Halperin, B. I., Lee, P. A. & Read, N. Theory of the half-filled Landau level. Phys. Rev. B 47, 7312–7343 (1993).

  3. 3.

    Jain, J. K. Composite-fermion approach for the fractional quantum Hall effect. Phys. Rev. Lett. 63, 199–202 (1989).

  4. 4.

    Santos, M. B. et al. Observation of a reentrant insulating phase near the 1/3 fractional quantum Hall liquid in a two-dimensional hole system. Phys. Rev. Lett. 68, 1188–1191 (1992).

  5. 5.

    Santos, M. B. et al. Effect of Landau-level mixing on quantum-liquid and solid states of two-dimensional hole systems. Phys. Rev. B 46, 13639–13642 (1992).

  6. 6.

    Kozuka, Y. et al. Insulating phase of a two-dimensional electron gas in MgxZn1−xO/ZnO heterostructures below ν = (1/3). Phys. Rev. B 84, 033304 (2011).

  7. 7.

    Halperin, B. I. & Nelson, D. R. Theory of two-dimensional melting. Phys. Rev. Lett. 41, 121–124 (1978).

  8. 8.

    Morf, R. H. Temperature dependence of the shear modulus and melting of the two-dimensional electron solid. Phys. Rev. Lett. 43, 931–935 (1979).

  9. 9.

    Young, A. P. Melting and the vector coulomb gas in two dimensions. Phys. Rev. B 19, 1855–1866 (1979).

  10. 10.

    Rees, DavidG. et al. Structural order and melting of a quasi-one-dimensional electron system. Phys. Rev. B 94, 045139 (2016).

  11. 11.

    Strandburg, K. J. Two-dimensional melting. Rev. Mod. Phys. 60, 161–207 (1988).

  12. 12.

    Spivak, B. & Kivelson, S. A. Phases intermediate between a two-dimensional electron liquid and Wigner crystal. Phys. Rev. B 70, 155114 (2004).

  13. 13.

    Spivak, B., Kravchenko, S. V., Kivelson, S. A. & Gao, X. P. A. Colloquium:transport in strongly correlated two-dimensional electron fluids. Rev. Mod. Phys. 82, 1743–1766 (2010).

  14. 14.

    Archer, A. C. & Jain, J. K. Static and dynamic properties of type-II composite fermion Wigner crystals. Phys. Rev. B 84, 115139 (2011).

  15. 15.

    Chang, C.-C., Jeon, G. S. & Jain, J. K. Microscopic verification of topological electron-vortex binding in the lowest Landau level crystal state. Phys. Rev. Lett. 94, 016809 (2005).

  16. 16.

    Yi, H. & Fertig, H. A. Laughlin-Jastrow-correlated Wigner crystal in a strong magnetic field. Phys. Rev. B 58, 4019–4027 (1998).

  17. 17.

    Narevich, R., Murthy, G. & Fertig, H. A. Hamiltonian theory of the composite-fermion Wigner crystal. Phys. Rev. B 64, 245326 (2001).

  18. 18.

    Archer, A.-C., Park, K. & Jain, J. K. Competing crystal phases in the lowest Landau level. Phys. Rev. Lett. 111, 146804 (2013).

  19. 19.

    Zhao, Jianyun, Zhang, Yuhe & Jain, J. K. Crystallization in the fractional quantum Hall regime induced by Landau-level mixing. Phys. Rev. Lett. 121, 116802 (2018).

  20. 20.

    Chen, Y. P. et al. Evidence for two different solid phases of two-dimensional electrons in high magnetic fields. Phys. Rev. Lett. 93, 206805 (2004).

  21. 21.

    Zhu, H. et al. Observation of a pinning mode in a Wigner solid with ν = 1/3 fractional quantum Hall excitations. Phys. Rev. Lett. 105, 126803 (2010).

  22. 22.

    Liu, Y. et al. Fractional quantum Hall effect and Wigner crystal of interacting composite fermions. Phys. Rev. Lett. 113, 246803 (2014).

  23. 23.

    Zhang, C., Du, R.-R., Manfra, M. J., Pfeiffer, L. N. & West, K. W. Transport of a sliding Wigner crystal in the four flux composite fermion regime. Phys. Rev. B 92, 075434 (2015).

  24. 24.

    Jang, J., Hunt, B. M., Pfeiffer, L. N., West, K. W. & Ashoori, R. C. Sharp tunnelling resonance from the vibrations of an electronic Wigner crystal. Nat. Phys. 13, 340–344 (2016).

  25. 25.

    Maryenko, D. et al. Temperature-dependent magnetotransport around ν = 1/2 in ZnO heterostructures. Phys. Rev. Lett. 108, 186803 (2012).

  26. 26.

    Falson, J. et al. Even-denominator fractional quantum Hall physics in ZnO. Nat. Phys. 11, 347–351 (2015).

  27. 27.

    Li, W., Luhman, D. R., Tsui, D. C., Pfeiffer, L. N. & West, K. W. Observation of reentrant phases induced by short-range disorder in the lowest Landau level of AlxGa1−xAs/Al0.32Ga0.68As heterostructures. Phys. Rev. Lett. 105, 076803 (2010).

  28. 28.

