Low Schottky Barrier on N-Type Si for N-Channel Schottky Source/Drain MOSFETs

2003 ◽  
Vol 765 ◽  
Author(s):  
Meng Tao ◽  
Darshak Udeshi ◽  
Shruddha Agarwal ◽  
Nasir Basit ◽  
Eduardo Maldonado ◽  
...  

AbstractSchottky source/drain (S/D) in Si-CMOS provide an alternative to current approaches in S/D, channel, and gate-stack engineering. The Schottky S/D PMOS has been demonstrated at a number of university and industrial laboratories. The bottleneck for the Schottky S/D NMOS is the fact that none of the common metals or metal silicides has a low enough barrier height (~0.2 eV) on n-type Si. A method to produce low Schottky barriers on n-type Si with common metals including aluminum (Al) and chromium (Cr) is reported in this paper. The interface between metal and Si(100) is engineered at the atomic scale with a monolayer of selenium (Se) to reduce the density of interface states, and the engineered interface shows inertness to chemical and electronic processes at the interface. One consequence of this electronic inertness is that the Schottky barrier is now more dependent on the metal work function. Al and Cr both have work functions very close to the Si electron affinity. It is found that the Schottky barrier of Al on Se-engineered n-type Si(100) is 0.08 eV, and that of Cr is 0.26 eV. These numbers agree well with the ideal Schottky barrier heights for Al and Cr on n-type Si(100), but are significantly different from the barrier heights known for four decades for these metals on n-type Si(100). These results bring new hope for the Schottky S/D NMOS with a metal commonly used in the Si industry.

2009 ◽  
Vol 615-617 ◽  
pp. 427-430 ◽  
Author(s):  
Shaweta Khanna ◽  
Arti Noor ◽  
Man Singh Tyagi ◽  
Sonnathi Neeleshwar

Available data on Schottky barrier heights on silicon and carbon rich faces of 4H-SiC have been carefully analyzed to investigate the mechanism of barrier formation on these surfaces. As in case of 3C and 6H-SiC, the barrier heights depend strongly upon method of surface preparation with a considerable scatter in the barrier height for a given metal-semiconductor system. However, for each metal the barrier height depends on the metal work function and strong pinning of the Fermi level has not been observed. The slopes of the linear relation between the barrier heights and metal work functions varies over a wide range from 0.2 to about 0.75 indicating that the density of interface states depends strongly on the method of surface preparation. By a careful examination of the data on barrier heights we could identify a set of nearly ideal interfaces in which the barrier heights vary linearly with metal work function approaching almost to the Schottky limit. The density of interface states for these interfaces is estimated to lie between 4.671012 to 2.631012 states/ cm2 eV on the silicon rich surface and about three times higher on the carbon rich faces. We also observed that on these ideal interfaces the density of interface states was almost independent of metal indicating that the metal induced gap states (MIGS) play no role in determining the barrier heights in metal-4H-SiC Schottky barriers.


2004 ◽  
Vol 59 (11) ◽  
pp. 795-798 ◽  
Author(s):  
Güven Çankaya ◽  
Nazım Uçar

We investigated Schottky barrier diodes of 9 metals (Mn, Cd, Al, Bi, Pb, Sn, Sb, Fe, and Ni) having different metal work functions to p-type Si using current-voltage characteristics. Most Schottky contacts show good characteristics with an ideality factor range from 1.057 to 1.831. Based on our measurements for p-type Si, the barrier heights and metal work functions show a linear relationship of current-voltage characteristics at room temperature with a slope (S=ϕb/ϕm) of 0.162, even though the Fermi level is partially pinned. From this linear dependency, the density of interface states was determined to be about 4.5 · 1013 1/eV per cm2, and the average pinning position of the Fermi level as 0.661 eV below the conduction band


Nanoscale ◽  
2018 ◽  
Vol 10 (1) ◽  
pp. 319-327 ◽  
Author(s):  
Jenifer R. Hajzus ◽  
Adam J. Biacchi ◽  
Son T. Le ◽  
Curt A. Richter ◽  
Angela R. Hight Walker ◽  
...  

