Page 50 - Wire Bonding in Microelectronics
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Ultrasonic Bonding Systems and Technologies       29


              interfacial motion ceases. ∗  Ultrasonic energy is then absorbed into the
              entire weldment area (wire, interface, and bond pad). As a consequence
              of deformation cleaning, the center of the bond area is left relatively
              unwelded in wedge bonds. This may not occur if there are orbital or
              sideways tool vibration modes present during bonding causing some
              center welding to occur.
                 Extensive microstructural details of bond interfaces were obtained
              with a transmission electron microscope [2-19] as well as some using
              a SEM [2-1]. Those taken along the interface of monometallic US
              welds showed, variously, grain boundaries, no grain boundaries,
              debris zones of oxides, and contaminants, as well as numerous crys-
              tallographic defects. However, in general, the monometallic bonding
              process results in interface formation that is similar to grain bound-
              aries in polycrystalline materials, but continuous along the interface.
              Au-Al US welds, made at room temperature, show debris zones as
              well as clear metallic boundaries (similar to grain boundaries). There
              are also intermetallics along this boundary, which are a normal part
              of such Au-Al bond formation [2-31]. As a consequence of deforma-
              tion cleaning, the center of the bond area is left unwelded (minimum
              mass motion occurs in the center of a compressed, deforming ball/
              wire). This may not occur if there are orbital or sideways tool (capil-
              lary) vibration modes present during bonding. Such modes can be
              easily revealed by modern laser vibrometer measurements as was
              shown in Fig 2-9.
                 Contaminants in the bond interface can inhibit weld formation by
              preventing the deforming metal surfaces from coming into intimate
              contact. A thin, hard oxide on a soft metal, such as 0.5 to 1 nm (50–100 A)
              of Al O  on Al, will break up and be thinly dispersed or pushed
                  2  3
              into “debris” zones with little effect on the average welded area.
              However, soft oxides on harder metals, such as NiO on Ni (which is
              used in large-wire power device packages), appear to serve as a lubri-
              cant during initial weldment contact and deformation, remaining on
              the surface and preventing weld formation. This holds true for soft
              oxides (e.g., Cu O ) on soft metals (e.g., whereas Au does not have an
                           x  y
              oxide, diffused-to-the-surface Cu will oxidize and has been shown to
              significantly increase the activation energy required for Au-to-Au TC
              bonding [2-32]). Also, as little as 0.2 nm (20 A) of a carbonaceous con-
              taminant has been shown to reduce bondability on any bonding sur-
              face (see Chap. 7). Thus, it is important to understand the nature of a

              ∗ Joshi [2-1] used a laser interferometer and observed that the tool, the bond, the
              pad, and the laminated polymer substrate moved in unison during most of the
              bonding process. This substrate motion would not occur on hard, brittle substrates,
              such as silicon or ceramic. Here the final motion must be between the tool and
              the wire, as was found in [2-9]. Ultrasonic energy is then absorbed into the entire
              weldment volume (wire, interface, and bond pad).
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