2011
DOI: 10.1088/1752-7155/5/3/037106
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Breath analysis system based on phase-shifting interferometric microscopy readout of microcantilever arrays

Abstract: Microcantilever (MC) sensors can provide ultrasensitive bio-chemical detection. Monitoring the bending response of large arrays of MC sensors coated with a library of receptors will produce a characteristic 'breath-print' corresponding to the breath composition; this promises to be suitable for non-invasive medical diagnostics. While MC arrays with hundreds of individual sensors can be produced readily, conventional MC readout methods are not suitable for the parallel readout of tens or hundreds of individual … Show more

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Cited by 4 publications
(5 citation statements)
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“…The compressive stress, together with the added mass, also gives rise to a change of the resonance frequency. This dynamic-mode response is shown in figure 1 , within the typical range for resonant gas sensors [1,6,7]. We find a different rate for the static-and dynamic-mode response, with…”
Section: Static and Dynamic Gas Sensing In The Linear Regimesupporting
confidence: 61%
See 1 more Smart Citation
“…The compressive stress, together with the added mass, also gives rise to a change of the resonance frequency. This dynamic-mode response is shown in figure 1 , within the typical range for resonant gas sensors [1,6,7]. We find a different rate for the static-and dynamic-mode response, with…”
Section: Static and Dynamic Gas Sensing In The Linear Regimesupporting
confidence: 61%
“…Sensitive techniques are available to detect these changes, which often involve a measurement of the cantilever's resonance frequency. Cantilever sensors are deployed in a variety of applications including environmental monitoring, exhaled breath analysis, point-of-care diagnostics, and biosensing, several of which have been commercialized [1][2][3][4][5][6][7][8][9][10][11].…”
Section: Introductionmentioning
confidence: 99%
“…(b) The cantilever deflections were plotted versus their length squared in order to find the slope of the linear fit ( ). This slope (--) was then used to calculate the surface stress using (10). The two points labeled 'stictioned' were excluded from the fit, as their extreme deflections indicated the beams were stictioned.…”
Section: Resonance Frequenciesmentioning
confidence: 99%
“…The remaining data were fit using linear regression. The slope of the fit was used to calculate σ s using (10). The result was σ s = 1.34±0.09 N m −1 .…”
Section: Resonance Frequenciesmentioning
confidence: 99%
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