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Artificial heavy fermions in a van der Waals heterostructure


Heavy-fermion systems represent one of the paradigmatic strongly correlated states of matter1,2,3,4,5. They have been used as a platform for investigating exotic behaviour ranging from quantum criticality and non-Fermi liquid behaviour to unconventional topological superconductivity4,5,6,7,8,9,10,11,12. The heavy-fermion phenomenon arises from the exchange interaction between localized magnetic moments and conduction electrons leading to Kondo lattice physics, and represents one of the long-standing open problems in quantum materials3. In a Kondo lattice, the exchange interaction gives rise to a band with heavy effective mass. This intriguing phenomenology has so far been realized only in compounds containing rare-earth elements with 4f or 5f electrons1,4,13,14. Here we realize a designer van der Waals heterostructure where artificial heavy fermions emerge from the Kondo coupling between a lattice of localized magnetic moments and itinerant electrons in a 1T/1H-TaS2 heterostructure. We study the heterostructure using scanning tunnelling microscopy and spectroscopy and show that depending on the stacking order of the monolayers, we can reveal either the localized magnetic moments and the associated Kondo effect, or the conduction electrons with a heavy-fermion hybridization gap. Our experiments realize an ultimately tunable platform for future experiments probing enhanced many-body correlations, dimensional tuning of quantum criticality and unconventional superconductivity in two-dimensional artificial heavy-fermion systems15,16,17.

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Fig. 1: Artificial heavy-fermion heterostructure.
Fig. 2: Kondo resonance in a 1T/1H-TaS2 vertical heterostructure.
Fig. 3: Heavy-fermion hybridization gap in a 1H/1T-TaS2 vertical heterostructure.

Data availability

All of the data supporting the findings are available from the corresponding authors upon request.


  1. 1.

    Stewart, G. R. Heavy-fermion systems. Rev. Mod. Phys. 56, 755–787 (1984).

    ADS  CAS  Google Scholar 

  2. 2.

    Yazdani, A., da Silva Neto, E. H. & Aynajian, P. Spectroscopic imaging of strongly correlated electronic states. Annu. Rev. Condens. Matter Phys. 7, 11–33 (2016).

    ADS  Google Scholar 

  3. 3.

    Dzero, M., Xia, J., Galitski, V. & Coleman, P. Topological Kondo insulators. Annu. Rev. Condens. Matter Phys.7, 249–280 (2016).

    ADS  CAS  Google Scholar 

  4. 4.

    Wirth, S. & Steglich, F. Exploring heavy fermions from macroscopic to microscopic length scales. Nat. Rev. Mater. 1, 16051 (2016).

    ADS  CAS  Google Scholar 

  5. 5.

    Jiao, L. et al. Chiral superconductivity in heavy-fermion metal UTe2. Nature 579, 523–527 (2020).

    ADS  CAS  PubMed  Google Scholar 

  6. 6.

    Pfleiderer, C. et al. Partial order in the non-Fermi-liquid phase of MnSi. Nature 427, 227–231 (2004).

    ADS  CAS  PubMed  Google Scholar 

  7. 7.

    Stewart, G. R. Non-Fermi-liquid behavior in d- and f-electron metals. Rev. Mod. Phys. 73, 797–855 (2001).

    ADS  CAS  Google Scholar 

  8. 8.

    Löhneysen, H. V., Rosch, A., Vojta, M. & Wölfle, P. Fermi-liquid instabilities at magnetic quantum phase transitions. Rev. Mod. Phys. 79, 1015–1075 (2007).

    ADS  Google Scholar 

  9. 9.

    Gegenwart, P., Si, Q. & Steglich, F. Quantum criticality in heavy-fermion metals. Nat. Phys. 4, 186–197 (2008).

    CAS  Google Scholar 

  10. 10.

    Aynajian, P. et al. Visualizing heavy fermions emerging in a quantum critical Kondo lattice. Nature 486, 201–206 (2012).

    ADS  CAS  PubMed  Google Scholar 

  11. 11.

    Allan, M. P. et al. Imaging Cooper pairing of heavy fermions in CeCoIn5. Nat. Phys. 9, 468–473 (2013).

    CAS  Google Scholar 

  12. 12.

    Zhou, B. B. et al. Visualizing nodal heavy fermion superconductivity in CeCoIn5. Nat. Phys. 9, 474–479 (2013).

    CAS  Google Scholar 

  13. 13.

    Chen, C., Sodemann, I. & Lee, P. A. Competition of spinon Fermi surface and heavy Fermi liquid states from the periodic Anderson to the Hubbard model. Phys. Rev. B 103, 085128 (2021).

