Publication Details
Overview
 
 
Pieter Cardinael, Pieter Cardinael, Sachin Yadav, Sachin Yadav, Herwig Hahn, Herwig Hahn, Sourish Banerjee, Sourish Banerjee, Babak Kazemi Esfeh, Babak Kazemi Esfeh, Christof Mauder, Christof Mauder, Barry O'Sullivan, Barry O'Sullivan, Uthayasankaran Peralagu, Uthayasankaran Peralagu, Anurag Vohra, Anurag Vohra, Robert Langer, Robert Langer, Nadine Collaert, Nadine Collaert, Bertrand Parvais, Bertrand Parvais, Jean-Pierre Raskin, Jean-Pierre Raskin
 

Contribution to journal

Abstract 

Fabrication of low-RF loss GaN-on-Si high electron mobility transistor stacks is critical to enable competitive front-end-modules for 5G and 6G applications. The main contribution to RF losses is the interface between the III-N layer and the HR Si wafer, more specifically the AlN/Si interface. At this interface, a parasitic surface conduction layer exists in Si, which decreases the substrate effective resistivity sensed by overlying circuitry below the nominal Si resistivity. However, a clear understanding of this interface with control of the parasitic channel is lacking. In this Letter, a detailed physical and electrical description of metalorganic chemical vapor deposition-grown AlN/Si structures is presented. The presence of a SiCxNy interfacial layer is revealed, and its importance for RF losses is shown. Through C-V and I-V characterization, an increase in the C concentration of this interfacial layer is linked to the formation of negative charge at the AlN/Si interface, which counteracts the positive charge present in the 0-predose limit. The variation of the TMAl predose is shown to allow precise tuning of the C composition and, consequently, the resulting interface charge. Notably, a linear relationship between the predose and the net interface charge is observed and confirmed by the fabrication of an AlN/Si sample with close to zero net charge. In addition, a higher Dit (∼ 2 × 10 12 c m − 2 ) for such compensated samples is observed and can contribute to low-RF loss. An exceptionally high effective resistivity of above 8 kΩ cm is achieved, corresponding to an RF loss below 0.3 dB/mm at 10 GHz.

Reference