|Jmol-3D images||Image 1|
|Molar mass||487.08 g/mol|
|Appearance||solid, dark grey|
|Melting point||716 °C (1,321 °F; 989 K)|
|Solubility in water||decomposes in water|
exposure limit (PEL)
|5 micrograms (Cd)/m3|
|Except where noted otherwise, data are given for materials in their standard state (at 25 °C (77 °F), 100 kPa)|
2(s) is proven to dissociate thermally between 220° to 280° according to the reaction
2(s) → 3Cd
(g) + 0.5 As
An energy barrier was found for the nonstoichiometric vaporization of arsenic due to the irregularity of the partial pressures with temperature. The range of the energy gap is from 0.5 to 0.6 eV. Cd
3As melts at 716 °C and changes phase at 615 °C/
Pure cadmium arsenide undergoes several phase transitions at high temperatures, making phases labeled α (stable phase), α’, α” (metastable phase), β. At 593° the polymorphic transition α → β happens.
3As <-> α’-Cd
3As happens at ~500K.
3As <-> α’’-Cd
3As happens at ~742 and is a regular first order phase transition with marked hysteresis loop.
3As <-> β-Cd
3As happens at 868 K.
Singly crystal x-ray diffraction was used to determine the lattice parameters of Cd
3As between 23 and 700 °C. Transition α → α′ happens slowly and there is most likely an intermediate phase. The transition α′ → α″ occurs much faster than α → α′ and has very small thermal hysteresis. This transition results in a change in the fourfould axis of the tetragonal cell, causing Crystal twinning. The width of the loop is independent of the rate of heating although it becomes narrower after several temperature cycles.
The compound cadmium arsenide has a lower vapor pressure (0.8 atm) than both cadmium and arsenic separately. Cadmium arsenide does not decompose when it is vaporized and re-condensed. Carrier Concentration in Cd
3As are usually between 1 and 4 x 1018 electrons/cm3. Despite having high carrier concentrations, the electron mobilities are also very high (up to 10,000 cm2/Vs at room temperature).
In 2014 Cd
2 was shown to be a “semi-metal” material analogous to graphene that exists in a 3D form that should be much easier to shape into electronic devices. Three-dimensional (3D) topological Dirac semimetals (TDSs) are bulk analogues of graphene that also exhibit non-trivial topology in its electronic structure that shares similarities with topological insulators. Moreover, a TDS can potentially be driven into other exotic phases (such as Weyl semimetals, axion insulators and topological superconductors), Angle-resolved photoemission spectroscopy revealed a pair of 3D Dirac fermions in Cd
2. Compared with other 3D TDSs, for example, β-cristobalite BiO
2 and Na3Bi, Cd
2 is stable and has much higher Fermi velocities. In situ doping was used to tune its Fermi energy.
Cadmium Arsenide is a II-V semiconductor showing degenerate N-type semiconductor intrinsic conductivity with a large mobility, low effective mass and highly non parabolic conduction band, or a Narrow-gap semiconductor. It displays an inverted band structure, and the optical energy gap, eg, is less than 0. When deposited by thermal evaporation (deposition), cadmium arsenide displayed the Schottky (Thermionic emission) and Poole–Frenkel effect at high electric fields.
Cadmium arsenide can be prepared as amorphous semiconductive glass. According to Hiscocks and Elliot, the preparation of cadmium arsenide was made from cadmium metal, which had a purity of 6 N from Kock-Light Laboratories Limited. Hoboken supplied β-arsenic with a purity of 99.999%. Stoichiometric proportions of the elements cadmium and arsenic were heated together. Separation was difficult and lengthy due to the ingots sticking to the silica and breaking. Liquid encapsulated Stockbarger growth was created. Crystals are pulled from volatile melts in liquid encapsulation. The melt is covered by a layer of inert liquid, usually B2O3, and an inert gas pressure greater than the equilibrium vapor pressure is applied. This eliminates the evaporation from the melt which allows seeding and pulling to occur through the B2O3 layer.
The unit cell of Cd
3As is tetragonal. The arsenic ions are cubic close packed and the cadmium ions are tetrahedrally coordinated. The vacant tetrahedral sites provoked research by von Stackelberg and Paulus (1935), who determined the primary structure. Each arsenic ion was surrounded by cadmium ions at six of the eight corners of a distorted cube and the two vacant sites were at the diagonals.
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