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Black Phosphorus - crystal  pieces -  5.0g in ampoule
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Palladium melted pellet, purity 99,95%, 0.5g
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Erbium Metal 99,99% purity 5 grams in sealed vial under Argon
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Complete Collection of 16 highly Rare Earth Doped Glass Ingot Set - 30mm
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200 grams pure Hafnium metal melted pellets, purity 99.9%
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Acrylic Element cube - Cobalt Co - 50mm
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Aluminum precision density cube 10mm - 2.70g
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Acrylic Element cube - He Helium - 50mm
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5g Cerium Metal in sealed in ampoule under Argon
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100g Cerium metal pieces 99,9% under argon!
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50mm Terbium metal precision density cube 1kg - 99.95%
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Scandium precision density cube 10mm - 2.98g
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5 grams Yttrium Metal pieces sealed vial under Argon
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MOLYBDENUM precision density cube 10mm - 10.22g
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New! Aerogel Nanogel Granules 10ml
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Gases discharge tube set, size approximately ~75x75mm
 199,00
Big Copper polished density cube 10cm3 89.6 grams
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Europium 3+ doped fluorescent glass bead 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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