2020
DOI: 10.1039/c9nr10351a
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Three dimensional spatiotemporal nano-scale position retrieval of the confined diffusion of nano-objects inside optofluidic microstructured fibers

Abstract: Fiber-based 3D tracking of nano-scale objects with high spatiotemporal resolution is demonstrated for exploring dynamics at the nanoscale levels.

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Cited by 23 publications
(18 citation statements)
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“…The choice of nanosphere diameter represents a compromise between the intensity decay across the water-filled microchannel, the in-fiber power, the scattering cross section and the frame rate, allowing the nanosphere to be tracked along the transverse direction at any time. The particle diameter considered here is larger compared to our previous work [13], imposed by a smaller scattering coefficient and a faster field decay, both of which result from the smaller RI of water compared to the liquid used in our previous work.…”
Section: Methodsmentioning
confidence: 82%
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“…The choice of nanosphere diameter represents a compromise between the intensity decay across the water-filled microchannel, the in-fiber power, the scattering cross section and the frame rate, allowing the nanosphere to be tracked along the transverse direction at any time. The particle diameter considered here is larger compared to our previous work [13], imposed by a smaller scattering coefficient and a faster field decay, both of which result from the smaller RI of water compared to the liquid used in our previous work.…”
Section: Methodsmentioning
confidence: 82%
“…In order to decode the axial position from the scattered intensity, an bijective function between the local intensity distribution of the evanescent field and the y-coordinate (I = f(y), y = f −1 (I)), (f −1 is the reverse of f) is required, i.e., the y-position can be uniquely determined from one certain intensity. In contrast to the water-DMSO mixture used in our previous work (RI n r = 1.44 at a wavelength of λ = 640 nm) [13], in which the field intensity can be described by a uniform exponential function within the whole channel, the intensity distribution (simulated by finite-element modeling using COMSOL) of the evanescent field inside the microchannel in case of pure water filling is substantially more complex regarding the following three aspects: (i) First, using water leads to a distinct variation of the intensity inside the microchannel not only along the y-axis but also along the x-direction in contrast to our previous work using DMSO/ water. Consequently, the mathematical function that relates y-position and intensity must be determined separately for each x-position.…”
Section: Concept and Working Principlementioning
confidence: 78%
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