Four different metals were patterned onto individual, solution-synthesized SnS nanoribbons to determine Schottky barrier heights and specific contact resistances.


2003 ◽  
Vol 82 (24) ◽  
pp. 4364-4366 ◽  
Author(s):  
Zhaojun Lin ◽  
Wu Lu ◽  
Jaesun Lee ◽  
Dongmin Liu ◽  
Jeffrey S. Flynn ◽  
...  

1987 ◽  
Vol 95 ◽  
Author(s):  
Jerzy Kanicki

The contact properties between different metals and hydrogenated amorphous silicon, prepared by various deposition techniques in different laboratories, are reviewed. From these studies the appropriate metallizations have been established for the achievement of Schottky diode, quasi-ohmic or ohmic contact to undoped and doped films. The various characteristic parameters describing Schottky barrier interfaces such as ideality factor, current saturation, contact resistance and barrier height are discussed. The dependence of Schottky barrier height upon the metal work function, measuring and annealing temperature, and optical band-gap are also reported. The minority-carrier injection and series resistance effects on the contact properties of a-Si:H diodes are described. All the results are interpreted in terms of a self-consistent model that exhibits an electrode-limited to bulk-limited transition.


2017 ◽  
Vol 31 (24) ◽  
pp. 1750198
Author(s):  
Jian Wang ◽  
Jiang-Tao Cheng ◽  
Shang-Yi Ma ◽  
Hong-De Wang

The density function theory is used to explore the structures of alkyl-thiolate (RS, R=CH3, CF3) monolayer on the Cu(111) surface. By performing the total energy calculations for RS at three possible adsorption sites (fcc, hcp, bridge) with five different coverages (1/12, 1/9, 1/6, 1/4, 1/3), we obtained the stable adsorption configurations of the Cu–RS system. Especially, the effect of Van der Waals interaction on the adsorption configurations was studied by the DFT-D2 method. The work functions for Cu–RS (R=CH3, CF3) systems were calculated, we find that the CH3S adsorbed on the Cu(111) surface decreases the metal work function remarkably, and the work functions strongly depend on the coverage. In the case of the Cu–CF3S system, the results are just the opposite. Thus, controlling the kind and coverage of the surface adsorbates would be an effective technique to tune the work function of the metal.


2002 ◽  
Vol 745 ◽  
Author(s):  
James Pan ◽  
Christy Woo ◽  
Minh-Van Ngo ◽  
Bryan Tracy ◽  
Ercan Adem ◽  
...  

ABSTRACTThe metal gate process becomes a promising candidate for sub-65nm CMOS, due to the elimination of polysilicon depletion effects, and the possibility of adjusting the CMOS threshold voltage without more threshold implants. Our goal is to process mteal films with tunable work functions, in order to meet the demand of sub-65nm metal gate CMOS.PVD TaN films are deposited with various processing conditions. Auger analysis shows that by changing the nitrogen flow rate and the plasma power, the nitrogen content in the TaN films can be adjusted. In order to accurately determine the work function of these TaN materials, we have developed a Schottky Diode CV technique (or Metal-Silicon CV, or MS-CV). This approach not only improves the accuracy of the metal work function measurement, compared with the traditional MOS-CV technique (which is affected by the thickness and quality of the oxide), but also simplifies the fabrication.With the MS-CV's, we have successfully measured the work functions of Ni and Co, and compared the data with published references. The work function of PVD TaN actually decreases with higher nitrogen content, according to the Auger data and the MS-CV measurement, ranging from 3.42 – 4.20 Volts. The MS-CV technique is shown to be independent to the size of the capacitors, and is little affected by the measurement frequency. By changing the frequency from 100KHz to 1MHz, the error in the work function is less than 50mV.


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