    ADS  CAS  Google Scholar 

  14. 14.

    Ramires, A. & Lado, J. L. Emulating heavy fermions in twisted trilayer graphene. Phys. Rev. Lett. 127, 026401 (2021).

    ADS  CAS  PubMed  Google Scholar 

  15. 15.

    Neumann, M., Nyéki, J., Cowan, B. & Saunders, J. Bilayer 3He: a simple two-dimensional heavy-fermion system with quantum criticality. Science 317, 1356–1359 (2007).

    ADS  CAS  PubMed  Google Scholar 

  16. 16.

    Shishido, H. et al. Tuning the dimensionality of the heavy fermion compound CeIn3. Science 327, 980–983 (2010).

    ADS  CAS  PubMed  Google Scholar 

  17. 17.

    Mizukami, Y. et al. Extremely strong-coupling superconductivity in artificial two-dimensional Kondo lattices. Nat. Phys. 7, 849–853 (2011).

    CAS  Google Scholar 

  18. 18.

    Geim, A. K. & Grigorieva, I. V. Van der Waals heterostructures. Nature 499, 419–425 (2013).

    CAS  PubMed  Google Scholar 

  19. 19.

    Liu, Y. et al. Van der Waals heterostructures and devices. Nat. Rev. Mater. 1, 16042 (2016).

    ADS  CAS  Google Scholar 

  20. 20.

    Novoselov, K. S., Mishchenko, A., Carvalho, A. & Castro Neto, A. H. 2D materials and van der Waals heterostructures. Science 353, aac9439 (2016).

    CAS  PubMed  Google Scholar 

  21. 21.

    Kennes, D. M. et al. Moiré heterostructures as a condensed-matter quantum simulator. Nat. Phys. 17, 155–163 (2021).

    CAS  Google Scholar 

  22. 22.

    Andrei, E. Y. et al. The marvels of moiré materials. Nat. Rev. Mater. 6, 201–206 (2021).

    ADS  CAS  Google Scholar 

  23. 23.

    Ugeda, M. M. et al. Characterization of collective ground states in single-layer NbSe2. Nat. Phys. 12, 92–97 (2015).

    Google Scholar 

  24. 24.

    de la Barrera, S. C. et al. Tuning Ising superconductivity with layer and spin–orbit coupling in two-dimensional transition-metal dichalcogenides. Nat. Commun. 9, 1427 (2018).

    ADS  PubMed  PubMed Central  Google Scholar 

  25. 25.

    Law, K. T. & Lee, P. A. 1T-TaS2 as a quantum spin liquid. Proc. Natl Acad. Sci. USA 114, 6996–7000 (2017).

    ADS  CAS  PubMed  PubMed Central  Google Scholar 

  26. 26.

    Cho, D. et al. Nanoscale manipulation of the Mott insulating state coupled to charge order in 1T-TaS2. Nat. Commun. 7, 10453 (2016).

    ADS  CAS  PubMed  PubMed Central  Google Scholar 

  27. 27.

    Qiao, S. et al. Mottness collapse in 1T-TaS2−xSex transition-metal dichalcogenide: an interplay between localized and itinerant orbitals. Phys. Rev. X 7, 041054 (2017).

    Google Scholar 

  28. 28.

    Chen, Y. et al. Strong correlations and orbital texture in single-layer 1T-TaSe2. Nat. Phys. 16, 218–224 (2020).

    CAS  Google Scholar 

  29. 29.

    Ruan, W. et al. Evidence for quantum spin liquid behaviour in single-layer 1T-TaSe2 from scanning tunnelling microscopy. Nat. Phys. 17, 1154–1161 (2021).

  30. 30.

    Kratochvilova, M. et al. The low-temperature highly correlated quantum phase in the charge-density-wave 1T-TaS2 compound. npj Quant. Mater. 2, 42 (2017).

    ADS  Google Scholar 

  31. 31.

    Coqblin, B. & Schrieffer, J. R. Exchange interaction in alloys with cerium impurities. Phys. Rev. 185, 847–853 (1969).

    ADS  CAS  Google Scholar 

  32. 32.

    Wen, C. et al. Roles of the narrow electronic band near the Fermi level in 1T-TaS2-related layered materials. Phys. Rev. Lett. 126, 256402 (2021).

    ADS  CAS  PubMed  Google Scholar 

  33. 33.

    Zhang, Y.-H. et al. Temperature and magnetic field dependence of a Kondo system in the weak coupling regime. Nat. Commun. 4, 2110 (2013).

    ADS  PubMed  Google Scholar 

  34. 34.

