Compound Semiconductors 1997. Proceedings of the IEEE Twenty-Fourth International Symposium on Compound Semiconductors 1997
DOI: 10.1109/iscs.1998.711642
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Hydrogenation effect of InGaP grown on GaAs by molecular beam epitaxy

Abstract: Hydrogenation effects on electrical properties of n-type and undoped InGaP epi layers lattice matched to GaAs was investigated. It was found that the hydrogenation under a proper condition can be resulted in a Auh-InGaP Schottky diode with a good rectifying characteristics as well as an effective defect passivation. These improvement were thought to be resulted from the atomic hydrogen diffused into InCaP neutralized Si donor and passivated recombination centers near the surface.

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“…The Schottky barrier height (SBH) at the metal‐semiconductor interface plays a key role in determining the contact resistance. In an ideal contact interface, the SBH (ϕB0) is given by the difference between the metal work function ( W m ) and the semiconductor electron affinity (χ s ), as predicted by the Schottky‐Mott rule [ 5 ] : ϕB0=Wmχs However, in a real scenario, the interfacial dipole, metal induced gap states (MIGS), and interfacial defects lead to Fermi level pinning (FLP), [ 6–8 ] which has plagued the development of ultra‐low resistance contacts for several materials, including n‐Ge, [ 9,10 ] p‐InGaAs, [ 11,12 ] and p‐MoS 2 . [ 13–17 ]…”
Section: Introductionmentioning
confidence: 99%
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“…The Schottky barrier height (SBH) at the metal‐semiconductor interface plays a key role in determining the contact resistance. In an ideal contact interface, the SBH (ϕB0) is given by the difference between the metal work function ( W m ) and the semiconductor electron affinity (χ s ), as predicted by the Schottky‐Mott rule [ 5 ] : ϕB0=Wmχs However, in a real scenario, the interfacial dipole, metal induced gap states (MIGS), and interfacial defects lead to Fermi level pinning (FLP), [ 6–8 ] which has plagued the development of ultra‐low resistance contacts for several materials, including n‐Ge, [ 9,10 ] p‐InGaAs, [ 11,12 ] and p‐MoS 2 . [ 13–17 ]…”
Section: Introductionmentioning
confidence: 99%
“…However, in a real scenario, the interfacial dipole, metal induced gap states (MIGS), and interfacial defects lead to Fermi level pinning (FLP), [6][7][8] which has plagued the development of ultra-low resistance contacts for several materials, including n-Ge, [9,10] p-InGaAs, [11,12] and p-MoS 2 . [13][14][15][16][17] In the context of the layered semiconductors, the possibility of ultra-clean, atomically smooth, dangling-bond-free surface, coupled with a relatively weak van der Waals (vdW) interaction at the interface reignited the hope to achieve a completely de-pinned contact close to the Schottky-Mott limit.…”
mentioning
confidence: 99%