Abstract:Measurements of the gauge factor of suspended, top-down silicon nanowires are presented. The nanowires are fabricated with a CMOS compatible process and with doping concentrations ranging from 2 × 10(20) down to 5 × 10(17) cm(-3). The extracted gauge factors are compared with results on identical non-suspended nanowires and with state-of-the-art results. An increase of the gauge factor after suspension is demonstrated. For the low doped nanowires a value of 235 is measured. Particular attention was paid throug… Show more
“…From equations (12) and (13) and the estimations made for the deflection at rest and first-mode vibration amplitude (a 1 E1 nm, d 0 ¼ 5-50 nm), we infer gauge factor values in the range from a few units to a few hundreds. This is the range expected from a conventional piezoresistive effect in SiNWs depending on the doping level 24 . Therefore, high-sensitivity piezoresistive transduction, enhanced by an asymmetric beam profile at rest, does not require extraordinarily large piezoresistive coefficients as those reported on high-resistivity bottom-up NWs, which reach up to 1,000 and above 21 .…”
Section: Discussionmentioning
confidence: 73%
“…Therefore, high-sensitivity piezoresistive transduction, enhanced by an asymmetric beam profile at rest, does not require extraordinarily large piezoresistive coefficients as those reported on high-resistivity bottom-up NWs, which reach up to 1,000 and above 21 . Nevertheless, larger gauge factors are still expected for bottom-up NWs as compared with their top-down counterparts according to the literature 23,24 . In fact, a larger gauge factor for bottom-up SiNWs explains why the quadratic component of the resistance variation with vibration is only detected for these devices (Fig.…”
Section: Discussionmentioning
confidence: 98%
“…The so-called giant piezoresistance effect has indeed been explored for electrical read-out of highfrequency SiNW resonators 2 . Several studies in top-down SiNWs have not been able to find giant values of piezoresistance coefficients 23,24 .…”
Highly sensitive conversion of motion into readable electrical signals is a crucial and challenging issue for nanomechanical resonators. Efficient transduction is particularly difficult to realize in devices of low dimensionality, such as beam resonators based on carbon nanotubes or silicon nanowires, where mechanical vibrations combine very high frequencies with miniscule amplitudes. Here we describe an enhanced piezoresistive transduction mechanism based on the asymmetry of the beam shape at rest. We show that this mechanism enables highly sensitive linear detection of the vibration of low-resistivity silicon beams without the need of exceptionally large piezoresistive coefficients. The general application of this effect is demonstrated by detecting multiple-order modes of silicon nanowire resonators made by either top-down or bottom-up fabrication methods. These results reveal a promising approach for practical applications of the simplest mechanical resonators, facilitating its manufacturability by very large-scale integration technologies.
“…From equations (12) and (13) and the estimations made for the deflection at rest and first-mode vibration amplitude (a 1 E1 nm, d 0 ¼ 5-50 nm), we infer gauge factor values in the range from a few units to a few hundreds. This is the range expected from a conventional piezoresistive effect in SiNWs depending on the doping level 24 . Therefore, high-sensitivity piezoresistive transduction, enhanced by an asymmetric beam profile at rest, does not require extraordinarily large piezoresistive coefficients as those reported on high-resistivity bottom-up NWs, which reach up to 1,000 and above 21 .…”
Section: Discussionmentioning
confidence: 73%
“…Therefore, high-sensitivity piezoresistive transduction, enhanced by an asymmetric beam profile at rest, does not require extraordinarily large piezoresistive coefficients as those reported on high-resistivity bottom-up NWs, which reach up to 1,000 and above 21 . Nevertheless, larger gauge factors are still expected for bottom-up NWs as compared with their top-down counterparts according to the literature 23,24 . In fact, a larger gauge factor for bottom-up SiNWs explains why the quadratic component of the resistance variation with vibration is only detected for these devices (Fig.…”
Section: Discussionmentioning
confidence: 98%
“…The so-called giant piezoresistance effect has indeed been explored for electrical read-out of highfrequency SiNW resonators 2 . Several studies in top-down SiNWs have not been able to find giant values of piezoresistance coefficients 23,24 .…”
Highly sensitive conversion of motion into readable electrical signals is a crucial and challenging issue for nanomechanical resonators. Efficient transduction is particularly difficult to realize in devices of low dimensionality, such as beam resonators based on carbon nanotubes or silicon nanowires, where mechanical vibrations combine very high frequencies with miniscule amplitudes. Here we describe an enhanced piezoresistive transduction mechanism based on the asymmetry of the beam shape at rest. We show that this mechanism enables highly sensitive linear detection of the vibration of low-resistivity silicon beams without the need of exceptionally large piezoresistive coefficients. The general application of this effect is demonstrated by detecting multiple-order modes of silicon nanowire resonators made by either top-down or bottom-up fabrication methods. These results reveal a promising approach for practical applications of the simplest mechanical resonators, facilitating its manufacturability by very large-scale integration technologies.
“…8 A lot of excitement was produced by the report of giant piezoresistivity in silicon nanowires, 9,10 with the latest room temperature value reported being G = 280. 11 The earliest work hinting at a higher piezoresistive effect in n-type SiGe alloys of high Ge compositions was performed by R. W. Keyes in 1957. 12 He found a piezoresistive effect 15% larger than in pure Ge at a Ge composition of x = 0.96.…”
Type of publicationArticle (peer-reviewed) We use first-principles electronic structure methods to show that the piezoresistive strain gauge factor of single-crystalline bulk n-type silicon-germanium alloys at carefully controlled composition can reach values of G = 500, three times larger than that of silicon, the most sensitive such material used in industry today. At cryogenic temperatures of 4 K we find gauge factors of G = 135 000, 13 times larger than that observed in Si whiskers. The improved piezoresistance is achieved by tuning the scattering of carriers between different ( and L) conduction band valleys by controlling the alloy composition and strain configuration.
“…A number of publications have shown the enhanced sensitivity of silicon piezoresistors [12]- [14]. Overall, the piezoresistance coefficient has been found to increase with decreasing nanowire doping and cross-sectional area.…”
Abstract-This paper reports on the enhanced piezoresistive effect in p-type <110> silicon nanowires, fabricated using a top down approach. The silicon nanowire width is varied from 100 to 500nm with thickness of 200 nm and length of 9µm. It is found that the piezoresistive effect increases when the nanowire width is reduced below 350 nm. Compared with micrometre sized piezoresistors, silicon nanowires have produced up to 50% enhancement. Silicon nanowire with cross-section of (100 × 200 nm) with doping concentration of 3.2 × 10 18 cm -3 has produced a gauge factor of 150. The extracted gauge factors are compared with other silicon nanowire experimental publications. The enhancement in piezoresistive effect by employing non-suspended silicon nanowire is beneficial for new MEMS pressure sensors with medium doping concentrations.
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