A 600 Degrees C Wireless Multimorph-Based Capacitive MEMS Temperature Sensor for Component Health Monitoring

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Purdue University Purdue e-pubs Birck and NCN Publications Birck Nanotechnology Center 1-29-2012 A 600 Degrees C Wireless Multimorph-Based Capacitive MEMS Temperature Sensor for Component Health Monitoring S. Scott Birck Nanotechnology Center, Purdue University M. Scuderi Birck Nanotechnology Center, Purdue University, mscuderi@purdue.edu Dimitrios Peroulis Birck Nanotechnology Center, Purdue University, dperouli@purdue.edu Follow this and additional works at: http://docs.lib.purdue.edu/nanopub Part of the Nanoscience and Nanotechnology Commons Scott, S.; Scuderi, M.; and Peroulis, Dimitrios, "A 600 Degrees C Wireless Multimorph-Based Capacitive MEMS Temperature Sensor for Component Health Monitoring" (2012). Birck and NCN Publications. Paper 1281. http://dx.doi.org/10.1109/memsys.2012.6170246 This document has been made available through Purdue e-pubs, a service of the Purdue University Libraries. Please contact epubs@purdue.edu for additional information.

A 600 C WIRELESS MULTIMORPH-BASED CAPACITIVE MEMS TEMPERATURE SENSOR FOR COMPONENT HEALTH MONITORING S. Scott, M. Scuderi and D. Peroulis School of Electrical and Computer Engineering, Birck Nanotechnology Center, Purdue University, West Lafayette, IN, USA ABSTRACT This paper presents the design and fabrication of a new packaged MEMS capacitive temperature sensor for engine component health-monitoring applications and measurement results above 500-600 C. The multimorphs employed are thermal-sio 2 /LPCVD-Si 3 N 4 /sputtered-au beams designed for deflection at these temperatures. The mean initial capacitance of the sensors is 6.441 pf; with a standard deviation of 0.197 pf. The robust fabrication process and packaging yield consistent capacitancetemperature profiles from device-to-device. Similarly, the devices exhibit a consistently-high measured average quality factor of 1,727 with a standard deviation of 54 for 5 packaged devices. Also presented are laser confocal microscope profiles from the thermal-annealing process, detailing the break-in period, after which no additional creep is observed, even after over 24 hours at 650 C. This is a first-of-its-kind MEMS sensor with unparalleled performance for harsh-environment wireless temperature sensing. INTRODUCTION In a variety of applications, engine components undergo a large amount of maintenance. For many components, this maintenance is scheduled, and occurs regardless of necessity. In order to reduce this, it is highly-desirable to create sensors that can create an accurate depiction of component health, so maintenance only needs to be performed when the component starts to fail [1]. One such component is a bearing. When a crack or spall forms in the bearing, temperature due to friction begins to increase. The defect propagates over time, and with it, the temperature rise continues until failure. For this reason, it would be optimal to have a temperature sensor as close as possible to the point of failure, monitoring for any shift outside of a specified tolerance for a given speed. These wireless sensors need to operate in temperature ranges not possible with existing technologies. Some high-speed engine components reach operating at temperatures as high as 600 C. While desire for these harsh environment sensors has existed for some time, little in the way of solutions has been demonstrated. Thermocouples, fiber optic sensors [2], or SAW-based sensors are robust solutions, but unfortunately are not appropriate when a wired connection and line-of-sight are not feasible. Active silicon circuits unfortunately do not operate far beyond 120 C due to the small band-gap. High band-gap active circuits such as Silicon Carbide (SiC) or Gallium Nitride (GaN) have been demonstrated [3], but they suffer from reliability issues when operation for extended periods of time at these temperatures is desired [4]. Powering these devices also becomes problematic as battery use is not practical at these temperatures. Some work has been completed in passive implementations for sensors suitable at these temperatures. For example, passive SiC-based pressure sensors have been shown to operate at temperatures up to 600 C [5]. However, even these sensors require temperature compensation for accurate pressure knowledge. The authors present a passive, capacitive temperature-sensing solution based on multimorph cantilevers. As temperature increases, the cantilevers deflect due to the mismatch in the thermal coefficients of expansion. This deflection results in a change in capacitance between the cantilever and a fixed electrode. The passive implementation, silicon micro-fabrication, and robust materials used result in an inexpensive, yet efficient sensor for harsh environment applications. The first section details the design of the sensor, including electromagnetic considerations. Next, the fabrication and associated packaging are discussed. This is followed by the experimental results including capacitance performance and quality factor. Also performed is an experimental study detailing the annealing of the sensor and preliminary reliability results (creep testing) for over 24 hours at 650 C. DESIGN Analytical models for multimorph cantilevers have been presented in [4]. The authors have also demonstrated the use of thermally-grown SiO 2 results in veryrobust devices with excellent reliability performance to 300 C [6]. As temperature increases, the cantilevers deflect downward, increasing capacitance between the beam and the conductive silicon substrate. Using the silicon substrate as an electrode simultaneously reduces the complexity of the design and increases the quality factor (Q) of the device. There are several options that can be employed when pushing the operation to higher temperatures. For one, the gold film previously used can be replaced with a low-cte film like tungsten or molybdenum. However, these were found to be incompatible with the XeF 2 release process, one of the factors that resulted in very high yield. The gold is also a useful material to wirebond to. Instead, the authors consider a tri-layer multimorph consisting of thermal-sio 2 /LPCVD-Si 3 N 4 /sputtered-au, all of thickness being 500 nm (Fig. 1). As shown in Fig. 2, analytical models suggest the beam has an expected maximumdeflection at a significantly higher temperature. 978-1-4673-0325-5/12/$31.00 2012 IEEE 496 MEMS 2012, Paris, FRANCE, 29 January - 2 February 2012

