2022
DOI: 10.1103/physrevb.105.l161402
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Enhanced critical field and anomalous metallic state in two-dimensional centrosymmetric 1TWS2

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Cited by 7 publications
(4 citation statements)
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“…This results in an out-of-plane upper critical magnetic field 0 of 5.3 T and an in-plane GL superconducting coherence length of ξ GL (0) ∼7.9 nm. Fitting the in-plane H c 2 versus T c yields an in-plane upper critical magnetic field 0 of 30.1 T. Similar to the recently reported mechanically exfoliated few-layer 1T′-WS 2 ( 46 ) and printed NbSe 2 film ( 6 ), the 0 of the printed 1T′-WS 2 film is very high, far beyond its Bardeen-Schrieffer-Cooper Pauli paramagnetic limit of 13.1 T ( H p ∼1.84 T c ) ( 47 ). However, the symmetry of the centrosymmetric 1T′ structure of WS 2 is fundamentally different from the noncentrosymmetric hexagonal structure of NbSe 2 , where Ising-type superconductivity is responsible for exceeding the Pauli limit ( 6 , 45 ).…”
Section: Resultssupporting
confidence: 83%
“…This results in an out-of-plane upper critical magnetic field 0 of 5.3 T and an in-plane GL superconducting coherence length of ξ GL (0) ∼7.9 nm. Fitting the in-plane H c 2 versus T c yields an in-plane upper critical magnetic field 0 of 30.1 T. Similar to the recently reported mechanically exfoliated few-layer 1T′-WS 2 ( 46 ) and printed NbSe 2 film ( 6 ), the 0 of the printed 1T′-WS 2 film is very high, far beyond its Bardeen-Schrieffer-Cooper Pauli paramagnetic limit of 13.1 T ( H p ∼1.84 T c ) ( 47 ). However, the symmetry of the centrosymmetric 1T′ structure of WS 2 is fundamentally different from the noncentrosymmetric hexagonal structure of NbSe 2 , where Ising-type superconductivity is responsible for exceeding the Pauli limit ( 6 , 45 ).…”
Section: Resultssupporting
confidence: 83%
“…Here, C is a dimensionless constant, R n is the sheet resistance of the normal state, and H c2 is the perpendicular upper critical field. Besides ZrNCl, experimental signatures of the anomalous metal states have also been reported in other crystalline nanodevices made of exfoliated 2D materials, such as WTe 2 [149], TiSe 2 [150], MoS 2 [151], TaSe 2 [152], Li x TiSe 2 [153], and WS 2 [154] (see table 4 for a list of representative anomalous metal states and the tuning methods).…”
Section: Experimental Signatures In Strongly Disordered 2d Supercondu...mentioning
confidence: 77%
“…The developments of film growth and nanofabrication technique in recent decades have made new opportunity to study the quantum phase transitions and the anomalous metal states in crystalline superconducting films and nanodevices. In this section, we focus on recent progress on the signatures of anomalous metal states observed in 2D crystalline superconductors [32,38,[149][150][151][152][153][154][155][156][157][158][159][160][161][162].…”
Section: Experimental Signatures In Strongly Disordered 2d Supercondu...mentioning
confidence: 99%
“…However, this method usually generates low yields of the desired products. Because the physicochemical quality of exfoliated TMD nanosheets remains the same as that of the bulk, mechanical exfoliation is an ideal platform for studying properties in the extremely thin regime or transferring films to substrates for further fabricating devices. , However, during the monolayer transfer, the exposure to ambient air and removal of the adhesive tape in solution probably stain the basal plane of the exfoliated ultrathin TMD nanosheet via small molecules or organic residues, which would induce the degradation of properties by shifting the Raman frequency and weakening the PL emission . This issue is well addressed using dry transfer via PDMS stamping and thermal-release tape instead of conventional Scotch tape. , Dry transfer exploits the strong interaction between the TMD monolayer and substrate, such as MoS 2 and gold.…”
Section: Direct Synthesis Of Ultrathin 1t/1t′ Tmd Nanosheetsmentioning
confidence: 99%