2021
DOI: 10.1103/physrevb.104.l100418
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Possible electron doping of geometrically perfect spin-1/2 kagome-lattice barlowite by reduced graphene oxide

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Cited by 4 publications
(6 citation statements)
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“…In the Cu-HHTP-rGO sample, the chemical interaction would result in the doping of electrons from rGO sheets to Cu 3 (HHTP) 2 crystallites, similar to our recent report on a Cu-based coordination complex anchored onto rGO. 38 Further, as rGO sheets are more conducting than Cu 3 (HHTP) 2 crystallites, the charge-transfer pathway should majorly pass through rGO sheets, which, due to the deficit of electrons, exhibits a p-type semiconducting behavior. Such doping phenomenon must not be occurring in the Cu-HHTP/rGO or Cu-HHTP+rGO sample, as rGO is simply acting as an additive; hence, they remain n-type material, similar to pristine Cu-HHTP.…”
Section: ■ Results and Discussionsupporting
confidence: 84%
See 1 more Smart Citation
“…In the Cu-HHTP-rGO sample, the chemical interaction would result in the doping of electrons from rGO sheets to Cu 3 (HHTP) 2 crystallites, similar to our recent report on a Cu-based coordination complex anchored onto rGO. 38 Further, as rGO sheets are more conducting than Cu 3 (HHTP) 2 crystallites, the charge-transfer pathway should majorly pass through rGO sheets, which, due to the deficit of electrons, exhibits a p-type semiconducting behavior. Such doping phenomenon must not be occurring in the Cu-HHTP/rGO or Cu-HHTP+rGO sample, as rGO is simply acting as an additive; hence, they remain n-type material, similar to pristine Cu-HHTP.…”
Section: ■ Results and Discussionsupporting
confidence: 84%
“…Remarkably, the Cu-HHTP-rGO sample was realized to be a p-type semiconductor with a positive Seebeck coefficient (Figure a), and such opposite semiconducting property in the Cu-HHTP-rGO sample suggested that, indeed, Cu-HHTP and rGO must be chemically interacting. In the Cu-HHTP-rGO sample, the chemical interaction would result in the doping of electrons from rGO sheets to Cu 3 (HHTP) 2 crystallites, similar to our recent report on a Cu-based coordination complex anchored onto rGO . Further, as rGO sheets are more conducting than Cu 3 (HHTP) 2 crystallites, the charge-transfer pathway should majorly pass through rGO sheets, which, due to the deficit of electrons, exhibits a p-type semiconducting behavior.…”
Section: Resultsmentioning
confidence: 68%
“…Out-of-plane XRD data were recorded at room temperature using a Bruker D8 Advance diffractometer using Cu Kα radiation (λ = 1.5406 Å). Rietveld refinement of the PXRD patterns were carried out by a standardized procedure using the FullProf program 53 , 54 . Raman spectra (λ exc = 632.8 nm) were recorded at Raman microscope (LabRAM HR, HoribaJobinYvon) with a 50× objective lens (spectral resolution of the system is ~1 cm −1 ).…”
Section: Methodsmentioning
confidence: 99%
“…Such a site doping approach could lead to the loss of spin frustration with the dopant occupying the Kagome plane instead of the interlayer sites in the Herbertsmithite‐like systems [14] . To overcome this problem, in our previous reports, we have adopted an unconventional approach of anchoring various atacamite family‐based minerals with S= 1/2 ${{ 1/2 }}$ Kagome lattices onto reduced graphene oxide (rGO), [6d,7c,15] which resulted in the enhanced electrical transport properties with the retention of characteristic magnetic signatures of the pristine material [6d,7c] . Especially, in the Barlowite system, we demonstrated the elusive electron doping phenomenon which resulted in the insulator‐to‐semiconductor transition [7c] .…”
Section: Introductionmentioning
confidence: 93%
“…To overcome this problem, in our previous reports, we have adopted an unconventional approach of anchoring various atacamite family‐based minerals with S= 1/2 ${{ 1/2 }}$ Kagome lattices onto reduced graphene oxide (rGO), [6d,7c,15] which resulted in the enhanced electrical transport properties with the retention of characteristic magnetic signatures of the pristine material [6d,7c] . Especially, in the Barlowite system, we demonstrated the elusive electron doping phenomenon which resulted in the insulator‐to‐semiconductor transition [7c] . However, Barlowite is a non‐QSL material, while 2D‐MOFs are promising QSL materials, which are even realized to be stable with the presence of site‐dopants [9a] .…”
Section: Introductionmentioning
confidence: 93%