Measurement evidence
Toward Enhancing Performance of Electromagnetic Wave Absorption for Conductive Metal-Organic Frameworks: Nanostructure Engineering or Crystal Morphology Controlling · Wang X., Zhang X., He A. et al. · Inorganic Chemistry · 2024 · 6948-6956
Reported values remain attached to the sample, method, conditions, extraction quality and source location that produced them.
A-Cu-HHTP/paraffin coaxial ring · Pellet
Cole-Cole curves used to infer Debye polarization relaxation and conduction-loss slopes.
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| A-Cu-HHTP Cole-Cole high-frequency slope KMarked as a best value within this paper | K = 0.613 | — | — | Text Exact Reported | 6 · 3.2 · Figure 6d |
B-Cu-HHTP/paraffin coaxial ring · Pellet
Cole-Cole curves used to infer Debye polarization relaxation and conduction-loss slopes.
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| B-Cu-HHTP Cole-Cole high-frequency slope K | K = 0.472 from Figure 6e label | — | read from rendered figure label | Figure Axis Rounded Reported | 5 · 3.2 · Figure 6e |
C-Cu-HHTP/paraffin coaxial ring · Pellet
Cole-Cole curves used to infer Debye polarization relaxation and conduction-loss slopes.
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| C-Cu-HHTP Cole-Cole high-frequency slope K | K = 0.513 from Figure 6f label | — | read from rendered figure label | Figure Axis Rounded Reported | 5 · 3.2 · Figure 6f |
A-Cu-HHTP/paraffin coaxial ring · Pellet
2-18 GHz electromagnetic parameters and reflection loss calculated by transmission-line theory; sample/paraffin mass ratio 1:1.
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| A-Cu-HHTP maximum effective absorption bandwidthMarked as a best value within this paper | maximum EAB = 5.73 GHz with thickness 2.5 mm | — | — | Text Exact Reported | 4-5 · 3.2 · Figure 5d,g; Table S1 |
| A- and B-Cu-HHTP band coverage with thickness tuning | EAB of nanosheet A-Cu-HHTP and nanorod B-Cu-HHTP can cover C-band (4-8 GHz), X-band (8-12 GHz), and Ku-band (12-18 GHz) by adjusting thickness from 2 to 5 mm. | — | — | Text Qualitative | 5 · 3.2 · Figure 5; Figure S4 |
| A-Cu-HHTP epsilon double-prime at high-frequency end | epsilon double-prime decreases from 3.46 to 1.58 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5b |
| A-Cu-HHTP epsilon double-prime at low-frequency end | epsilon double-prime decreases from 3.46 to 1.58 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5b |
| A-Cu-HHTP epsilon prime at high-frequency end | epsilon prime decreases from 7.95 to 5.12 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5a |
| A-Cu-HHTP epsilon prime at low-frequency end | epsilon prime decreases from 7.95 to 5.12 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5a |
| A-Cu-HHTP minimum reflection lossMarked as a best value within this paper | RLmin = -51.08 dB at 7.25 GHz with thickness 4.4 mm | — | — | Text Exact Reported | 4-5 · 3.2 · Figure 5d,g; Table S1 |
B-Cu-HHTP/paraffin coaxial ring · Pellet
2-18 GHz electromagnetic parameters and reflection loss calculated by transmission-line theory; sample/paraffin mass ratio 1:1.
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| B-Cu-HHTP maximum effective absorption bandwidth | maximum EAB = 5.20 GHz with thickness 2.0 mm | — | — | Text Exact Reported | 4 · 3.2 · Figure 5e,h; Table S1 |
| B-Cu-HHTP epsilon double-prime at high-frequency endMarked as a best value within this paper | epsilon double-prime decreases from 5.32 to 2.65 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5b |
| B-Cu-HHTP epsilon double-prime at low-frequency endMarked as a best value within this paper | epsilon double-prime decreases from 5.32 to 2.65 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5b |
| B-Cu-HHTP epsilon prime at high-frequency endMarked as a best value within this paper | epsilon prime decreases from 11.47 to 6.60 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5a |
| B-Cu-HHTP epsilon prime at low-frequency endMarked as a best value within this paper | epsilon prime decreases from 11.47 to 6.60 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5a |
| B-Cu-HHTP minimum reflection loss | RLmin = -40.33 dB at 7.76 GHz with thickness 3.5 mm | — | — | Text Exact Reported | 4 · 3.2 · Figure 5e,h; Table S1 |
C-Cu-HHTP/paraffin coaxial ring · Pellet
2-18 GHz electromagnetic parameters and reflection loss calculated by transmission-line theory; sample/paraffin mass ratio 1:1.
| Property | Reported value | Normalised value | Uncertainty | Origin and quality | Source |
|---|---|---|---|---|---|
| C-Cu-HHTP epsilon double-prime at high-frequency end | epsilon double-prime decreases from 1.94 to 0.96 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5b |
| C-Cu-HHTP epsilon double-prime at low-frequency end | epsilon double-prime decreases from 1.94 to 0.96 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5b |
| C-Cu-HHTP epsilon prime at high-frequency end | epsilon prime decreases from 6.02 to 4.57 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5a |
| C-Cu-HHTP epsilon prime at low-frequency end | epsilon prime decreases from 6.02 to 4.57 over 2-18 GHz | — | — | Text Exact Reported | 4 · 3.2 · Figure 5a |
| C-Cu-HHTP approximate minimum reflection loss | approximately -14 dB from Figure 5f 2D RL curves | — | visual estimate from rendered figure | Figure Axis Approximate | 5 · 3.2 · Figure 5f |