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Deuterium oxide - heavy water - sealed in ampoule 0.75 grams
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Nice Indium Metal hemisphere  99,99% min.  -  50 grams
Nice Indium Metal hemisphere 99,99% min. - 50 grams
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Iron 150 grams melted pellets, purity 99.9%
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1.50 grams single crystal silicon fractures in ampoule
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Tantal 250g melted pellets, purity 99.99%
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Fine Niobium Powder, 50 grams , purity 99.9%
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2.5g Titanium Granules  - 99,6% - in Ampoule under Argon
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100g Praseodymium metal pieces 99,9% under argon!
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5 grams zinc pellets >99.9% in ampoule under argon
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Fine Vanadium powder, 15 grams - ~200 mesh 99.9% purity
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Acrylic Element cube - Ultrapure Phosphorus red P - 50mm
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Magnesium precision density cube 10mm sealed under argon 1.74g
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Palladium melted pellet, purity 99,95%, 1.0g
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Hafnium diboride HfB2   5 grams - 99.5%
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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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