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Single-Crystal Silicon Carbide MEMS: Fabrication, Characterization, and Reliability         7-5


             Hillocks between 10 µm and 50µm formed randomly on the diaphragm surface. The presence of uncon-
             trollable discontinuities of this size results in nonuniform stress distributions that adversely affect the
             operation of a sensor. Although the cause of the hillock formation was not conclusively determined, there
             was evidence that the formations were associated with bubbles generated during the high-rate etching.
               The existence of micropipes in the SiC wafers, which could lead to high current–density concentrations
             in localized areas, could result in selectively high etch rates around the defect sites, increasing the possi-
             bility of etch pit formation. Although the etching potential of highly doped n-type SiC using the ECE
             process  is  much  higher  than  that  of p-type SiC, it  is  possible  to  stop  the  etching  process  at  the  np-

             junction if the ohmic contact used for anodization potential control is made only to the n -SiC epilayer
             (refer to Figure 7.1). The positive anodic potential on the n -SiC layer will cause the junction  to be
                                                                      +
             reverse-biased, thereby preventing the flow of current through the underlying p-SiC epilayer. In order for
             the etch-stop to be effective, the breakdown voltage of the np-junction must be higher than the etching

             potential of the n -SiC epilayer. Also, the p-type layer should have a doping level significantly lower than

             that of the n -SiC epilayer to minimize the possibility of tunneling current [Shor et al., 1993].
               The process of using PECE of SiC for the purpose of fabricating well-defined resistor structures is
             described as follows. As shown in Figure 7.1, the starting wafer is an n-type 6H-SiC substrate upon which
                                                   3
                                              18
             a 5-µm thick, lightly doped (3   10 cm ) p-type epilayer is grown by CVD, followed by a 2µm thick

             n -type 6H-SiC epilayer. An ohmic contact metallization, preferably nickel, is deposited and patterned

             into a circular shape on the top n -SiC epilayer to enable control of the anodization potential during the
             PECE process. Platinum is sputtered onto the top of the wafer, covering the ohmic contact metal and the

             entire n -SiC epilayer. The platinum in direct contact with the epilayer is then patterned into the shape of
             serpentine resistor elements. This platinum acts as an etch mask, so that the serpentine resistor patterns

             can be transferred onto the n -SiC during the PECE process. Contact electrode wire is wire-bonded on
             the section of the platinum mask that is in direct contact with the nickel ohmic contact. A thin layer of
             black wax is then applied over areas covered by the ohmic contact electrode. The wafer is then immersed
             in dilute HF electrolyte, with the side to be etched facing up. This face is then exposed to a UV light
             source, with the anodization potential set at 1.7V  (SCE means Standard Calomel Electrode, which is
                                                          SCE
             the reference electrode against which the anode voltage is measured). Under this condition, the exposed

             sections of the n -SiC epilayer are photoelectrochemically etched, and the sections under the serpentine-
             shaped platinum etch mask are unetched. After the anodization process, the wax is stripped in acetone
             and the platinum mask and nickel ohmic contacts are stripped in aqua regia and nitric-hydrochloric acid

             in a 50:50 mixture, respectively. After stripping, the resistor patterns transferred to the n epilayer are
             revealed.
               The current vs. time curves of a typical PECE are shown in Figure 7.2. For the epilayer thickness used,
             the photocurrent rises to a first maximum in the first five minutes, and then drops rapidly because of the
             blocking action of the bubbles during the release of gaseous products. A second maximum appears in the
             curve  after  twelve  minutes, when  the  bubbles  deflate, after  which  time  the  current  density  gradually


                                  2.0
                                                               P UV  = 90 mW/cm 2
                                  1.5                             Run 1
                                Current (mA)  1.0                 Run 2




                                  0.5

                                   0
                                     0           10           20           30           40
                                                           Time (min)

             FIGURE 7.2 Current density vs. time during photoelectrochemical etching of n-type 6H-SiC in dilute HF electrolyte.
             Two anodization I–t characteristics indicate the reproducibility of the process as long as ohmic contact is present.



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