Figure 1: The multimorphs operate similarly to previous devices, with a static capacitance pad and a temperaturesensitive multimorph. The capacitance is changed between the metal on the beam and the low-resistivity silicon substrate. Figure 3: Fabrication process: A thermal oxide is grown (a) along with an LPCVD nitride layer (b). The nitride is patterned with an RIE tool and the oxide is etched with BOE (c). A Ti adhesion layer and Au are deposited and patterned (d). A thicker Au layer is deposited on the opposite side of the wafer for packaging (e). Figure 2: Analytical bending of the proposed thermal- SiO 2 /LPCVD-Si 3 N 4 /sputtered-au (500nm/500nm/500nm) multimorph cantilever. The expected maximum deflection occurs at a much higher temperature. FABRICATION MEMS Bimorphs The fabrication process includes some steps from lower temperature devices detailed in [7]. First, a thermal oxide is grown on a silicon wafer (Figure 3(a)). Then, a low-stress LPCVD nitride film is grown on top of the oxide (Figure 3(b)). The two films are then patterned together with traditional lithography (Figure 3(c)). First, the nitride is patterned with a dry etch in an RIE tool. The oxide beneath it is then removed with a wet etch. Next, a thin (30 nm) Ti adhesion layer and 500 nm Au film are deposited and patterned with a wet-etch (Figure 3(d)). Finally, a thicker gold film (1 μm) is deposited on the back side of the wafer for Au-Au bonding used in packaging (Figure 3(e)). Figure 4: Post-anneal SEM image of a fabricated array of multimorph beams, each 250 µm x 10 µm. Packaging The devices are attached to the header with a goldgold thermo-compression bond (Fig. 5). The pick-andplace tool used applies approximately 10 MPa of pressure on the 2 x 2 mm 2 chip. The bond is performed at 330 C for 15 minutes. Next, the pad is wirebonded to the TO package lead. The beams are then released with a XeF 2 dry etch of the silicon, and the can is resistively-welded to the header, hermetically-sealing the device in the cleanroom environment. 497

