Abstract

Carbon seems to be an ubiquitous impurity in high-melting oxides and silicates which have been exposed to CO/CO 2 during crystal growth. The study of synthetic MgO crystals has provided insight into the dissolution mechanism of CO/CO 2 and the diffusion mechanism of solute carbon through a dense oxide matrix. Treating the dissolution of CO 2 in MgO as a solid solution between the majority divalent oxide and a minority tetravalent oxide, two Mg 2+ vacancies are introduced for each CO 2 molecule dissolved. Carbon, sitting off-center in one cation vacancy, forms an anion complex, CO 2- 2. This complex corresponds formally to a dissolved CO molecule: CO+ O 2= CO 2- 2. The second cation vacancy is chargewise compensated by two O - undergoing spin pairing to give a peroxy anion, O 2- 2, which formally corresponds to a dissolved oxygen atom: O+ O 2-= O 2- 2. Chemically the dissolution of CO 2 can be described as redox process producing reduced and oxidized solute species, e.g. CO 2- 2 and O 2- 2. When the solute carbon passes from the cation vacancy site to interstitial sites, the CO 2- 2 anion complex dissociates into CO - and O -. While one O - remains with the cation vacancy forming a V - center, the C atom diffuses with the other O - state, e.g. a positive hole or defect electron on the O 2- sublattice. Because an O - is much smaller than an O 2- the local lattice contraction associated with the CO - lowers the activation energy barrier for the C diffusion through the dense MgO matrix. This makes C a very mobile solute species, capable of diffusing already at low temperatures when cation vacancy diffusion is not yet activated. At the same time the C diffusion is coupled to the diffusion of an electric charge. Therefore, when the MgO-CO 2 solid solution turns supersaturated during cooling, C segregation builds up a space charge layer near the surface. Its bias counteracts further segregation. This leads to the prediction that the exsolution of the MgO-CO 2 solid solution (e.g. degassing) may be controlled by space charges rather than by the carbon mobility. Experimental support is derived from SIMS measurements. However, if C-C bonds can form at the surface, CO -+ CO -= C 2 O -+ O -, the positive holes, e.g. O - states, may retrodiffuse to the bulk. This reduces the space charge at the surface, while reconverting V - centers in the bulk into peroxy anions which compensate the extrinsic cation vacancies introduced initially. If the C-C polymerization goes on, C n O -=C n+1O -+O -, with n å 1, the exsolution can procede and the solu te CO 2 component eventually splits into graphitic carbon which precipitates at the surface and solute oxygen which remains in the bulk in the form of peroxy defects.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call