Oxide fluxes are often combined to reduce volatility, viscosity, and reactivity towards the crucibles. Metallic fluxes aren't typically combined,3 as they do not suffer from the same volatility, viscosity, and reactivity issues. An ideal flux should have the following properties:4
The growth (starting materials, flux, and crucible) are heated to form a complete liquid solution. The growth is cooled to a temperature where the solution is fully saturated. Further cooling causes crystals to precipitate from the solution, lowering the concentration of starting materials in solution, and lowering the temperature where the solution is fully saturated. The process is repeated, decreasing temperature and precipitating more crystals. The process is then stopped at a desired temperature, and the growth is removed from the furnace. Practically, the flux method is done by placing the growth into a programmable furnace:
Additional steps may be added to this basic temperature profile, such as additional dwells or different cooling rates over different points of the cool. Crystallization can occur through spontaneous nucleation, encouragement with a seed, or through mechanical stress.
After crystallization, often some solidified flux remains on the surface or inside the desired crystal. This flux may cause defects in the crystal due to the different thermal expansivities of the flux and crystal.5 A solvent (typically an acid or a base) can dissolve the flux, but it's difficult to find a solvent that doesn't also dissolve the crystal. The flux can be removed mechanically using a blade or drill. If the crystal and flux have significantly different boiling points, the flux may be removed with evaporation. Flux can also be removed through recrystallization through use of a seed in the liquid phase, leaving the flux behind as the crystals accumulate.
The removal of excess flux is important to assess a crystals properties, as the flux can affect measurements. For example, tin and lead super conduct at low temperatures,6 if a sample has tin or lead flux superconductivity can be observed even if the desired crystal is not a superconductor.
Byrappa, K.; Ohachi, Tadashi (Eds.) (2003). "17.2.4 Flux method". Crystal Growth Technology. Norwich, N.Y.: William Andrew Pub. p. 567. ISBN 3-540-00367-3. Components of the gem materials desired in a single crystal form are dissolved in a flux (solvent). 3-540-00367-3 ↩
Tachibana, Makoto (2017). Beginner's Guide to Flux Crystal Growth. Tsukuba, Ibaraki Japan: Springer. pp. 61–87. ISBN 978-4-431-56586-4. 978-4-431-56586-4 ↩
Kanatzidis, Mercouri G.; Pöttgen, Rainer; Jeitschko, Wolfgang (2005-11-04). "The Metal Flux: A Preparative Tool for the Exploration of Intermetallic Compounds". Angewandte Chemie International Edition. 44 (43): 6996–7023. doi:10.1002/anie.200462170. ISSN 1433-7851. PMID 16259022. https://onlinelibrary.wiley.com/doi/10.1002/anie.200462170 ↩
Wolf, Thomas (July 2012). "Flux separation methods for flux-grown single crystals". Philosophical Magazine. 92 (19–21): 2458–2465. Bibcode:2012PMag...92.2458W. doi:10.1080/14786435.2012.685193. ISSN 1478-6435. S2CID 137541564. http://www.tandfonline.com/doi/abs/10.1080/14786435.2012.685193 ↩
Buzea, Cristina; Robbie, Kevin (2005-01-01). "Assembling the puzzle of superconducting elements: a review". Superconductor Science and Technology. 18 (1): R1 – R8. arXiv:cond-mat/0410302. doi:10.1088/0953-2048/18/1/R01. ISSN 0953-2048. https://iopscience.iop.org/article/10.1088/0953-2048/18/1/R01 ↩