2020
DOI: 10.1016/j.apmt.2019.100532
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Pressure-induced band-gap closure and metallization in two-dimensional transition metal halide CdI2

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Cited by 12 publications
(11 citation statements)
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“…Figure 2e presents the typical Raman spectra of CdI 2 flakes grown on mica substrate. Obviously, there are two prominent and strong characteristic peaks around 45 and 110 cm −1 , which correspond to the in-plane (E g ) and the out-of-plane (A 1g ) phonon vibration mode, respectively, in consist with the recently reported 2D CdI 2 crystals [43,44]. The inset is the representative Raman intensity maps of E g and A 1g modes of a typical CdI 2 triangular flake, indicating highly uniform crystalline quality throughout the entire flake.…”
Section: Growth and Characterization Of Layered CDI 2 Flakessupporting
confidence: 70%
“…Figure 2e presents the typical Raman spectra of CdI 2 flakes grown on mica substrate. Obviously, there are two prominent and strong characteristic peaks around 45 and 110 cm −1 , which correspond to the in-plane (E g ) and the out-of-plane (A 1g ) phonon vibration mode, respectively, in consist with the recently reported 2D CdI 2 crystals [43,44]. The inset is the representative Raman intensity maps of E g and A 1g modes of a typical CdI 2 triangular flake, indicating highly uniform crystalline quality throughout the entire flake.…”
Section: Growth and Characterization Of Layered CDI 2 Flakessupporting
confidence: 70%
“…Thus, their structural responses and physical and chemical properties may differ while under compression at high pressure (HP). For example, at high pressure, the metallic-like graphite can be turned into insulating diamond, whereas insulating/semiconducting compounds can be turned into metallic (e.g., CrPS 4 ) and even superconducting states (e.g., FePSe 3 and CrSiTe 3 ). , At high pressure, 2D-vdW materials can also be turned into bulk (or bulk-like) vdW materials via strong coupling of the vdW layers. This would produce significant modifications of the physical chemical properties present initially in the 2D materials.…”
Section: Introductionmentioning
confidence: 99%
“…It is apparent that, by changing the chemical composition and/or external pressure, the structures and properties of vdW materials can be modified significantly. For this reason, layered 2D materials such as graphene, transition metal dichalcogenides, , metal phosphorus trichalcogenides, ,, transition metal dihalides, and bismuth oxyhalides , have been studied extensively at high pressures. It is noteworthy that the element copper was not concerned in these prior studies.…”
Section: Introductionmentioning
confidence: 99%
“…In a word, the metallization appears through engineering vdW interactions, which provides an effective route to modulate the electrical band structure, enabling the tuning of spin properties and the electronic state of VS 2 . [11,172] Until now, the state transitions from an insulator or semiconductor state to the metallic state in various materials involving CdI 2 , [174] Bi 2 X 3 , Sb 2 X 3 , and Ag 2 X (e.g., X = S, Se, and Te), MOF, [44] perovskites, [39][40][41][42][43] BP, [32] etc., [20] have been investigated. In these metallizations, the large structural reconstructions or atomic movements mostly take place to close the vdW gaps or lead to first-order structural transitions although the unique metallization of hybrid perovskites without structural transition has been found.…”
Section: Metallizationmentioning
confidence: 99%
“…It shows a slow-down drop of resistance and a tendency toward a low-temperature curve with the increase of magnetic fields, proving the emergence of the superconducting phase. [180] Chi et al also investigated the www.advancedsciencenews.com www.advancedscience.com [39] (CH 3 NH 3 )PbI 3 Above 60 (RT) [42] Cs 3 Bi 2 I 9 28 (338 K) [ 200] 2D TMDs ZrTe 2 T-ZrTe 2 ≈ 2 (H-Zr-Te 2 ≈ 6) [ 201] 1T-TiSe 2 2-4 (1.8 K) [ 191] WTe 2 10.5 (2.8 K); [ 183] 4-5 (300 K) [ 184] WS 2 22 (280 K) [17] WSe 2 51.7 (RT) [ 202] ZrS 2 5.6-25 [ 186] 5.6-25 (1.1-1.9 K) or 25-100 (0.3-0.1 K) [ 186] MoTe 2 14.9 [ 203] MoS 2 30 (270 K); [ 167] 9 (RT) [19] 90 (3 K) [ 167] Intermediate state: 10-19; semiconducting state: 0-10 [19] CdI 2 62 (240 K) [ 174] 35 (270 K) [ 174] semiconducting phase FeCL 2 47 (300 K) [ 204] NI 2 19 (310 K) [ 205] MgC 2 Ambient pressure (15 K) [ 206] BP 1.7, 10 [ 207] Above 5 (6-13 K); [ 181] above 10 (5-10 K); [ 182] 11-30 (4-10.7 K), 15 (6 K) [ 207] MoSe 2 40.7-60 [20] 0-40.7 semiconducting phase CaC 2 43 (7.9 K) and 95 (9.8 K) [ 185] CaC 6 7.5 (15.1 K) [ 208] superconductivity in pristine 2H a -MoS 2 and this is explained by the occurrence of a new flat Fermi pocket at ultrahigh pressure. [167] Using the external magnetic field, superconductivity was again verified.…”
Section: Superconductingmentioning
confidence: 99%