Abstract:An infrared (IR) thermal detector, which used the torsional oscillation of a micromechanical resonator, was developed to achieve a high sensitivity. The detector has a bimaterial structure consisting of a tense Si film (oscillating body) and a metal film (IR absorber). Owing to the difference in thermal expansion between the two materials, the resonator is bent by light incidence. Because the axis of torsion is bent from the initial flat state, the spring for torsional oscillation hardens and resonant frequenc… Show more
“…The best TCF is ~8% K −1 at an operation temperature of T sub = 45 °C. This TCF is 2 orders of magnitude higher than the best TCF reported so far (~0.1% K −1 ) for IR resonant sensors 25 . In addition, the TCF is more than an order of magnitude higher than resonant temperature sensors 45–47 , for which the best reported TCF is 1.7% K −1 .…”
Section: Resultsmentioning
confidence: 56%
“…The TCF were calculated according to the normalized frequency change within each 5 °C step using the measurements from Figure 2.a. The best TCF is around 8% at the operation temperature of Tsub=45 °C; which is 2 order of magnitude higher than the best TCF reported so far for IR resonant sensors 25 . Since there is a tradeoff between the TCF and Q, the operation temperature of Tsub=45 °C has very high AD value for the integration time τ=500 ms as it is illustrated in Figure 3.b.…”
Section: Smp Resonator Characterizationmentioning
confidence: 65%
“…) consists of the two key parameters that are specific for resonant IR sensors. High sensitivity can be achieved by increasing the TCF 25,26 and/or improving the frequency stability [27][28][29] .…”
Uncooled infrared detectors have enabled the rapid growth of thermal imaging applications. These detectors are predominantly bolometers, reading out a pixel’s temperature change due to infrared radiation as a resistance change. Another uncooled sensing method is to transduce the infrared radiation into the frequency shift of a mechanical resonator. We present here highly sensitive resonant infrared sensors, based on thermo-responsive shape memory polymers. By exploiting the phase-change polymer as transduction mechanism, our approach provides 2 orders of magnitude improvement of the temperature coefficient of frequency. Noise equivalent temperature difference of 22 mK in vacuum and 112 mK in air are obtained using f/2 optics. The noise equivalent temperature difference is further improved to 6 mK in vacuum by using high-Q silicon nitride membranes as substrates for the shape memory polymers. This high performance in air eliminates the need for vacuum packaging, paving a path towards flexible non-hermetically sealed infrared sensors.
“…The best TCF is ~8% K −1 at an operation temperature of T sub = 45 °C. This TCF is 2 orders of magnitude higher than the best TCF reported so far (~0.1% K −1 ) for IR resonant sensors 25 . In addition, the TCF is more than an order of magnitude higher than resonant temperature sensors 45–47 , for which the best reported TCF is 1.7% K −1 .…”
Section: Resultsmentioning
confidence: 56%
“…The TCF were calculated according to the normalized frequency change within each 5 °C step using the measurements from Figure 2.a. The best TCF is around 8% at the operation temperature of Tsub=45 °C; which is 2 order of magnitude higher than the best TCF reported so far for IR resonant sensors 25 . Since there is a tradeoff between the TCF and Q, the operation temperature of Tsub=45 °C has very high AD value for the integration time τ=500 ms as it is illustrated in Figure 3.b.…”
Section: Smp Resonator Characterizationmentioning
confidence: 65%
“…) consists of the two key parameters that are specific for resonant IR sensors. High sensitivity can be achieved by increasing the TCF 25,26 and/or improving the frequency stability [27][28][29] .…”
Uncooled infrared detectors have enabled the rapid growth of thermal imaging applications. These detectors are predominantly bolometers, reading out a pixel’s temperature change due to infrared radiation as a resistance change. Another uncooled sensing method is to transduce the infrared radiation into the frequency shift of a mechanical resonator. We present here highly sensitive resonant infrared sensors, based on thermo-responsive shape memory polymers. By exploiting the phase-change polymer as transduction mechanism, our approach provides 2 orders of magnitude improvement of the temperature coefficient of frequency. Noise equivalent temperature difference of 22 mK in vacuum and 112 mK in air are obtained using f/2 optics. The noise equivalent temperature difference is further improved to 6 mK in vacuum by using high-Q silicon nitride membranes as substrates for the shape memory polymers. This high performance in air eliminates the need for vacuum packaging, paving a path towards flexible non-hermetically sealed infrared sensors.
“…A number of groups have demonstrated that MEMS/NEMS resonators can work as fast and highly sensitive THz/IR detectors. Depending on the vibrational mode and geometrical shape, they can be categorized as torsional mode [72][73][74][75][76], bending mode [59,77], or membranous shape [57,78,79]. Table 1 provides a survey of the performance of THz/IR detectors based on MEMS/NEMS resonators, allowing for an objective comparison of existing MEMS bolometers.…”
Section: Thz/ir Detection Based On Mems/nems Resonatorsmentioning
The doubly clamped microelectromechanical system (MEMS) beam resonators exhibit extremely high sensitivity to tiny changes in the resonance frequency owing to their high quality (Q-) factors, even at room temperature. Such a sensitive frequency-shift scheme is very attractive for fast and highly sensitive terahertz (THz) detection. The MEMS resonator absorbs THz radiation and induces a temperature rise, leading to a shift in its resonance frequency. This frequency shift is proportional to the amount of THz radiation absorbed by the resonator and can be detected and quantified, thereby allowing the THz radiation to be measured. In this review, we present an overview of the THz bolometer based on the doubly clamped MEMS beam resonators in the aspects of working principle, readout, detection speed, sensitivity, and attempts at improving the performance. This allows one to have a comprehensive view of such a novel THz detector.
“…Their use as micromirrors has led to the rapid advances in digital light processing [1]; they have been shown to act as thermal infrared detectors [2,3] and also as resonant mass sensing devices [4,5]. A resonant micropaddle is one such resonant torsional system and has been considered as a potential bio/chemical sensor platform [6,7].…”
The reference cantilever method is shown to act as a direct and simple method for determination of torsional spring constant. It has been applied to the characterization of micropaddle structures similar to those proposed for resonant functionalized chemical sensors and resonant thermal detectors. It is shown that this method can be used as an effective procedure to characterize a key parameter of these devices and would be applicable to characterization of other similar MEMS/NEMS devices such as micromirrors. In this study, two sets of micropaddles are manufactured (beams at centre and offset by 2.5 μm) by using LPCVD silicon nitride as a substrate. The patterning is made by direct milling using focused ion beam. The torsional spring constant is achieved through micromechanical analysis via atomic force microscopy. To obtain the gradient of force curve, the area of the micropaddle is scanned and the behaviour of each pixel is investigated through an automated developed code. The experimental results are in a good agreement with theoretical results.
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