Tony Hyun Kim April 23, 2009 6.152: MEMS Presentation.

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Presentation transcript:

Tony Hyun Kim April 23, : MEMS Presentation

1. Introduction 1. MEMS Cantilevers, Fixed-fixed beams 2. Theory of cantilever mechanics: Young’s modulus, etc. 2. Fabrication details 3. Experimental setup for mechanical test 4. Analysis and results 1. Young’s modulus of SiNx 2. Breaking point of the fixed-fixed beam 5. Sources of error 6. Conclusions

 Most ubiquitous structure in MEMS  Starting point for many applications:  Sensors  Platform for material experiments  It’s easy to build and easy to use (in principle). Image source: Hayden, Taylor. “MEMS Analysis 2” (On Stellar)

 Most ubiquitous structure in MEMS  Starting point for many applications:  Sensors  Platform for material experiments  It’s easy to build and easy to use (in principle). Our experimental goals: Build an array of MEMS cantilevers and fixed-fixed (FF) beams. Perform optical and mechanical verification of the devices.

 Once the structure is built, we want to test it.  i.e. perform consistency checks against literature Image source: Schwartzman, Alan. “MEMS Analysis 1” (On Stellar)

 The deflection of the target point (at distance L from fixed end):  Young’s modulus (E) is a material property measuring stiffness.

 Silicon nitride was deposited on wafer by Scott.  Thickness was measured by ellipsometry: SiN x Silicon wafer

 Silicon nitride patterned according to mask on left.  Pattern transferred by contact lithography.  The nitride was etched by SF 6 /plasma.

 Finally, an anisotropic etch (KOH) was utilized to etch the Si bulk.  Two hour etch in 80ºC KOH bath.  The orientation is stable against KOH   Allows for the material below the bridge to be removed first.

 “TriboIndenter” in the NanoLab  Optical microscope:  Position target.  Force-displacement transducer:  With a blunt tip.

 The spring constant is dependent on the point of application of force, L:  Can deduce Young’s modulus without L, by the above scheme

 The Young’s modulus was computed using the following:  “b” is the slope of k -1/3 vs. L  Optically measured width (W); thickness (t) from ellipsometry  Our results are within 1 std. of published values.

 Geometric complications  Sloped cantilevers  “Effective” width smaller  Undercut below the fixed-end

 Constructed MEMS cantilevers (and fixed beams)  Performed a mechanical experiment using the cantilevers  Provides consistency check:  Also verifies MEMS as useful platform for doing material studies.

 Model is:  Young’s modulus is directly related to the cubic coefficient.

 Young’s modulus through the cubic coefficient a:  Significant deviation from published values.

 Possible sources of errors to consider:  Sloped edges have huge effect on width: 6 vs. 9 um.  Bridge is slanted  Force-displacement profile prefers quadratic term.