Abstract
Porous silicon (PS) is known to form during electrochemical dissolution of silicon in HF-based solutions. This dissolution is obtained by monitoring either the anodic current or potential. In general, constant current is preferable, as it allows a better control of both the porosity and thickness and a good reproducibility from run to run. The simplest cell which can be used to anodize silicon is shown in Figure 1. The silicon wafer serves as the anode. The cathode is made of platinum or any HF-resistant and conducting material. The cell body itself is in general made of highly acid-resistant polymer such as Teflon. Since the entire silicon wafer serves as the anode, PS is formed on any wafer surface in contact with the HF solution, including the cleaved edges. The advantage of such equipment is its simplicity and ability to anodize Silicon-On-Insulator structures. Its drawback is the non uniformity in both the porosity and thickness of the resulting layer. This inhomogeneity is mainly due to a lateral potential drop. In fact, since the current flows laterally along the bulk of the silicon wafer, there is a difference in potential between the top (point A in Fig. 1) and the bottom (point B in Fig. 1). The potential drop across the wafer leads to different values of the local current density which induce porosity and thickness gradients.
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Halimaoui, A. (1995). Porous silicon: material processing, properties and applications. In: Vial, JC., Derrien, J. (eds) Porous Silicon Science and Technology. Centre de Physique des Houches, vol 1. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-03120-9_3
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DOI: https://doi.org/10.1007/978-3-662-03120-9_3
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