2021
DOI: 10.1038/s41586-021-04021-0
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Artificial heavy fermions in a van der Waals heterostructure

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Cited by 111 publications
(95 citation statements)
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“…In addition, we perform the magnetic field dependent d I /d V measurements at 0.6 K. As shown in Fig. 3c , no clear splitting of the Kondo resonance peak is observed with external magnetic field up to 8.5 T. However, the Kondo resonance peak in the single layer 1 T -TaS 2 is clearly split with 10 T magnetic field 20 . The difference is that the width of Kondo resonance peak in Fig.…”
Section: Resultsmentioning
confidence: 92%
See 1 more Smart Citation
“…In addition, we perform the magnetic field dependent d I /d V measurements at 0.6 K. As shown in Fig. 3c , no clear splitting of the Kondo resonance peak is observed with external magnetic field up to 8.5 T. However, the Kondo resonance peak in the single layer 1 T -TaS 2 is clearly split with 10 T magnetic field 20 . The difference is that the width of Kondo resonance peak in Fig.…”
Section: Resultsmentioning
confidence: 92%
“…More surprisingly, the very recent study demonstrates that when the monolayer 1 T -TaS 2 is grown on the monolayer metallic 1 H -TaS 2 by molecular beam epitaxy, the Kondo resonance peak appears in the 1 T -TaS 2 layer 20 , which confirms the local moment formation and possible cluster Mott physics in the monolayer 1 T -TaS 2 . If the insulating gap of the Type-II surface in the bulk 1 T -TaS 2 is truly a Mott-insulating gap, there should be local magnetic moment formation that is similar as the monolayer 1 T -TaS 2 .…”
Section: Introductionmentioning
confidence: 74%
“…[4] Recently, localized spins have been observed in the charge density wave (CDW) superlattice of 1T-phase single-layer group-V TMDs materials, such as single-layer 1T-TaS2, 1T-TaSe2 and 1T-NbSe2, and the Kondo lattice emerges when they couple to the two-dimensional metallic layers. [5][6][7] Stacking the group-V TMDs layers hosting Kondo lattice with the two-dimensional superconductors would provide a new platform for exploring the interplay between superconductivity and Kondo lattice. 4Hb-TaS2 is a superconducting van der Waals material consisting of an alternate stacking of 1T-TaS2 and 1H-TaS2 layers [Fig.…”
mentioning
confidence: 99%
“…We now elaborate on the material we will focus on in our discussion, 1T-TaS 2 . 1T-TaS 2 hosts a chargedensity-wave (CDW) instability leading to the formation of the Star-of-David (SOD) unit cell with 13 atoms at low temperature [23,[49][50][51][52]. The CDW as well as spinorbit coupling (SOC) result in a half-filled narrow band at the Fermi energy, with a bandwidth of a few 10meV [53].…”
mentioning
confidence: 99%