Electrical Transport — Construction of 1D Molecular Conductive Wires Through a Polarized Gene Weaving Strategy for Efficient Electromagnetic Wave Absorption

5 measurement groups · 11 results

Reported values remain attached to the sample, method, conditions, extraction quality and source location that produced them.

CuTBTT-1D-15% paraffin ring · Pellet

Cole-Cole curves for CuTBTT-1D at 5%, 10% and 15% filler densities; epsilon_p'' and epsilon_c'' contributions calculated.

Temperature: room temperature
Geometry: Paraffin composite toroidal rings
Context: composite sample with pristine CuTBTT-1D active component
Measurement source: main p.7 · Analysis of Polarization Loss Mechanism · Figure 5a-e

Property	Reported value	Normalised value	Uncertainty	Origin and quality	Source
Cole-Cole semicircles for CuTBTT-1D-10%	10 semicircles	—	—	Figure Axis Rounded Reported	main p.7 · Analysis of Polarization Loss Mechanism · Figure 5d
Cole-Cole semicircles for CuTBTT-1D-15%Marked as a best value within this paper	15 semicircles	—	—	Figure Axis Rounded Reported	main p.7 · Analysis of Polarization Loss Mechanism · Figure 5d
Cole-Cole semicircles for CuTBTT-1D-5%	7 semicircles	—	—	Figure Axis Rounded Reported	main p.7 · Analysis of Polarization Loss Mechanism · Figure 5d
Polarisation relaxation dominates dielectric absorption	epsilon_p'' is obviously greater than epsilon_c'' after 4 GHz	—	—	Text Qualitative	main p.7 · Contribution of Conduction and Polarization Loss · Figures 5e and S25

CuTBTT-2D-25% paraffin ring · Pellet

Cole-Cole curves for CuTBTT-2D at 15% and 25% filler densities; epsilon_p'' and epsilon_c'' contributions calculated.

Property	Reported value	Normalised value	Uncertainty	Origin and quality	Source

Pristine CuTBTT-1D powder/ribbon network · Powder

Room-temperature conductivity tested for CuTBTT-1D at different filling densities.

Temperature: room temperature
Geometry: Two-probe method; sample geometry not otherwise specified
Context: pristine framework and filling-density series
Measurement source: main p.6 · Analysis of Conduction Loss Mechanism · Figure 4f

Property	Reported value	Normalised value	Uncertainty	Origin and quality	Source
Electrical conductivity of CuTBTT-1D at 5% filling	0.05 S m-1	—	—	Figure Axis Rounded Reported	main p.6 · Analysis of Conduction Loss Mechanism · Figure 4f
Maximum electrical conductivity of CuTBTT-1DMarked as a best value within this paper	11.14 S m-1	—	—	Text Exact Reported	main p.6 · Analysis of Conduction Loss Mechanism · Figure 4f

Pristine CuTBTT-2D nanosheets · Powder

Room-temperature conductivity tested for CuTBTT-2D at different filling densities.

Property	Reported value	Normalised value	Uncertainty	Origin and quality	Source
Electrical conductivity of CuTBTT-2D at 15% filling	approximately 0.025 S m-1	—	approximately from plotted bar	Visual Estimate Approximate	SI p.17 · 4. Performance analysis · Figure S18
Electrical conductivity of CuTBTT-2D at 25% fillingMarked as a best value within this paper	approximately 0.044 S m-1	—	approximately from plotted bar	Visual Estimate Approximate	SI p.17 · 4. Performance analysis · Figure S18

CuTBTT-1D-15% paraffin ring · Pellet

2-18 GHz electromagnetic parameters derived from VNA data at room temperature for CuTBTT-1D filler series, with emphasis on 15% loading.

Property	Reported value	Normalised value	Uncertainty	Origin and quality	Source
Eddy current loss coefficient trend	C0 values across all filling levels fluctuate between 2 and 18 GHz	—	—	Text Qualitative	main p.6 · Electromagnetic Parameters Analysis · Figure 4e
Imaginary permeability magnitude	mu'' remains approximately 0.2 across all frequency ranges	—	approximately	Text Approximate	main p.5 · Electromagnetic Parameters Analysis · Figure 4b
Dielectric loss dominates over magnetic loss	For CuTBTT-1D-15%, tan(delta_epsilon) consistently exceeds tan(delta_mu)	—	—	Text Qualitative	main p.5 · Electromagnetic Parameters Analysis · Figure 4d