1997
DOI: 10.1109/16.644639
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The influence of TiN ARC thickness on stress-induced void formation in tungsten-plug vias

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Cited by 12 publications
(5 citation statements)
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“…Therefore, the ratio of for narrow to wide line/via structure is given by (2) where the superscripts narrow and wide correspond to the narrow and wide line/via, respectively. The subscript int refers to the interface current density at the line/via bottom interface, and is the difference in activation energies of the narrow and wide line/via structures which is found to be eV as computed previously.…”
Section: Via Bottom Current Density Dependencymentioning
confidence: 99%
“…Therefore, the ratio of for narrow to wide line/via structure is given by (2) where the superscripts narrow and wide correspond to the narrow and wide line/via, respectively. The subscript int refers to the interface current density at the line/via bottom interface, and is the difference in activation energies of the narrow and wide line/via structures which is found to be eV as computed previously.…”
Section: Via Bottom Current Density Dependencymentioning
confidence: 99%
“…Table 2 summarizes the contribution from the various mechanisms of EM at the three stress conditions. In all three cases, the dominant mechanism found is SM, which is consistent with the reports from other works [47,74].…”
Section: Finite Element Modelingsupporting
confidence: 92%
“…Once the current density in an interconnect line exceeds the maximum current-carrying capacity J max of the conductor, the material fails due to the displacement of atoms along the path of electrons, resulting in voids, and such a mechanism is known as electromigration. The J max of Cu is 2.5 MA cm −2 [20] and 1 MA cm −2 for W [21,22]. In order to extend the J max for Cu and W, material engineering approaches such as stress engineering and capping are employed [2].…”
Section: Introductionmentioning
confidence: 99%