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Iridium metal arc melted bead, 5 grams, 99,95% purity!
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High purity Terbium Metal - 99,95% purity under Argon
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10g Cerium Metal 99.9% in Ampoule under Argon
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10g Cerium Metal 99.9% in Ampoule under Argon
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Solid Chromium Metal Sphere 30mm - 99.9% purity - ~ 100 grams
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100g Lanthanum metal pieces 99,9% under argon!
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100g Lanthanum metal pieces 99,9% under argon!
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Red Phosphorus - 7N semiconductor grade - 99.99999% 0.5g
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Acrylic Element cube - Molybdenum disc Mo - 50mm
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Sodium metal, shiny - sealed in ampoule under argon, 99,5%
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Zinc granules 3mm- 99,99% purity under Argon 10 grams
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50g high purity Cesium Metal 99,99% in ampoule - Last one
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FERROFLUID 250ml For magnetic experiments
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FERROFLUID 250ml For magnetic experiments
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Acrylic Element cube - Hydrogen H2- 50mm
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Ytterbium Oxide ~99% - Yb2O3 - 100 grams
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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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