Page 128 - Wire Bonding in Microelectronics
P. 128

106    Cha pte r  F o u r


                 Table 4-1 was summarized from extensive data from several
              sources to show the bond characteristics and values obtained by this
              method. Shear force, SS values, and intermetallic percentages are com-
              pared for bonds intended for a range of fine-pitch processes. The cor-
              relation between the amount of intermetallic, or metal disruption, on
              the ball and the shear strength has been established [4-26, 4-27], and,
              thus, the actual amount of intermetallic is only determined occasion-
              ally (e.g., for a major change in metallization or Au wire dopant).
                 One would assume that a simple square-law equation (related to
              the bonded-ball area) using the data from Table 4-1 could be used to
              predict the expected shear force of fine pitch bonds, knowing the actual
              welded area (percentage of intermetallics). This could then be related
              back to Fig. 4-17. However, the actual curve-fitting equation using data
              from Table 4-1 turned out to be less than square law. ∗  It is
                               SF          = 0.024 D 1.78           (4-7)
                                 (welded area dia.)
              where SF is the shear force in gf, and D is the equivalent diameter of the
              actual welded area in micrometers. The correlation coefficient is: r =
                                                                     2
              0.999. This equation can be used on fine-pitch bonds (≤100 µm) to deter-
              mine the equivalent welded diameter (and from that the percent that are
              intermetallics) or the shear force if the percentage of intermetallics is
              known. Also, using the data from Table 4-1, one can project that, for a
              60-µm pitch process, the effective bonded-ball diameter would be 34 µm
              (for 80% welded area and represents an actual diameter of 38 µm) and
              the shear force would be 13.4 gf. From Fig. 4-17 it would be nearer 12 gf,
              not a bad approximation. (See Chap. 9 for further fine pitch details.)
                 Using the actual measured bonded-ball diameter (in micrometers),
              the equation becomes:

                                 SF     = 0.023 D 1.75             (4-7a)
                                   (ball dia.)
                    2
              where r = 0.98. Equation (4-7a) assumes ∼80% welded area under the
              bonds, and the diameter is measured optically as the outer perimeter.
              This equation is easier to use than Eq. (4-7), since only the measured
              diameter of the bonded ball is required. However, since the welded
              area under production bonds normally varies, results on any experi-
              ment may also vary. Still, this equation is an adequate approximation
              for most finer-pitch (≤70  µm) situations (see testing of fine pitch
              bonds, Chap. 9).


              ∗ Since the actual bonded area was used, a square-law behavior related to the
              in creased cross-section should have been observed. The reasons for fine-pitch
              bonded balls producing a shear-force-to-bonded-area relationship different from
              larger diameter bonds are not understood, and more study is indicated. Very fine
              pitch bonds have been observed to have a larger percentage of welded area (shear
                                    2
              strengths consistently >7 gf/mil  than equivalent larger diameter balls).
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