Analysis of a Latent Deep Submicron CMOS Device Isolation Leakage Mechanism

Author(s):  
H. Sur ◽  
A. Cohen ◽  
E. de Muizon

Abstract An investigation into latent CMOS device isolation failures during the process development phase of an advanced 0.35 μm CMOS ASIC process is presented. The failure mechanism manifested itself electrically during wafer sort as a non-typical Iddq distribution and subsequently resulted in large leakage failures during reliability stress testing experiments. Emission microscopy analysis on failing units revealed specific leakage sites in the CMOS SRAM core. Layer removal/SEM inspections revealed no physical anomalies in the emission area. Manual toggling of the RAM internal electrical nodes revealed that the leakage occurred through a parasitic field transistor (i.e. between two P+ diffusion islands gated by a polysilicon runner). Probing of test structures with similar layout features revealed that the diffusion isolation between the P+ diffusions was marginal, resulting in subthreshold field leakage. In addition, the subthreshold leakage current between the two diffusions on the test structures increased as a function of stress voltage and time - similar to the failing signature of the actual SRAM. The mechanism responsible for the latent increase in leakage current is believed to be electron trapping near the drain end of the parasitic field device. Improvement of the transistor isolation properties was achieved through process modifications and subsequently the failure mechanism was eliminated

2019 ◽  
Vol 13 (2) ◽  
pp. 229-235
Author(s):  
Brett N. Williams ◽  
Filip Bauwens ◽  
Thomas Haskett ◽  
Steven Vandeweghe ◽  
Todd A. Corsetti ◽  
...  

Coatings ◽  
2019 ◽  
Vol 9 (11) ◽  
pp. 720
Author(s):  
He Guan ◽  
Shaoxi Wang

Au-Pt-Ti/high-k/n-InAlAs metal-oxide-semiconductor (MOS) capacitors with HfO2-Al2O3 laminated dielectric were fabricated. We found that a Schottky emission leakage mechanism dominates the low bias conditions and Fowler–Nordheim tunneling became the main leakage mechanism at high fields with reverse biased condition. The sample with HfO2 (4 m)/Al2O3 (8 nm) laminated dielectric shows a high barrier height ϕB of 1.66 eV at 30 °C which was extracted from the Schottky emission mechanism, and this can be explained by fewer In–O and As–O states on the interface, as detected by the X-ray photoelectron spectroscopy test. These effects result in HfO2 (4 m)/Al2O3 (8 nm)/n-InAlAs MOS-capacitors presenting a low leakage current density of below 1.8 × 10−7 A/cm2 from −3 to 0 V at 30 °C. It is demonstrated that the HfO2/Al2O3 laminated dielectric with a thicker Al2O3 film of 8 nm is an optimized design to be the high-k dielectric used in Au-Pt-Ti/HfO2-Al2O3/InAlAs MOS capacitor applications.


2011 ◽  
Author(s):  
K. Tomida ◽  
M. Popovici ◽  
J. Swerts ◽  
W. C. Wang ◽  
B. Kaczer ◽  
...  

1977 ◽  
Vol 3 (4) ◽  
pp. 233-246 ◽  
Author(s):  
J. Brettle ◽  
N. F. Jackson

The failure mechanism of solid tantalum and aluminium capacitors have been investigated using a combination of electrical measurements and electron microscopy. The capacitor dielectric was examined before and after life testing and changes correlated with electrical measurements.The basic mechanism of failure of solid tantalum capacitors is found to be field crystallisation of the essentially amorphous dielectric oxide. The growth of higher conductivity crystalline oxide during operation of the capacitors causes an increase in leakage current and may result in catastrophic failure. The effect of field crystallisation can be minimised by using high purity tantalum to reduce the number of crystallisation nucleation sites. Since crystalline growth is primarily dependant on applied voltage, high voltage capacitors are much more susceptible to failure than low voltage units.There appears to be no long term failure mechanism in solid aluminium capacitors. However, a particular problem with these units is that they are difficult to make. This is because the anodic layer is chemically less stable in the case of aluminium than in the case of tantalum. The attack is initiated during the deposition of manganese oxide by pyrolysis from manganese nitrate solution and developed by the reform process. Solid aluminium capacitors often have a lower capacitance and higher initial leakage current than comparable solid tantalum units; however, the leakage current decreases on life tests and their reliability is high.


Author(s):  
Y.E. Hong ◽  
M.T.T. We

Abstract As transistor dimension shrinks down below submicron to cater for higher speed and higher packing density, it is very important to characterize the shrinkage carefully to avoid unwanted parametric problems. Leakage current across short poly end-cap is a new failure mechanism that falls in this category and was for the first time, uncovered in submicron multilayered CMOS devices. This mechanism was responsible for a systematic yield problem; identified as the 'centre wafer striping' functional failure problem. This paper presents the advanced failure analysis techniques and defect modeling used to narrow down and identify this new mechanism. Post process change by loosening the marginal poly end-cap criteria eliminated the problem completely.


2011 ◽  
Vol 32 (6) ◽  
pp. 064004 ◽  
Author(s):  
Zhangli Liu ◽  
Zhiyuan Hu ◽  
Zhengxuan Zhang ◽  
Hua Shao ◽  
Ming Chen ◽  
...  

2000 ◽  
Vol 611 ◽  
Author(s):  
Ken-ichi Goto

ABSTRACTWe have clarified a new leakage mechanism in Co salicide process for the ultra-shallow junctions of 0.1-um CMOS devices and revealed the optimum Co salicide process conditions for minimizing the leakage current. We found that leakage currents generate from many localized points that are randomly distributed in the junction area, and not from the junction edge. We successfully verified our localized leakage model using Monte Carlo simulation. We identified abnormal CoSix spiking growth under the Co silicide film, as being the origin of the localized leakage current. These CoSix spikes grow rapidly only during annealing between 400°C and 450°C when Co2Si phase is formed. These spikes never grow during annealing at over 500°C, and decrease with high temperature annealing over 500°C. A minimum leakage current can be achieved by optimized annealing at between 800°C and 850°C for 30 sec. This is because a trade-off between reducing the CoSix spikes and preventing the Co atom diffusion from Co silicide film to Si substrate, which begins at annealing above 900°C.


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