    Moon, B.-H., Engel, L. W., Tsui, D. C., Pfeiffer, L. N. & West, K. W. Pinning modes of high-magnetic-field Wigner solids with controlled alloy disorder. Phys. Rev. B 89, 075310 (2014).

  29. 29.

    Kärcher, D. F. et al. Observation of microwave induced resistance and photovoltage oscillations in MgZnO/ZnO heterostructures. Phys. Rev. B 93, 041410 (2016).

  30. 30.

    Uchida, M. et al. Calibration and control of in-plane Mg doping distribution in MgZnO/ZnO heterostructures grown by molecular beam epitaxy. Jpn. J. Appl. Phys. 54, 028004 (2015).

  31. 31.

    Maryenko, D. et al. Polarization-dependent Landau level crossing in a two-dimensional electron system in a MgZnO/ZnO heterostructure. Phys. Rev. B 90, 245303 (2014).

  32. 32.

    Pan, W., Csáthy, G. A., Tsui, D. C., Pfeiffer, L. N. & West, K. W. Transition from a fractional quantum Hall liquid to an electron solid at Landau level filling ν = (1/3) in tilted magnetic fields. Phys. Rev. B 71, 035302 (2005).

  33. 33.

    Piot, B. A. et al. Wigner crystallization in a quasi-three-dimensional electronic system. Nat. Phys. 4, 936–939 (2008).

  34. 34.

    Das Sarma, S. & Hwang, E. H. Parallel magnetic field induced giant magnetoresistance in low density quasi-two-dimensional layers. Phys. Rev. Let. 84, 5596–5599 (2000).

  35. 35.

    Solovyev, V. A. et al. Optical probing of MgZnO/ZnO heterointerface confinement potential energy levels. Appl. Phys. Lett. 106, 082102 (2015).

  36. 36.

    Kunze, U. et al. Effective-mass change of electrons in Si inversion layers under parallel magnetic fields. Phys. Rev. B 35, 9168–9173 (1987).

  37. 37.

    Smrčka, L. et al. Cyclotron effective mass of a two-dimensional electron layer at the GaAs/AlxGa1−xAs heterojunction subject to in-plane magnetic fields. Phys. Rev. B 51, 18011–18014 (1995).

  38. 38.

    Smreka, L. & Jungwirth, T. The single-layer/bilayer transition of electron systems in AlGaAs/GaAs/AlGaAs quantum wells subject to in-plane magnetic fields. J. Phys. Condens. Matter 7, 3721–3732 (1995).

  39. 39.

    Kamburov, D. et al. Composite fermions with tunable Fermi contour anisotropy. Phys. Rev. Lett. 110, 206801 (2013).

  40. 40.

    Kamburov, D. et al. Fermi contour anisotropy of GaAs electron-flux composite fermions in parallel magnetic fields. Phys. Rev. B 89, 085304 (2014).

  41. 41.

    Fang, F. F. & Stiles, P. J. Effects of a tilted magnetic field on a two-dimensional electron gas. Phys. Rev. 174, 823–828 (1968).

  42. 42.

    Gee, P. J. et al. Composite fermions in tilted magnetic fields and the effect of the confining potential width on the composite-fermion effective mass. Phys. Rev. B 54, R14313–R14316 (1996).

  43. 43.

    Zhang, F. C. & Das Sarma, S. Excitation gap in the fractional quantum Hall effect: finite layer thickness corrections. Phys. Rev. B 33, 2903–2905 (1986).

  44. 44.

    Rokhinson, L. P., Su, B. & Goldman, V. J. Logarithmic temperature dependence of conductivity at half-integer filling factors: Evidence for interaction between composite fermions. Phys. Rev. B 52, R11588–R11590 (1995).

  45. 45.

    Geraedts, S. D. et al. The half-filled Landau level: the case for Dirac composite fermions. Science 352, 197–201 (2016).

  46. 46.

    Wang, C. & Senthil, T. Composite Fermi liquids in the lowest Landau level. Phys. Rev. B 94, 245107 (2016).

  47. 47.

    Son, D. T. Is the composite fermion a Dirac particle? Phys. Rev. X 5, 031027 (2015).

  48. 48.

    Wang, C. & Senthil, T. Half-filled Landau level, topological insulator surfaces, and three-dimensional quantum spin liquids. Phys. Rev. B 93, 085110 (2016).

Download references


We acknowledge the support of the HFML-RU/FOM member of the European Magnetic Field Laboratory (EMFL). This work was partly supported by JST CREST No. JPMJCR16F1. We would like to thank M. Kawamura, A. S. Mishchenko, M. Ueda, K. von Klitzing, N. Nagaosa, and J. K. Jain for fruitful discussions and comments.

Author information

D.M. and M.K. initiated the project. M.K. supervised the project. D.M. conceived and designed the experiment. J.F. and Y.K. fabricated the samples. D.M., A.M., J.B., and U.Z. performed the high-field magnetotransport experiment and analyzed the data. D.M. and U.Z. wrote the paper with input from all co-authors.

Competing interests

The authors declare no competing interests.

Correspondence to D. Maryenko.

Electronic supplementary material

  1. Supplementary Information

  2. Peer Review File

Rights and permissions

Creative Commons BY

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as 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. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit

About this article


By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.