temperature are far beyond what can be found in commercial devices (Fig. 7). Figure 5: The sensors are packaged using Au-Au thermocompression bonding to a commercial transistor outline (TO) package, and resistively-welding a cap. PERFORMANCE Capacitance and Quality Factor The sensors are measured by attaching wires to the leads and placing them in a laboratory oven, along with an external thermocouple connected to a thermocouple reader. A capacitance meter and the thermocouple reader are connected via GPIB to a laptop, and the data collection occurs automatically. Due to inability to use solder or epoxy at these temperatures, the wires are wrapped around the leads and attached with Aremco 597- A, an electrically and thermally-conducting silver-based paste [8]. The oven temperature is then increased to the desired set-point. The mean initial capacitance of the sensors is 6.441 pf; with a standard deviation of 0.197 pf. Figure 7: Room temperature quality factor and operating temperature of this work compared to existing technologies. Reliability Presented in this section are laser confocal microscope profiles from the thermal-annealing process, detailing the break-in period, after which no additional creep is observed, even after over 24 hours at 650 C. Annealing is required to allow the stress in the beams to reach a stable point. After this point, the beam deflections are extremely-consistent, and exhibited no additional creep or hysteresis. Fig. 8 shows the room-temperature beam profiles versus amount of time kept at 650 C. First, an 8 hour anneal relaxes the film stress. An additional 24 hour creep measurement is performed to show that no additional creep is observed after this point. Figure 6: Capacitance versus temperature for five separate, packaged devices, as well as the capacitance versus temperature an empty hermetic package. The parasitic-capacitance of the package actually changes in our favor. The frequency versus temperature of an LCresonator is extracted from the capacitance trend-line. Although the change is small at low temperatures, it is still mostly over 1 khz/ C, which is sufficient for receivers to obtain acceptable accuracy As shown in Fig. 4, the robust fabrication process and packaging yield consistent capacitance-temperature profiles from device-to-device. Similarly, the devices exhibit a consistently-high measured quality factor of 1,727 with a standard deviation of 54 for 5 packaged devices. This quality factor and maximum operating 498

(a) (b) Figure 8: (a) Room-temperature beam profiles of the samples after certain amounts of time kept at 650 C and (b), extracted beam heights versus time. The devices are annealed for 8 hours, after which they exhibit no further creep, even after 24 hours at 650 C. REFERENCES [1] R. Draney, "High temperature sensor for bearing health monitoring", in 2008 IEEE Aerospace Conference, Big Sky, MT, March 1-8, 2008. [2] N. Riza, M. Sheikh, and F. Perez, "Design and Fabrication of an Extreme Temperature Sensing Optical Probe using Silicon Carbide Technologies", in IEEE Sensors, pp. 600-602, 2007. [3] J. Casady, W. Dillard, R. Johnson, and U. Rao, "A Hybrid 6H-SiC Temperature Sensor Operational from 25 C to 500 C", in IEEE Transactions on Components, Packaging, and Manufacturing Technology - Part A, vol. 19, pp. 416-422, Sep. 1996. [4] S. Scott, J.I. Kim, F. Sadeghi, and D. Peroulis, An Analytical Capacitance Model of Temperature- Sensitive, Large-Displacement Multimorph Cantilevers: Numerical and Experimental Validation, accepted for publication in the IEEE/ASME JMEMS, Sept. 2011. [5] A. Ned, R. Okojie, and A. Kurtz, "6H-SiC Pressure Sensor Operation at 600 C", in High Temperature Electronics Conference, pp. 257-260, 1998. [6] S. Scott, F. Sadeghi and D. Peroulis, "An inherentlyrobust 300 degrees C MEMS temperature sensor for wireless health monitoring of ball and rolling element bearings", in IEEE Sensors, pp 929-932, 2009. [7] S. Scott, A. Kovacs, L. Gupta, J. Katz, F. Sadeghi and D. Peroulis, "Wireless temperature microsensors integrated on bearings for health monitoring applications", in IEEE MEMS, pp. 660-663, 2011. [8] Aremco Pyroduct 597-A, Aremco Products Inc., Valley Cottage, NY. [9] Murata Manufacturing Company, Ltd., Kyoto, Japan [10] Johanson Dielectrics, Sylmar, CA [11] Wright Capacitors, Santa Ana, CA [12] HT-300 and HT-460, TRS Technologies, State College, PA CONTACT *D. Peroulis, tel: +1-765-4943491; dperouli@purdue.edu Conclusion This chapter presented the design and fabrication of a new packaged capacitive temperature sensor for engine component health-monitoring applications and measurement results above 600 C. The thermal- SiO 2 /LPCVD-Si 3 N 4 /sputtered-au multimorph sensors robust fabrication process and packaging yield consistent capacitance-temperature profiles from device-to-device, and a high quality factor. Reliability of the devices was also studied, including the thermal-annealing process, after which no additional creep is observed, even after over 24 hours at 650 C. All of this gives way to a first-ofits-kind sensor with unparalleled performance for harshenvironment wireless temperature sensing. 499