Bismuth Sputtering Target - 6mm Thickness, 50-75mm Diameter
Bismuth Sputtering Target - 6mm Thickness, 50-75mm Diameter
SKU:BIS-b1e9f7
High-purity Bismuth Sputtering Target for precise sputtering processes. 99.97% purity, 6mm thickness, 50-75mm diameter.
Regular price
$399.99
Regular price
Sale price
$399.99
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Bismuth Sputtering Target - 6mm Thickness, 50-75mm Diameter
$399.99
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Bismuth Sputtering Target - 6mm Thickness, 50-75mm Diameter
$399.99
Quantity: 1
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The Bismuth Sputtering Target with a thickness of 6mm and a diameter range of 50-75mm is a high-purity material essential for sputtering processes in various applications. With a purity level of 99.97%, this target exhibits excellent quality and performance. Its atomic properties, electrical and thermal conductivity, mechanical strength, and physical properties make it a reliable choice for scientific and industrial uses. Suitable for both consumer and institutional buyers, this target meets stringent procurement standards ensuring precision and effectiveness in sputtering applications.
Product Specifications
Atomic Properties Atomic Number
83
Atomic Properties Atomic Radius Goldschmidt
0 nm
Atomic Properties Atomic Weight
208.98040 amu
Atomic Properties Crystal Structure
Rhombohedral
Atomic Properties Electronic Structure
Xe4f145d106s26p3
Atomic Properties Ionization Potential Number
1 | 2 | 3 | 4 | 5 | 6
Atomic Properties Ionization Potential Number 1
7.29 eV
Atomic Properties Ionization Potential Number 2
16.7 eV
Atomic Properties Ionization Potential Number 3
25.6 eV
Atomic Properties Ionization Potential Number 4
45.3 eV
Atomic Properties Ionization Potential Number 5
56.0 eV
Atomic Properties Ionization Potential Number 6
88.3 eV
Atomic Properties Photo Electric Work Function
4.40 eV
Atomic Properties Thermal Neutron Absorption Cross Section
0.0340 Barns
Atomic Properties Valences Shown
3 | 5
Electrical Properties Electrical Resistivity At 20 Degree Celsiu
117 µΩ·cm
Electrical Properties Temperature Coefficient At 0 To 100 Degree
0.00460 k-1
Electrical Properties Thermal Emf Against Pt Cold 0 Degree Celsi
-7.34 mV
Material Material
BismuthDiscovered in the fifteenth century, although its discoverer is not known. Bismuth is a brittle metal which is silvery in color with a pink tinge. It is stable in air and water. It has poor thermal and electrical properties and finds applications in the manufacture of fusible alloys, a range of materials with low melting points which are suitable for various applications including solders and thermal fuses. Pure bismuth shows a high absorbtion of gamma rays which makes it useful as a filter or window for these particles, whilst at the same time permitting the passage of neutrons.
Mechanical Properties Bulk Modulus Polycrystalline
31.3 GPa
Mechanical Properties Hardness Vickers Polycrystalline
16 to 19 Kgf mm-2
Mechanical Properties Material Condition
Polycrystalline
Mechanical Properties Poissons Ratio Polycrystalline
0.330
Mechanical Properties Tensile Modulus Polycrystalline
34.00 GPa
Note Note
These targets are normally available for immediate shipment from stock. Other sizes are available to special order.
Physical Properties Boiling Point
1560 ºC
Physical Properties Density At 20 Degree Celsius C Temperature
9.800 g·cm-3
Specifications Diameter
50 to 75 mm
Specifications Purity
99.97 %
Specifications Thickness
6 mm
Thermal Properties Coefficient Of Thermal Expansion At 0 To 100
13.400 x10-6 K-1
Thermal Properties Latent Heat Of Evaporation
857 Jg-1
Thermal Properties Latent Heat Of Fusion
52.00 Jg-1
Thermal Properties Melting Point
271.30 ºC
Thermal Properties Specific Heat At 25 Degree Celsius C Temperat
124.0 J K-1 kg-1
Thermal Properties Thermal Conductivity At 0 To 100 Degree Celsi
7.90 W m-1K-1
Tolerances Disc Diameter Tolerance
0.5 mm
Tolerances Thickness Tolerance
0.5 mm
Type Type
MetalA metal is generally considered to be a pure element which readily forms cations. Metals are characterized by their opacity and high thermal and electrical conductivities, the latter properties resulting from the delocalized and mobile nature of the electrons over the crystal structure.