TY - JOUR
T1 - Source/Drain Materials for Ge nMOS Devices: Phosphorus Activation in Epitaxial Si, Ge, Ge1-xSnx and SiyGe1-x-ySnx
AU - Vohra, Anurag
AU - Makkonen, Ilja
AU - Pourtois, Geoffrey
AU - Slotte, Jonatan
AU - Porret, Clement
AU - Rosseel, Erik
AU - Khanam, Afrina
AU - Tirrito, Matteo
AU - Douhard, Bastien
AU - Loo, Roger
AU - Vandervorst, Wilfried
PY - 2020/5/7
Y1 - 2020/5/7
N2 - This paper benchmarks various epitaxial growth schemes based on n-type group-IV materials as viable source/drain candidates for Ge nMOS devices. Si:P grown at low temperature on Ge, gives an active carrier concentration as high as 3.5 × 1020 cm−3 and a contact resistivity down to 7.5 × 10−9 Ω.cm2. However, Si:P growth is highly defective due to large lattice mismatch between Si and Ge. Within the material stacks assessed, one option for Ge nMOS source/drain stressors would be to stack Si:P, deposited at contact level, on top of a selectively grown n-Si y Ge1−x−y Sn x at source/drain level, in line with the concept of Si passivation of n-Ge surfaces to achieve low contact resistivities as reported in literature (Martens et al. 2011 Appl. Phys. Lett., 98, 013 504). The saturation in active carrier concentration with increasing P (or As)-doping is the major bottleneck in achieving low contact resistivities for as-grown Ge or Si y Ge1−x−y Sn x . We focus on understanding various dopant deactivation mechanisms in P-doped Ge and Ge1−x Sn x alloys. First principles simulation results suggest that P deactivation in Ge and Ge1−x Sn x can be explained both by P-clustering and donor-vacancy complexes. Positron annihilation spectroscopy analysis, suggests that dopant deactivation in P-doped Ge and Ge1−x Sn x is primarily due to the formation of P n -V and Sn m P n -V clusters.
AB - This paper benchmarks various epitaxial growth schemes based on n-type group-IV materials as viable source/drain candidates for Ge nMOS devices. Si:P grown at low temperature on Ge, gives an active carrier concentration as high as 3.5 × 1020 cm−3 and a contact resistivity down to 7.5 × 10−9 Ω.cm2. However, Si:P growth is highly defective due to large lattice mismatch between Si and Ge. Within the material stacks assessed, one option for Ge nMOS source/drain stressors would be to stack Si:P, deposited at contact level, on top of a selectively grown n-Si y Ge1−x−y Sn x at source/drain level, in line with the concept of Si passivation of n-Ge surfaces to achieve low contact resistivities as reported in literature (Martens et al. 2011 Appl. Phys. Lett., 98, 013 504). The saturation in active carrier concentration with increasing P (or As)-doping is the major bottleneck in achieving low contact resistivities for as-grown Ge or Si y Ge1−x−y Sn x . We focus on understanding various dopant deactivation mechanisms in P-doped Ge and Ge1−x Sn x alloys. First principles simulation results suggest that P deactivation in Ge and Ge1−x Sn x can be explained both by P-clustering and donor-vacancy complexes. Positron annihilation spectroscopy analysis, suggests that dopant deactivation in P-doped Ge and Ge1−x Sn x is primarily due to the formation of P n -V and Sn m P n -V clusters.
UR - http://www.scopus.com/inward/record.url?scp=85085249895&partnerID=8YFLogxK
U2 - 10.1149/2162-8777/ab8d91
DO - 10.1149/2162-8777/ab8d91
M3 - Article
SN - 2162-8777
VL - 9
SP - 1
EP - 13
JO - ECS Journal of Solid State Science and Technology
JF - ECS Journal of Solid State Science and Technology
IS - 4
M1 - 044010
ER -