In order to identify suitable diffusion barrier materials for Cu, the diffusion of Cu into Si through these barrier metals was investigated. The behavior of Cu in Cu/M/Si multi-layers was measured, after annealing, by using X-ray diffraction analysis, secondary ion mass spectroscopy, Rutherford back-scattering spectroscopy, and resistometry. It was found that only Cu/Ta/Si and Cu/W/Si multi-layers retained their multilayer structures after annealing (600C, 1h, H2), without resistivity increases. Multi-layers of the other metals did not retain their structures under the same annealing conditions. The differences in barrier properties were attributed to differing forms of the metal-Cu binary phase diagrams, and to their self-diffusion coefficients.
Diffusion Barrier Effects of Transition Metals for Cu/M/Si Multilayers (M = Cr, Ti, Nb, Mo, Ta, W). H.Ono, T.Nakano, T.Ohta: Applied Physics Letters, 1994, 64[12], 1511-3
Table 76
Diffusivity of Be in Cu Crystals
Temperature (K) | Annealing Ambient | D (m2/s) |
583 | vacuum | 3.00 x 10-22 |
597 | vacuum | 6.97 x 10-22 |
603 | vacuum | 9.36 x 10-22 |
605 | vacuum | 1.00 x 10-21 |
615 | vacuum | 2.28 x 10-21 |
642 | vacuum | 1.21 x 10-20 |
651 | Ar/H2 | 1.56 x 10-20 |
654 | Ar/H2 | 2.13 x 10-20 |
654 | vacuum | 1.80 x 10-20 |
655 | vacuum | 2.27 x 10-20 |
682 | vacuum | 6.07 x 10-20 |
702 | vacuum | 1.70 x 10-19 |
705 | Ar/H2 | 1.73 x 10-19 |
718 | Ar/H2 | 3.93 x 10-19 |
730 | vacuum | 7.05 x 10-19 |
730 | vacuum | 6.82 x 10-19 |
751 | Ar/H2 | 1.50 x 10-18 |
774 | Ar/H2 | 5.00 x 10-18 |
800 | Ar/H2 | 1.30 x 10-17 |