    Ryu, H. et al. Persistent charge-density-wave order in single-layer TaSe2. Nano Lett. 18, 689–694 (2018).

    ADS  CAS  PubMed  Google Scholar 

  35. 35.

    McMillan, W. L. & Mochel, J. Electron tunneling experiments on amorphous Ge1−xAux. Phys. Rev. Lett. 46, 556–557 (1981).

    ADS  CAS  Google Scholar 

  36. 36.

    Ernst, S. et al. Emerging local Kondo screening and spatial coherence in the heavy-fermion metal YbRh2Si2. Nature 474, 362–366 (2011).

    CAS  PubMed  Google Scholar 

  37. 37.

    Röβler, S. et al. Hybridization gap and Fano resonance in SmB6. Proc. Natl Acad. Sci. USA 111, 4798–4802 (2014).

    ADS  Google Scholar 

  38. 38.

    Bose, S. & Ayyub, P. A review of finite size effects in quasi-zero dimensional superconductors. Rep. Prog. Phys. 77, 116503 (2014).

    ADS  PubMed  Google Scholar 

  39. 39.

    Ganguli, S. C., Vaňo, V., Kezilebieke, S., Lado, J. L. & Liljeroth, P. Controlling correlations in NbSe2 via quantum confinement. Preprint at (2020).

  40. 40.

    Kouwenhoven, L. P., Austing, D. G. & Tarucha, S. Few-electron quantum dots. Rep. Prog. Phys. 64, 701–736 (2001).

    ADS  CAS  Google Scholar 

  41. 41.

    She, J.-H., Kim, C. H., Fennie, C. J., Lawler, M. J. & Kim, E.-A. Topological superconductivity in metal/quantum-spin-ice heterostructures. npj Quant. Mater. 2, 64 (2017).

    ADS  Google Scholar 

  42. 42.

    Ribak, A. et al. Chiral superconductivity in the alternate stacking compound 4Hb-TaS2. Sci. Adv. 6, eaax9480 (2020).

    ADS  CAS  PubMed  PubMed Central  Google Scholar 

  43. 43.

    Seiro, S. et al. Evolution of the Kondo lattice and non-Fermi liquid excitations in a heavy-fermion metal. Nat. Commun. 9, 3324 (2018).

    ADS  CAS  PubMed  PubMed Central  Google Scholar 

  44. 44.

    Hall, J. et al. Molecular beam epitaxy of quasi-freestanding transition metal disulphide monolayers on van der Waals substrates: a growth study. 2D Mater. 5, 025005 (2018).

    Google Scholar 

  45. 45.

    Lin, H. et al. Growth of atomically thick transition metal sulfide films on graphene/6H-SiC(0001) by molecular beam epitaxy. Nano Res. 11, 4722–4727 (2018).

    CAS  Google Scholar 

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This research made use of the Aalto Nanomicroscopy Center (Aalto NMC) facilities and was supported by the European Research Council (ERC-2017-AdG no. 788185 “Artificial Designer Materials”), the Academy of Finland (Academy professor funding nos. 318995 and 320555, Academy postdoctoral researcher no. 309975, Academy research fellow nos. 331342 and 336243) and the Jane and Aatos Erkko Foundation. We acknowledge the computational resources provided by the Aalto Science-IT project.

Author information




V.V., J.L.L., S.K. and P.L. conceived the experiment, V.V., M.A., S.C.G. and S.K. carried out the sample growth and the low-temperature STM experiments. V.V. analysed the STM data. G.C. and J.L.L. developed the theoretical model. V.V., J.L.L. and P.L. wrote the manuscript with input from all co-authors.

Corresponding authors

Correspondence to Jose L. Lado or Peter Liljeroth.

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Competing interests

The authors declare no competing interests.

Additional information

Peer review information Nature thanks Milan Allan, Stefan Kirchner and the other, anonymous, reviewer(s) for their contribution to the peer review of this work. Peer reviewer reports are available.

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

Extended data figures and tables

Extended Data Fig. 1 Grid spectroscopy measurement of a 1T-TaS2/1H-TaS2 heterostructure.

a, STM image of a 1T/1H-TaS2 heterostructure (V = 200 mV and I = 10 pA). b, Tunneling spectra across the red line shown in (a), starting from top left. We observe a Kondo peak located on each of the CDW centers. c, dI/dV map at V = 0 mV measured on the area shown in (a) showing the Kondo lattice. Due to a Kondo peak, there is a higher dI/dV intensity on each of the CDW centers. Middle and bottom rows: dI/dV maps at given bias voltages, all measured on the area shown in (a) and using the same colour scale as in (c). Each of the dI/dV curves was normalized by dividing it by its mean value. Single tunneling spectra on different CDW centers and on a different area are shown in Extended Data Fig. 2.

