Electronic Supplementary Material
Synthesis of ultrathin rhenium disulfide nanoribbons using nano test tubes
Luke T. Norman
1, Johannes Biskupek
2, Graham A. Rance
3, Craig T. Stoppiello
3, Ute Kaiser
2, and Andrei N. Khlobystov
1( )
1
School of Chemistry, University of Nottingham, Nottingham, NG7 2RD, UK
2
Central Facility for Electron Microscopy, Ulm University, Albert Einstein-Allee 11, Ulm 89081, Germany
3
Nanoscale and Microscale Research Centre, University of Nottingham, Nottingham, NG7 2RD, UK Supporting information to https://doi.org/10.1007/s12274-021-3650-2
Figure S1 XPS high resolution scans with regions and components for Re2(CO)10@SWNT focussed on the (a) Re 4f, (b) C 1s, and (c) O 1s regions.
Table S1 G-band positions and shifts of each material in the stepwise synthesis using a 660 nm laser excitation.
Material G-band position [cm-1] Shift w.r.t. opened SWNTs Electron transfer
Opened SWNTs 1591.5 0 –
Re2(CO)10@SWNT 1591.2 –0.3 No electron transfer
Re2(CO)10@SWNT + I2 1602.1 +10.6 SWNT → I2
[Re6I14]2−@SWNT2n+ 1596.4 +4.9 -ve charged species within SWNTs
ReS2@SWNT 1597.4 +5.9 ReS2 δ-@SWNTδ+
Figure S2 Raman spectrum of Re2(CO)10@SWNT + I2 measured using a 532 nm excitation source. The spectrum is focussed on the low-frequency region and highlights the presence of two peaks at 106 and 175 cm-1 which are attributed to I3- and I5- respectively. However, the I5- band does have strong overlap with the radial breathing mode of the SWNTs.
Address correspondence to Andrei.Khlobystov@nottingham.ac.uk
Nano Res.
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Figure S3 XPS high resolution scans with regions and components for [Re6I14]2−@SWNT2+ focused on the (a) Re 4f, and (b) I 3d regions.
Figure S4 XPS high resolution scans with regions and components for ReS2@SWNTfocused on the (a) Re 4f, and (b) S 2p regions.