2012
DOI: 10.1039/c2cp40371d
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Selection and characterization of aerosol particle size using a bessel beam optical trap for single particle analysis

Abstract: Bessel beams were used to create a counter-propagating optical trap for capturing and manipulating aerosol particles. Aerosol droplets were characterized through measurement of the elastic scattered light at three wavelengths; the trapping wavelength of 532 nm was used in conjunction with two probe beams at 405 nm and 633 nm to reduce the uncertainty in estimating droplet radii of 1 μm or less. Control of the aerosol size distribution sampled by the counter-propagating trap was demonstrated by varying the trap… Show more

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Cited by 51 publications
(49 citation statements)
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“…The particle radius was obtained from the analysis of interference fringes for light scattered from the trapping laser and collected over a known angular range (the phase function). [11][12][13] In the analysis described in section 5, the beam waist of the TEM00 mode was obtained as 279 m, which compares well to the value expected for our design of linear optical cavity of 272 m. 9 Experimental measurements are overlaid by Mie scattering calculations in (2) to account for the measurement of extinction by light scattering within an optical cavity.…”
Section: Extinction Cross Section Determination In An Optical Cavitymentioning
confidence: 55%
“…The particle radius was obtained from the analysis of interference fringes for light scattered from the trapping laser and collected over a known angular range (the phase function). [11][12][13] In the analysis described in section 5, the beam waist of the TEM00 mode was obtained as 279 m, which compares well to the value expected for our design of linear optical cavity of 272 m. 9 Experimental measurements are overlaid by Mie scattering calculations in (2) to account for the measurement of extinction by light scattering within an optical cavity.…”
Section: Extinction Cross Section Determination In An Optical Cavitymentioning
confidence: 55%
“…1 in Cotterell et al (2015a) and Fig. 4 in Carruthers et al (2012) for examples of raw PF images recorded using our instrumentation. As described previously (Cotterell et al, 2015a, b), a mean Pearson correlation coefficient c (n λ ) is used to quantify the level of agreement between the measured PF data set and the set of best-fit Mie theory simulations, with c (n λ ) = 1 corresponding to perfect agreement and lower values of c (n λ ) indicative of a poorer fit.…”
Section: Radius and Refractive Index Retrieval From Recorded Phase Fumentioning
confidence: 99%
“…[18][19][20][21][22] In the field of aerosol science, Bessel beams are very appealing for the study of single aerosol particles and instrumentation 2 incorporating such beams has been recently demonstrated. [23][24][25][26][27][28][29] However, there remains the need for an approach to accurately characterize a particle once it has been trapped in such a beam. For a homogeneous spherical particle the radius and refractive index must be accurately determined.…”
Section: 9mentioning
confidence: 99%