Temperature-dependent diffusive to ballistic transport transition in aligned double walled carbon nanotubes in the high frequency regime George Chimowa, E. Flahaut and Somnath Bhattacharyya Supplementary Material Preparation of CNTs device involves the processes illustrated in Fig. S1 below: Schematic diagram of the whole fabrication process of the devices and the measurement set up. It consists of CNT alignment using dielectrophoresis. (b) Nano-manipulation (a) Dielectrophoresis ~ AC 1 V p-p 10 Mhz (c) Bonding G.I.S (d) HF Measurements ebe a m G. S. G Pr o b e G. S. G Pr o b e Figure S1. (a), CNT selection using nano-manipulators (b) and CNT metal contact bonding using a combination of e-beam lithography and gas injection system (GIS) (c). The HF impedance is then measured using G-S-G probes with a 50 µm pitch size (d). Figures [S2 (a), (b), (c)] below show SEM and TEM images of nanotubes aligned across the gap of a coplanar waveguide. (c) (d) Figure S2. SEM micrograph for DW2 (a) had eleven DWNTs but because of the scale only a few can be seen, DW1 (b) had four on separate positions as shown. (c–d) TEM micrographs DWNTs networks after catalyst removal and before alignment, showing good quality CNTs either isolated or forming small-diameter bundles. The extra data given in this section shows the rigorous test done to ensure measurement (shown in Fig. S3 and S4) accuracy as outlined in the paper. Fig. S4 indicates that the solvent that was used to disperse the CNTs does not affect the measurement accuracy. The inset illustrates the reproducibility of the data and the care practiced to ensure that the probe contact force is maintained the constant. This was made easier by the probe’s graduated screw-gauges used to lower them down. Average error over the entire spectrum = 0.027 dB -20 Mag S12 (dB) -30 MW9 A MW9 B -40 Checking drift CheckingInstrumement Instrument Drift -50 -60 0 10 20 30 40 50 60 Frequency (GHz) Figure S3. S - parameter data for a MWNT sample 9 measured at different times. MW9 B was measured 30 minutes after MW 9 A. It clearly shows that there is insignificant instrument drift with time. The above given data shows that the measurement done on the samples are very much reproducible with negligible instrument drift affecting the result. It further shows the accurate precise placements of the probe tips on the sample half an hour later. Average error in the entire spectrum = 0.03 dB -22 Open Control -24 -18 Reproducibility test -20 Mag S12 (dB) Mag S12 (dB) Checking effect of solvent -26 -22 -26 20 -28 MW9 MW9B MW10 MW10B -24 30 40 50 Frequency (GHz) 20 30 40 50 Frequency (GHz) Figure S4: Shows the test done to check the effect of solvent on the S-parameter measurement. The - Open data is for an open dummy waveguide with dichlorobenzene the solvent used dispersed on the one micron gap. And the - Control is for the same dummy without the solvent. Inset: Shows the test to check measurement reproducibility MWNT samples 9 and 10 were measured repeatedly every time lifting up the probes. The graph shows very good reproducibility.