2022
DOI: 10.3390/ma15207372
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Destabilization of the Charge Density Wave and the Absence of Superconductivity in ScV6Sn6 under High Pressures up to 11 GPa

Abstract: RV6Sn6 (R = Sc, Y, or rare earth) is a new family of kagome metals that have a similar vanadium structural motif as AV3Sb5 (A = K, Rb, Cs) compounds. Unlike AV3Sb5, ScV6Sn6 is the only compound among the series of RV6Sn6 that displays a charge density wave (CDW) order at ambient pressure, yet it shows no superconductivity (SC) at low temperatures. Here, we perform a high-pressure transport study on the ScV6Sn6 single crystal to track the evolutions of the CDW transition and to explore possible SC. In contrast … Show more

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Cited by 28 publications
(24 citation statements)
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References 57 publications
(57 reference statements)
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“…The measurement was performed in a Quantum Design physical property measurement system (PPMS). Good metallic behavior is observed in resistivity measurements (shown in Figure 1 All the sample fundamental characterizations are identified with the previous report 24,25 .…”
Section: Resultssupporting
confidence: 86%
See 1 more Smart Citation
“…The measurement was performed in a Quantum Design physical property measurement system (PPMS). Good metallic behavior is observed in resistivity measurements (shown in Figure 1 All the sample fundamental characterizations are identified with the previous report 24,25 .…”
Section: Resultssupporting
confidence: 86%
“…X-ray diffraction verified that an extra three-dimensional 3×3×3 periodic CDW lattice modulation forms below this temperature. High-pressure transport measurements indicate that the CDW order can be suppressed completely but no SC emerges yet under high pressures up to 11 GPa 25 . Unlike AV 3 Sb 5 systems, there are two kagome sheets per unit cell separated by alternating ScSn 2 and Sn 2 lay-ers in ScV 6 Sn 6 .…”
Section: Introductionmentioning
confidence: 97%
“…Furthermore, it is interesting to consider whether the competition between CDW instabilities in ScV 6 Sn 6 could be tilted in favor of q * -CDW via external tuning. In this regard, electrical transport measurements in pressurized ScV 6 Sn 6 reveal that the sharp drop in resistivity associated with q s -CDW persists up to ∼ 2.0 GPa, beyond which it is suddenly replaced by a much weaker kink in resistivity, before becoming fully suppressed at ∼ 2.4 GPa [49]. The sudden qualitative change in resistivity anomaly above ∼ 2.0 GPa is suggestive of a change in the ground state, and the much less pronounced resistivity anomaly between ∼ 2.0 GPa and ∼ 2.4 GPa suggests the associated transition being second-order.…”
Section: Discussionmentioning
confidence: 97%
“…GPa due to destabilization and disappearance of the CDW. 24 It is tempting to claim that this destabilization corresponds to P C,1 , but we must remember that our measurements are performed at room temperature -where the CDW is not fully developed. The recently reported short range CDW provides a way forward.…”
Section: Resultsmentioning
confidence: 97%