2018
DOI: 10.1038/s41598-018-34381-z
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Measurement of wavelength-dependent radiation pressure from photon reflection and absorption due to thin film interference

Abstract: Opto-mechanical forces result from the momentum transfer that occurs during light-matter interactions. One of the most common examples of this phenomenon is the radiation pressure that is exerted on a reflective surface upon photon reflection. For an ideal mirror, the radiation pressure is independent of the wavelength of light and depends only on the incident power. Here we consider a different regime where, for a constant input optical power, wavelength-dependent radiation pressure is observed due to coheren… Show more

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Cited by 10 publications
(12 citation statements)
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“…It can be noted that, in the presence of photothermal effects, this response function would be modified from the ideal harmonic oscillator form as described, e.g., in Refs. 30,31 . Thus, the ideal harmonic oscillator form of the frequency response function in Fig.…”
Section: Resultsmentioning
confidence: 99%
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“…It can be noted that, in the presence of photothermal effects, this response function would be modified from the ideal harmonic oscillator form as described, e.g., in Refs. 30,31 . Thus, the ideal harmonic oscillator form of the frequency response function in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…However, optical forces in those nanomicromechanical systems have been directly accompanied by photothermal effects due to short thermal time constants of the miniaturized resonators 6,7,[26][27][28][29] , which has required further sophisticated techniques to discern them from the radiation pressure effects. Therefore, various optical, mechanical, and thermal techniques have been developed to overcome the trade-off between the radiation pressure and the photothermal effects, such as complex resonator designs consisting of highly reflective multilayer coatings deposited on the cantilever to further increase the reflectivity 7,12 , attachment of an additional mass to increase the thermal time constant of the cantilever 13 , or other ways to separate the optical force from the photothermal effects 30,31 .…”
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confidence: 99%
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“…The exciting laser beam is focused down to 5 µm on the AFM tip, which is roughly half the base of the pyramidal tip. A tip-less geometry without electric fields or photovoltage effects was used in [30]. The EOM modulation was a sinusoidal shape, periodically changing the laser power from 0 to P , which can be up to P max = 40 mW.…”
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confidence: 99%