Extended Data Fig. 2 Single tunneling spectra in the centre of different CDW unit cells.

Left: STM image of a 1T-TaS2/1H-TaS2 heterostructure (V = 200 mV and I = 20 pA). Right: tunneling spectra measured at locations highlighted by the same-coloured dots on the STM image, spectra are vertically offset for clarity.

Extended Data Fig. 3 Fitting of the Kondo resonances.

Left: Temperature dependence of a Kondo resonance in tunneling spectroscopy (black lines), and their respective fits to the Fano lineshape (red lines). The spectra are vertically offset for clarity. Right: Table of the fit parameters.

Extended Data Fig. 4 Thermal broadening of the Kondo resonance.

Tunneling spectroscopy of a Kondo resonance at 300 mK (blue), 18 K (green), and a simulated tunneling spectrum at 18 K (red), where the 300 mK spectrum was taken as the density of states.

Extended Data Fig. 5 Tunneling spectra of 1H-TaS2 on different substrates.

Tunneling spectroscopy of 1H-TaS2 on HOPG (purple line), bilayer 1H-TaS2 (blue line) and 1H-TaS2 on monolayer 1T-TaS2 (green line). The spectra are measured on positions highlighted by the same-coloured dots in the STM image on the left. The spectra exhibit a dip around the Fermi level, but while 1H-TaS2 on HOPG (purple line) and bilayer 1H-TaS2 (blue line) have finite zero-bias conductance, only the spectroscopy of 1H/1T-TaS2 (green line) exhibits a heavy-fermion gap with zero conductance at zero bias.

Extended Data Fig. 6 Examples of different 1H/1T-TaS2 heterostructures.

STM images (left) and corresponding tunneling spectra measured on top of a heterostructure (right). Purple dots highlight the positions, where the tunneling spectra were taken. All the heterostructures exhibit a heavy-fermion gap with zero conductance at zero bias and approximately the same gap width, regardless of the island size.

Extended Data Fig. 7 Tunneling spectroscopy across middle of the 1H/1T-TaS2 island.

a, STM image of a 1H/1T-TaS2 vertical heterostructure (V = 900 mV and I = 20 pA). b, Tunneling spectra across the red line shown in (a). c, Average tunneling spectrum from the spectra across line in (b).

Extended Data Fig. 8 Spatial dependence of the heavy-fermion gap.

a, STM image of a 1H-TaS2/1T-TaS2 heterostructure (V = 50 mV and I = 500 pA). Larger scale topographic image is shown in Extended Data Fig. 9e. b, Tunneling spectra across the red line shown in (a). c, dI/dV map at V = 0 mV measured on the area shown in (a). Middle and bottom rows: dI/dV maps at given bias voltages, all measured on the area shown in (a) and using the same colour scale as in (c).

Extended Data Fig. 9 High-resolution STM images of different heterostructures.

a, c, e, g, Large area STM images. b, STM image of a 1H-TaS2 on HOPG (V = 50 mV and I = 500 pA). Inset shows fast Fourier transform of the image. d, STM image of a monolayer 1T-TaS2 on HOPG (V = 1 V and I = 20 pA). f, STM image of a 1H/1T-TaS2 vertical heterostructure (V = 50 V and I = 500 pA). Inset shows fast Fourier transform of the image. h, STM image of a 1T/1H-TaS2 vertical heterostructure (V = 0.3 V and I = 50 pA). 1H-TaS2 on HOPG exhibits a strong 3×3 CDW, while 1H-TaS2 on 1T-TaS2 shows no signs of CDW. Both 1T-TaS2 on HOPG and 1T-TaS2 on 1H-TaS2 exhibit a strong √13×√13 CDW.

Extended Data Fig. 10 Magnetic field dependence of a heavy-fermion gap.

Tunneling spectroscopy of a heavy-fermion gap measured on a 1H/1T-TaS2 vertical heterostructure at different applied magnetic fields, the spectra are vertically offset for clarity.

Supplementary information

Supplementary Information

This file contains Supplementary Sections 1–3: detailed description of the theoretical model; discussion on the comparison with the magnetic field dependence of natural heavy-fermion compounds; discussion on the potential further probes of the heavy-fermion regime.

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Vaňo, V., Amini, M., Ganguli, S.C. et al. Artificial heavy fermions in a van der Waals heterostructure. Nature 599, 582–586 (2021).

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