参数详细信息:
透射波段范围 : | 0.6 to 21.0 um |
折射率: | 2.4028 at 10.6 um |
反射损耗: | 29.1% at 10.6 um (2 surfaces) |
吸收系数: | 0.0005 cm-1at 10.6 um |
吸收峰: | 45.7 um |
dn/dT : | +61 x 10-6/℃ at 10.6 um at 298K |
dn/du = 0 : | 5.5 um |
密度: | 5.27 g/cc |
熔点: | 1525℃ (see notes below) |
导热系数: | 18 W m-1 K-1at 298K |
热膨胀: | 7.1 x 10-6/℃at 273K |
硬度 : | Knoop 120 with 50g indenter |
比热容量 : | 339 J Kg-1聽K-1 |
Dielectric Constant : | n/a |
Youngs Modulus (E) : | 67.2 GPa |
Shear Modulus (G) : | n/a |
Bulk Modulus (K) : | 40 GPa |
弹性系数 : | Not Available |
Apparent Elastic Limit : | 55.1 MPa (8000 psi) |
泊松比 : | 0.28 |
Solubility : | 0.001g/100g water |
Molecular Weight : | 144.33 |
Class/Structure : | HIP polycrystalline cubic, ZnS, F43m |
No = Ordinary Ray
μm | No | μm | No | μm | No |
0.54 | 2.6754 | 0.58 | 2.6312 | 0.62 | 2.5994 |
0.66 | 2.5755 | 0.7 | 2.5568 | 0.74 | 2.5418 |
0.78 | 2.5295 | 0.82 | 2.5193 | 0.86 | 2.5107 |
0.90 | 2.5034 | 0.94 | 2.4971 | 0.98 | 2.4916 |
1.0 | 2.4892 | 1.4 | 2.4609 | 1.8 | 2.4496 |
2.2 | 2.4437 | 2.6 | 2.4401 | 3.0 | 2.4376 |
3.4 | 2.4356 | 3.8 | 2.4339 | 4.2 | 2.4324 |
4.6 | 2.4309 | 5.0 | 2.4295 | 5.4 | 2.4281 |
5.8 | 2.4266 | 6.2 | 2.4251 | 6.6 | 2.4235 |
7.0 | 2.4218 | 7.4 | 2.4201 | 7.8 | 2.4183 |
8.2 | 2.4163 | 8.6 | 2.4143 | 9.0 | 2.4122 |
9.4 | 2.4100 | 9.8 | 2.4077 | 10.2 | 2.4053 |
10.6 | 2.4028 | 11.0 | 2.4001 | 11.4 | 2.3974 |
11.8 | 2.3945 | 12.2 | 2.3915 | 12.6 | 2.3883 |
13.0 | 2.3850 | 13.4 | 2.3816 | 13.8 | 2.3781 |
14.2 | 2.3744 | 14.6 | 2.3705 | 15.0 | 2.3665 |
15.4 | 2.3623 | 15.8 | 2.3579 | 16.2 | 2.3534 |
16.6 | 2.3487 | 17.0 | 2.3438 | 17.4 | 2.3387 |
17.8 | 2.3333 | 18.2 | 2.3278 |
关于晶体切割:
During Chemical Vapour Deposition the small crystallite grains align with the direction of growth, and are
normal to the thickness of the sheet produced. For windows of normal thickness and aspect ratios the alignment of the grain therefore is rarely a problem as they are cut from the grown sheet such that within an optical window the grains align perpendicular to the surfaces. This is optimum orientation for lowest internal absorption and scatter.
With prisms, the cutting direction requires more consideration. It is recommended that the thickness of the strip material corresponds to the apex
height of the prism. This ensures optimum crystallite orientation for most usual
prism applications.
For typical 45° prisms the most obvious use of material is shown in (A) but it
should be noted that this is not the optimum orientation.
The best choice is (B) and it also permits a higher limit on prism size or conversely allows thinner stock to be used. There is waste at the ends of the strip but this is small and so it may not be quite as economic as (A).
Cutting in direction (C) where the entire light beam runs at 90° to the grain
structure should be avoided completely if at all possible. Note that maximum available thickness of ZnSe and ZnS (FLIR) is approximately 60mm. Maximum available thickness of ZnS Cleartran is approximately 30mm
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