Evaluation of PECVD deposited Boron Nitride as Copper Diffusion Barrier on Porous Low-k Materials

2004 ◽  
Vol 812 ◽  
Author(s):  
J. Liu ◽  
W. D. Wang ◽  
L. Wang ◽  
D. Z. Chi ◽  
K. P. Loh

AbstractUltra low dielectric constant (κ) material is needed as the inter-metal dielectrics to reduce RC delay when device dimension is scaled to sub-100nm. Porous dielectric films have been considered as good candidates for the application as inter-metal dielectrics due to their ultra low-k properties. Identifying proper dielectric copper diffusion barrier on the porous low-k films is critical for the low-k/Cu damascene fabrication process. In this study, we have evaluated the compatibility of plasma-deposited amorphous Boron Nitride film as a dielectrics copper diffusion barrier on a MSQ-based porous low-k LKD5109 film (from JSR). Both microwave plasma enhanced CVD (2.45 GHz) and radio-frequency plasma enhanced CVD (13.56 MHz) were applied for the BN deposition in order to evaluate the compatibility of the two plasma processes with the porous film. Growth parameters were optimized to minimize the boron diffusion and carbon depletion in the porous low-k films, which were found to have deleterious effects on the dielectric properties of the low-k films. FTIR and micro-Raman were employed for analyzing the changes in chemical structure of the low-k films after BN growth. Capacitance-voltage measurement was used to characterize the dielectric constants of BN film on Si and the BN-deposited porous low-k film. SIMS characterization was carried out to evaluate the performance of the BN film against copper diffusion.

2012 ◽  
Vol 2 (3) ◽  
pp. P25-P27 ◽  
Author(s):  
N. Jourdan ◽  
Y. Barbarin ◽  
K. Croes ◽  
Y. Kong Siew ◽  
S. Van Elshocht ◽  
...  

2007 ◽  
Author(s):  
S. Tokuyama ◽  
M. K. Mazumder ◽  
D. Watanabe ◽  
C. Kimura ◽  
H. Aoki ◽  
...  

2009 ◽  
Vol 18 (5-8) ◽  
pp. 1048-1051 ◽  
Author(s):  
Hidemitsu Aoki ◽  
Shinji Tokuyama ◽  
Takuro Masuzumi ◽  
Makoto Hara ◽  
Motaharu Kabir Mazumder ◽  
...  
Keyword(s):  

1997 ◽  
Vol 46 (1-3) ◽  
pp. 101-104 ◽  
Author(s):  
O. Baehr ◽  
P. Thévenin ◽  
A. Bath ◽  
A. Koukab ◽  
E. Losson ◽  
...  

2018 ◽  
Author(s):  
K. A. Rubin ◽  
W. Jolley ◽  
Y. Yang

Abstract Scanning Microwave Impedance Microscopy (sMIM) can be used to characterize dielectric thin films and to quantitatively discern film thickness differences. FEM modeling of the sMIM response provides understanding of how to connect the measured sMIM signals to the underlying properties of the dielectric film and its substrate. Modeling shows that sMIM can be used to characterize a range of dielectric film thicknesses spanning both low-k and medium-k dielectric constants. A model system consisting of SiO2 thin films of various thickness on silicon substrates is used to illustrate the technique experimentally.


1993 ◽  
Vol 316 ◽  
Author(s):  
T. A. Friedmann ◽  
D. L. Medlin ◽  
P. B. Mirkarimi ◽  
K. F. McCarty ◽  
E. J. Klaus ◽  
...  

ABSTRACTWe are studying the boron nitride system by using a pulsed excimer laser to ablate from hexagonal BN (hBN) targets to form cubic BN (cBN) films. We are depositing BN films on heated (25 - 800°C) Si (100) surfaces and are using a broad-beam ion source operated with Ar and N2 source gasses to produce BN films with a high percentage of sp3-bonded cBN. In order to understand and optimize the growth and nucleation of cBN films, parametric studies of the growth parameters have been performed. The best films to date show >85% sp3-bonded BN as determined from Fourier-transform infrared (FTIR) reflection spectroscopy. High resolution transmission electron microscopy (TEM) and selected area electron diffraction confirm the presence of cBN in these samples. The films are polycrystalline and show grain sizes up to 30- 40 nm. We find from both the FTIR and TEM analyses that the cBN content in these films evolves with growth time. Initially, the films are deposited as hBN and the cBN nucleates on this hBN underlayer. Importantly, the position of the cBN IR phonon also changes with growth time. Initially this mode appears near 1130 cm-1 and the position decreases with growth time to a constant value of 1085 cm-1. Since in bulk cBN this IR mode appears at 1065 cm-1, a large compressive stress induced by the ion bombardment is suggested. In addition, we report on the variation in cBN percentage with temperature.


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