Highly scaled nanoelectronics requires effective channel doping above 5 x 10(19) cm(-3) together with ohmic contacts with extremely low specific contact resistivity. Nowadays, Ge becomes very attractive for modern optoelectronics due to the high carrier mobility and the quasi-direct bandgap, but n-type Ge doped above 5 x 10(19) cm(-3) is metastable and thus difficult to be achieved. In this letter, we report on the formation of low-resistivity ohmic contacts in highly n-type doped Ge via non-equilibrium thermal processing consisting of millisecond-range flash lamp annealing. This is a single-step process that allows for the formation of a 90 nm thick NiGe layer with a very sharp interface between NiGe and Ge. The measured carrier concentration in Ge is above 9 x 10(19) cm(-3) with a specific contact resistivity of 1.2 x 10(-6) Omega cm(2). Simultaneously, both the diffusion and the electrical deactivation of P are fully suppressed.
In situ ohmic contact formation for n-type Ge via non-equilibrium processing
Napolitani, E.;
2017
Abstract
Highly scaled nanoelectronics requires effective channel doping above 5 x 10(19) cm(-3) together with ohmic contacts with extremely low specific contact resistivity. Nowadays, Ge becomes very attractive for modern optoelectronics due to the high carrier mobility and the quasi-direct bandgap, but n-type Ge doped above 5 x 10(19) cm(-3) is metastable and thus difficult to be achieved. In this letter, we report on the formation of low-resistivity ohmic contacts in highly n-type doped Ge via non-equilibrium thermal processing consisting of millisecond-range flash lamp annealing. This is a single-step process that allows for the formation of a 90 nm thick NiGe layer with a very sharp interface between NiGe and Ge. The measured carrier concentration in Ge is above 9 x 10(19) cm(-3) with a specific contact resistivity of 1.2 x 10(-6) Omega cm(2). Simultaneously, both the diffusion and the electrical deactivation of P are fully suppressed.Pubblicazioni consigliate
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