Page 272 - Sami Franssila Introduction to Microfabrication
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Process Integration 251




                             Na +      −  − +  +
                                                                   + + +
                            Silicon substrate
           Figure 24.16 Oxide defects (left to right): Na +  mobile charge, thinning, fixed charge, surface and interface
           microroughness, pinhole, void, interface charge, particle, stacking fault. Adapted from Schr¨ oder, D.K. (1998), by
           permission of John Wiley & Sons

           Unreactive metals dissolve in the growing oxide, which  In polycrystalline material, grain boundary diffusion is
           leads to decreased intrinsic breakdown strength. Sodium  important and the elimination of grain boundaries will
           (Na) contamination leads to increased oxidation rate;  affect electromigration.
           whereas iron (Fe) and aluminium (Al) lead either  Mean time to failure (MTF) due to electromigration
           to increase or decrease depending on the level of  is given by
           contamination and time. Metals can also catalyse the
           reaction SiO 2 (s) + Si (s) → 2 SiO (g) (which takes   MTF = AJ  −n  exp (Ea/kT )  (24.3)
           place under low oxygen partial pressure, e.g., during
           ramp-up in a furnace), leading to oxide evaporation and  where A is a constant dependent on wire geometry and
           pinhole-like defects.                       metal microstructure, J is the current density and E a the
             Oxide dielectric strength is tested by a number of  activation energy. The factor n is not known accurately,
           different experimental set-ups:             but n = 1.7 is a usable value for aluminium.
                                                         For aluminium thin films E a is of the order of 0.5
           – Ramped voltage: the voltage between MOS gate and  to 0.8 eV, whereas for bulk aluminium it is 1.4 to
              substrate is linearly increased (0.1 or 1 V/s) until  1.5 eV. As a general trend, the higher the activation
              the oxide breaks down. Breakdown voltage V BD  energy, the better the electromigration resistance. It can
              is defined as the voltage where a sudden voltage  be roughly estimated on the basis of metal melting
              drop occurs.                             point T m : the higher the melting point, the higher
           – Time-to-breakdown under constant current (TTBD;  the electromigration resistance. To put it in another
              t BD ): constant, preset current is fed into the insulator,  way: high melting point equals high bond energy.
              and the voltage is recorded as a function of  At room temperature, which is T m /3 for aluminium,
              time. TTBD is the time when a sudden voltage  aluminium atoms have a reasonable probability for
              drop occurs.                             diffusion. For tungsten, room temperature corresponds
           – Charge-to-breakdown (Q BD ): in constant current  to T m /10, and electromigration is less by orders of
              test Q BD = J injected × t BD . Good oxides exhibit val-  magnitude. Copper falls between the two. For short lines
                          2
              ues of 10 C/cm , but this is dependent on the  and/or for low current densities, electromigration is not
              injected current.                        an issue.
           24.9.2 Electromigration
                                                       24.9.3 Stress migration
           Electromigration (recall page 58) depends on a large
           number of factors: macroscopic factors include geome-  Electromigration is studied by accelerated tests under
           try of the lines, and their width, shape and area. Micro-  higher-than-normal current densities at elevated temper-
           scopic factors include grain size, texture, and alloy  atures. However, voids appear in metal lines at elevated
           solutes and their precipitation at the grain boundaries  temperatures even when no current runs through them.
           and interfaces. Solutes like copper in aluminium (e.g.,  This is known as stress-induced voiding or stress migra-
           in Al-2 wt% Cu) increase resistance to electromigra-  tion. The driving force is the gradient in the strain field:
           tion because copper atoms block diffusion at grain  some atoms find it energetically favourable to move
           boundaries (Figure 24.17). What is more, grain size  to voids.
           and linewidth are not independent: when grain size and  The source of stress is thermal expansion mis-
           linewidth become equal (typically when thickness-to-  match between metal and the encapsulating (PE)CVD
           width ratio is about unity), the number of grain bound-  dielectric. Strain (elongation) is proportional to CTE
           aries is strongly reduced, leading to the so-called bam-  and temperature difference, which translates, for alu-
           boo structure with one grain extending across the line.  minum, to 1% linear elongation or ca. 3% volume
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