Factory best selling Ceramic Sputtering Targets - Tin – Rich
Factory best selling Ceramic Sputtering Targets - Tin – Rich Detail:
Tin is a silvery-white lustrous metal, with a bluish tinge. It has the density of 7.3g/cm3, melting point of 231.89℃ and boiling point of 2260℃. It is ductile and malleable to some extent and has a highly crystalline structure. Its electrical conductivity is about one-seventh that of silver and its hardness is slightly higher than lead.
Tin sputtering target could be made available for a variety of applications, including food container, mechanics, metallurgy, electronics, nuclear power and aerospace.
Impurity Analysis:
Purity
≥ |
Composition(wt%)≤ | |||||||
Fe | Cu | Pb | As | Zn | Al | Cd | Total | |
99.99 | 0.002 | 0.001 | 0.005 | 0.0002 | 0.0001 | 0.0001 | 0.0001 | 0.01 |
99.95 | 0.004 | 0.004 | 0.01 | 0.003 | 0.0008 | 0.008 | 0.0005 | 0.05 |
99.9 | 0.007 | 0.008 | 0.04 | 0.008 | 0.001 | 0.001 | 0.0008 | 0.1 |
Rich Special Materials is a Manufacturer of Sputtering Target and could produce high purity Tin Sputtering Materials according to Customers’ specifications. For more information, please contact us.
Product detail pictures:
Related Product Guide:
We are also focusing on improving the stuff management and QC system so that we could keep great advantage in the fiercely-competitive business for Factory best selling Ceramic Sputtering Targets - Tin – Rich , The product will supply to all over the world, such as: Lyon, Houston, Ecuador, To win customers' confidence, Best Source has set up a strong sales and after-sales team to provide the best product and service. Best Source abides by the idea of "Grow with customer" and philosophy of "Customer-oriented" to achieve cooperation of mutual trust and benefit. Best Source will always stand ready to cooperate with you. Let's grow together!
By Nina from Portland - 2018.12.22 12:52
We are really happy to find such a manufacturer that ensuring product quality at the same time the price is very cheap.
By Jacqueline from Washington - 2017.05.02 11:33