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Nickel cylinders, pellets purity 99.99% - 100g
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Nickel cylinders, pellets purity 99.99% - 100g
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Acrylic Element cube - Hydrogen H2- 50mm
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Europium metal - 1.50g in Ampoule under Argon - 99.99%
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Glassy carbon - 99.99% purity - 1 grams sealed in ampoule
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10g Neodymium Metal 99.9% in Ampoule under Argon
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Fine Niobium Powder, 25 grams , purity 99.9%
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High pure silver granules in ampoule under Argon 1.5 grams
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Ruthenium 10.14g melted pellet, purity 99.96%
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High purity Xenon gas ampoule, purity 99.998%
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High purity Xenon gas ampoule, purity 99.998%
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Niobium foil - 99.9% - 200mm x 99mm x 0.025mm
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Niobium foil - 99.9% - 200mm x 99mm x 0.025mm
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High purity electrolytic Manganese chips shiny surface 5g 4N
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10g High purity Scandium Metal 99,9% purity min. - granules
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GOLD 24K precision density cube 10mm - 19.32g NEW!
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Bulk o-SiP orthorhombic Silicon phosphide single crystals

o-SiP bulk orthorhombic Silicon phosphide single crystals

Properties: Copper-shining, red translucent crystal platelets. Air stable, stable in conc. non-oxidizing acids. Melting point ~ 1110–1130 °C 

SKU: 04951-1-1 Categories: , , , ,

o-SiP bulk orthorhombic Silicon phosphide single crystals

Properties: Copper-shining, red translucent crystal platelets. Air stable, stable in conc. non-oxidizing acids. Melting point ~ 1110–1130 °C 

Orthorhombic SiP (o-SiP) is a 2D layered crystal and may have a significant impact on optoelectronic technologies.

Differentialscanning calorimetry (DSC) and thermogravimetric
analysis (TGA) curves show that o-SiP is thermally stable even
at a temperature of 1045 °C. This is very important for device
fabrication and practical applications. Unlike graphene, o-SiP
has an appropriate band gap that is determined to be 1.7 eV.
Bulk o-SiP is a p-type semiconductor with a carrier mobility
of 2.034 × 103 cm2 V−1 s−1, which is tenfold that of MoS2. The
photoresponse properties of o-SiP were investigated by excitation
using a 671 nm laser with different powers of 20, 40, 60,
80, 100 and 120 mW, respectively. Its appropriate band gap
and high enough carrier mobility, together with clear photoswitching
behavior and relatively fast response, make it possible
for o-SiP to be a 2D electronic and optoelectronic
material.

 

 

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