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| Lattice constant (Å) |
3.567 |
| Density (g/cm3) |
3.52 |
|
Thermal conductivity (W/cm·K) |
20 ¸ 25 |
|
Dielectric constant |
5.68 |
|
Emission wavelength, µm |
0.23 |
|
Refractive index |
2.41 |
|
Bandgap (eV) |
5.47 |
|
Mobility (cm2/V·s) |
|
|
Electrons |
2500 |
|
Holes |
2100 |
|
Saturation velocity (107 cm/s) |
2.7 |
|
Breakdown field (107 V/cm) |
2 |
|
Radiation resistance |
very stable |
|
Heat resistance (°C) |
>1000 |
|
Hardness (Knoop), (GPa) |
80 |
|
Energy to create e/h pair, (eV) |
13,6 |
Diamonds are classified depending on the amount of nitrogen contained
within material and whether it is held as an interstitial or substitutional
defect.
| type Ia |
Nitrogen present up to levels of 4000¸4500 ppm (0.3 wt %), incorporated
in interstitial sites or aggregates. |
| type Ib |
500 ppm of nitrogen (0.06 wt %). Incorporated as substitutional point
defects. Most of synthetic diamonds are of this type. |
| type IIa |
Effectively free of nitrogen impurity. Very rare in nature, these diamonds have enhanced optical and thermal properties. |
| type IIb |
Extremely rare in nature; p-type semiconductor due to boron defects. |
We offer high-technological diamond-based industrial and scietific products,
including plates and windows with wide spectrum of parameters, as well
as advanced optical and electronic diamond
devices for the following applications:
Certified diamond substrates and plates for industrial and science applications with unique thermo, mechanical, optical, electric and radiation resistance parameters;
“Solar-blind” UV-photodetectors with high spectral selectivity in the UV-range;
Advanced detectors of ionizing radiation (a,b- and γ- particles, heavy ions, X-ray) intended
for science and industrial applications, including nuclear engineering,
medicine, space applications, high energy physics, etc.;
Durable ultra-sharp diamond scalpels and diamond microinstruments for medical and industrial purposes.
