Abstract
The temperature coefficient of Vth (=dVth/dT), which is commonly utilized for circuit design, was systematically obtained against various TiN and capping layer thicknesses in high-k/metal gate field-effect transistors (FETs). It is known that the magnitude of |dVth/dT| for such FETs is larger than that of polycrystalline silicon (poly-Si) gate FETs. The origins of the dVth/dT difference among high-k/metal gate FETs were attributed to differences in the temperature coefficient of flat band voltage (=dVFB/dT) and the equivalent gate oxide thickness (EOT). Thicker TiN layers reduced dVFB/dT, which enlarged the magnitude of |dVth/dT|. The EOT increased as the TiN metal layer or Al2O3 capping layer increased in thickness. The large EOT led to an increase in |dVth/dT|, since dVth/dT is a function of the inverse of gate capacitance. In contrast, La2O3 capping hardly affected dVth/dT. This is because La2O3 capping did not affect EOT differently from Al2O3 capping. The relationship between dVth/dT and EOT implies that EOT scaling relieves the issue of large |dVth/dT| for high-k/metal gate FETs.