Invited: Direct Bonding: A Key Enabler for 3D Monolithic Integration

Monolithic 3D Integration (3DMI) consists in processing transistors on top of each other sequentially. This technology appears to be an alternative solution to scaling, from the 7nm node integration and below, as substantial gain in area and performance as compared to planar technology is expected without scaling the transistor technology node. 3DMI appears to be the most optimized way to take advantage of the vertical dimension as almost no alignment constraints remains. By using a standard lithography, the top transistors can be aligned directly onto their bottom counterparts with a high accuracy (see Fig. 1), contrary to TSV-based 3D technologies [2]. Furthermore, 3DMI is a highly versatile technology as the different transistor levels can be optimized independently, from the choice of the channel characteristics (e.g. material, orientation, strain) to the architecture itself (e.g. CMOS on CMOS, PMOS on NMOS, FinFET on BULK, LVT on RVT) [3]. Such sequential integration raises two main technological challenges: Creating an active layer above a bottom transistor which will become the channel of the top transistor. In order to achieve similar performance for top FET than bottom FET, the substrate quality must be equivalent than commercial substrates. Thus, this layer must be monocristalline and defect free in order to optimize the mobility and to be consistent with high performance criteria. A precise thickness control is also necessary in order to avoid device performance dispersion . Realizing a high performance top transistor level without degrading the bottom level as the stacked transistor levels are processed sequentially, i.e. at low temperature process –typically below 600°C . Recent results demonstrate some integration solutions, such as junction activation by Solid Phase Epitaxy Regrowth below 600°C [4]. To tackle the first challenge, we transfer a thin silicon layer from a high quality Silicon On Insulator (SOI) wafer by direct bonding. It appears to be the most effective solution to obtain a defect free monocristalline active layer with a well-controlled thickness. This method is preferred to different techniques which have been developed to create large monocristal grains of silicon either by laser anneal of amorphous Poly-Silicon [5] or by µ-Czochralsky process [6]. However, in both cases, large “seed layers” are necessary to control the orientation and the size of these grains, which is not consistent with for high density circuits. For this