Diffusion in Condensed Matter 2005
DOI: 10.1007/3-540-30970-5_16
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Diffusion in Colloidal and Polymeric Systems

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Cited by 6 publications
(9 citation statements)
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“…The form of eq suggests that G D ( t ) in that case can approximately be expressed as a correlation function for a particle of the same size but fluorescently labeled only in the center and illuminated by an effectively larger beam of the intensity profile defined in the reciprocal space by The effective beam profile is also assumed to be Gaussian to preserve the simple analytical form of the time correlation function (eq ). This can be achieved, for example, by fitting | B ( qa )| with a function ( A e –(1/2) kq 2 a 2 ), which allows the effective beam waist size in the x–y plane to be expressed as , In refs and a value of k = 0.22 was reported; however, it was obtained for fitted value of A ( A ≠ 1) and for fitting range reaching the first secondary maximum of | B ( qa )|. Combining eq with eq leads to where τ 0 is the correlation time of a particle of the same size but fluorescently labeled only in the center and τ c is the correlation time fitted to the measured correlation function using eq .…”
Section: Resultsmentioning
confidence: 99%
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“…The form of eq suggests that G D ( t ) in that case can approximately be expressed as a correlation function for a particle of the same size but fluorescently labeled only in the center and illuminated by an effectively larger beam of the intensity profile defined in the reciprocal space by The effective beam profile is also assumed to be Gaussian to preserve the simple analytical form of the time correlation function (eq ). This can be achieved, for example, by fitting | B ( qa )| with a function ( A e –(1/2) kq 2 a 2 ), which allows the effective beam waist size in the x–y plane to be expressed as , In refs and a value of k = 0.22 was reported; however, it was obtained for fitted value of A ( A ≠ 1) and for fitting range reaching the first secondary maximum of | B ( qa )|. Combining eq with eq leads to where τ 0 is the correlation time of a particle of the same size but fluorescently labeled only in the center and τ c is the correlation time fitted to the measured correlation function using eq .…”
Section: Resultsmentioning
confidence: 99%
“…The size of the effective confocal volume for a uniformly labeled spherical NP has been previously calculated, , and the approximate simple correction formula was proposed.…”
Section: Introductionmentioning
confidence: 99%
“…In the case of particles comparable in size to the size of the confocal volume, diffusion times measured by FCS are not proportional to the particle size. A proper correction was proposed in a former study [39]. The proposed model was successfully validated for the polymeric and silica particles, whose diameters were larger than 500 nm [36].…”
Section: H1mentioning
confidence: 95%
“…In the case where the size of the fluorescent particle becomes comparable to or larger than the focal spot dimensions, the size and shape of the particle, the dye distribution within the particle, and other modes of motion (except translation) have to be considered. For spherical particles with a spherically symmetric dye distribution the rotational modes do not contribute, and the normalized FCS CF can be numerically calculated as 14…”
Section: Methodsmentioning
confidence: 99%
“…In the case where the size of the fluorescent particle becomes comparable to or larger than the focal spot dimensions, the size and shape of the particle, the dye distribution within the particle, and other modes of motion (except translation) have to be considered. For spherical particles with a spherically symmetric dye distribution the rotational modes do not contribute, and the normalized FCS CF can be numerically calculated as where is the Fourier transform (FT) of the Gaussian beam intensity profile and B ( q ) is the FT of the function χ­( r ) describing the dye distribution within the colloidal particle: For a uniform dye distribution, | B ( q )| 2 is equal to the static form factor, well-known in all scattering techniques, however, with the restriction that it refers only to the labeled part of the particle. The fluorescent form factor of a sphere of radius a with homogeneous fluorescent core radius a c has the form while that of a thin spherical shell Hence, for a body-labeled particle eq and for a surface labeled particle eq should be used.…”
Section: Methodsmentioning
confidence: 99%