2005
DOI: 10.1063/1.2150581
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Effective Schottky barrier lowering in silicon-on-insulator Schottky-barrier metal-oxide-semiconductor field-effect transistors using dopant segregation

Abstract: We present an investigation of the use of dopant segregation in Schottky-barrier metal-oxide-semiconductor field-effect transistors on silicon-on-insulator. Experimental results on devices with fully nickel silicided source and drain contacts show that arsenic segregation during silicidation leads to strongly improved device characteristics due to a strong conduction/valence band bending at the contact interface induced by a very thin, highly doped silicon layer formed during the silicidation. With simulations… Show more

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Cited by 81 publications
(44 citation statements)
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“…This means that the device behaves like a "bulk-switching", conventional MOSFET, where thermionic emission of carriers over the source bulk potential barrier in the channel is responsible for the current flow instead of tunneling through a SB. The reason for this is a strongly decreased effective SB height due to the highly doped area at the silicide-silicon interface [22]. The highly doped layer leads to a strong band bending at the interface.…”
Section: 3mentioning
confidence: 99%
“…This means that the device behaves like a "bulk-switching", conventional MOSFET, where thermionic emission of carriers over the source bulk potential barrier in the channel is responsible for the current flow instead of tunneling through a SB. The reason for this is a strongly decreased effective SB height due to the highly doped area at the silicide-silicon interface [22]. The highly doped layer leads to a strong band bending at the interface.…”
Section: 3mentioning
confidence: 99%
“…by inserting a thin insulator layer [3] or by creating a highly doped region located at the silicide/Si interface with a dopant segregation technique [5]- [6]. To our knowledge, no such reports were available for hole SBH modulation.…”
Section: Introductionmentioning
confidence: 99%
“…I DS vs V GS was measured from room temperature up to 90°C for V DS =−5 V. Figure 2 shows drain current I DS as a function of the gate voltage V GS for a drain voltage V DS of −5 V and for different temperatures in the range of 303-363 K. Two distinct kinks are observed among the graphs, dividing the coordinate plane into three regimes, A, B, and C, in a similar manner as found in planar Schottky barrier metal-oxide-semiconductor field effect transistors. 11 For negative V GS values in regime A, where the energy bands in the channel between the source and drain contacts tend to be bended to higher electron energies, hole injection from source is favored. In regime B, the energy bands in the channel are pressed down by V GS in relation to the drain contact.…”
mentioning
confidence: 99%