483591
Diamond
synthetic monocrystalline powder, ≤1 μm
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About This Item
Fórmula empírica (Notação de Hill):
C
Número CAS:
Peso molecular:
12.01
Número CE:
Número MDL:
Código UNSPSC:
12352103
NACRES:
NA.23
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forma
synthetic monocrystalline powder
Nível de qualidade
tamanho de partícula
≤1 μm
densidade
3.5 g/mL at 25 °C (lit.)
aplicação(ões)
battery manufacturing
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Categorias relacionadas
Aplicação
Monocrystalline diamond particles internalized in human endothelial cells have potential applications in drug delivery.
Código de classe de armazenamento
11 - Combustible Solids
Classe de risco de água (WGK)
nwg
Ponto de fulgor (°F)
Not applicable
Ponto de fulgor (°C)
Not applicable
Equipamento de proteção individual
Eyeshields, Gloves, type N95 (US)
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Micron-sized diamond particles are internalized by endothelial cells.
Walkowiak B, et al.
Diamond and Related Materials, 18, 651-656 (2009)
Pontus Forsberg et al.
Optics express, 21(3), 2693-2700 (2013-03-14)
Control of the sidewall angle of diamond microstructures was achieved by varying the gas mixture, bias power and mask shape during inductively coupled plasma etching. Different etch mechanisms were responsible for the angle of the lower and upper part of
P Pereira Nogueira et al.
The Journal of clinical pediatric dentistry, 37(1), 53-57 (2013-01-25)
The aim of the present study was to evaluate hybrid layer thickness of primary molars sectioned with diamond, carbide and ultrasonic CVD burs. The occlusal enamel surfaces often molars were removed and superficial dentin was exposed. Three standardized cavities were
H Pinto et al.
Journal of nanoscience and nanotechnology, 12(11), 8589-8593 (2013-02-21)
We have investigated using density functional theory the effect of fluorine termination of a (001) diamond surface on the electronic energy levels of an NV- centre buried beneath the surface. We find that, like OH termination, fluorine passivates the surface
Richard W Bowman et al.
Physical review letters, 110(9), 095902-095902 (2013-03-19)
Diamond anvil cells allow the behavior of materials to be studied at pressures up to hundreds of gigapascals in a small and convenient instrument. However, physical access to the sample is impossible once it is pressurized. We show that optical
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