Energy landscape of colloidal dumbbells in a periodic distribution of light
Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. As shown previously [E. Sarmiento-Gomez, J. A. Rivera-Moran and J. L. Aruaz-Lara, Soft Matter , 2018, 14 , 3684], planar aggrega...
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| Published in | Soft matter Vol. 15; no. 17; pp. 3573 - 3579 |
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| Main Authors | , , |
| Format | Journal Article |
| Language | English |
| Published |
England
Royal Society of Chemistry
24.04.2019
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| Abstract | Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. As shown previously [E. Sarmiento-Gomez, J. A. Rivera-Moran and J. L. Aruaz-Lara,
Soft Matter
, 2018,
14
, 3684], planar aggregates of spherical particles adopt discrete configurations in such light distribution. Here we focus on the case of colloidal dumbbells both symmetric and asymmetric from an experimental and theoretical point of view. It has been shown that the direct calculation using the ray tracing approximation is in excellent agreement with the experiment in spite of the fact that the particles size and the wavelength of the trapping light are comparable. We also corroborate, at least for the more simple case of a single particle in a parabolic light distribution, that the simple method used here provides the same results as the more complex and general Lorenz-Mie approach giving a more simple yet reliable method for the calculation of the energy landscape of colloidal aggregates in periodic light distributions.
Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. |
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| AbstractList | Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. As shown previously [E. Sarmiento-Gomez, J. A. Rivera-Moran and J. L. Aruaz-Lara, Soft Matter, 2018, 14, 3684], planar aggregates of spherical particles adopt discrete configurations in such light distribution. Here we focus on the case of colloidal dumbbells both symmetric and asymmetric from an experimental and theoretical point of view. It has been shown that the direct calculation using the ray tracing approximation is in excellent agreement with the experiment in spite of the fact that the particles size and the wavelength of the trapping light are comparable. We also corroborate, at least for the more simple case of a single particle in a parabolic light distribution, that the simple method used here provides the same results as the more complex and general Lorenz–Mie approach giving a more simple yet reliable method for the calculation of the energy landscape of colloidal aggregates in periodic light distributions. Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. As shown previously [E. Sarmiento-Gomez, J. A. Rivera-Moran and J. L. Aruaz-Lara, Soft Matter , 2018, 14 , 3684], planar aggregates of spherical particles adopt discrete configurations in such light distribution. Here we focus on the case of colloidal dumbbells both symmetric and asymmetric from an experimental and theoretical point of view. It has been shown that the direct calculation using the ray tracing approximation is in excellent agreement with the experiment in spite of the fact that the particles size and the wavelength of the trapping light are comparable. We also corroborate, at least for the more simple case of a single particle in a parabolic light distribution, that the simple method used here provides the same results as the more complex and general Lorenz-Mie approach giving a more simple yet reliable method for the calculation of the energy landscape of colloidal aggregates in periodic light distributions. Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. Using a ray tracing calculation, the energy landscape of dumbbells, made of spherical colloidal particles, interacting with a periodic distribution of light is calculated. As shown previously [E. Sarmiento-Gomez, J. A. Rivera-Moran and J. L. Aruaz-Lara, Soft Matter , 2018, 14 , 3684], planar aggregates of spherical particles adopt discrete configurations in such light distribution. Here we focus on the case of colloidal dumbbells both symmetric and asymmetric from an experimental and theoretical point of view. It has been shown that the direct calculation using the ray tracing approximation is in excellent agreement with the experiment in spite of the fact that the particles size and the wavelength of the trapping light are comparable. We also corroborate, at least for the more simple case of a single particle in a parabolic light distribution, that the simple method used here provides the same results as the more complex and general Lorenz–Mie approach giving a more simple yet reliable method for the calculation of the energy landscape of colloidal aggregates in periodic light distributions. |
| Author | Rivera-Morán, J. A Sarmiento-Gómez, E Arauz-Lara, J. L |
| AuthorAffiliation | Universidad Autónoma de San Luis Potosí Instituto de Física "Manuel Sandoval Vallarta" |
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| Cites_doi | 10.1038/ncomms8187 10.1103/PhysRevE.76.061503 10.1103/PhysRevLett.99.197802 10.1080/00107510110116051 10.1016/0030-4018(91)90159-B 10.1103/PhysRevE.88.022125 10.1038/nature01935 10.1103/PhysRevE.93.012608 10.1103/PhysRevE.67.050403 10.1146/annurev.biochem.77.043007.090225 10.1016/j.cocis.2005.04.001 10.1103/PhysRevD.3.825 10.1103/PhysRevE.91.031002 10.1088/1361-6463/aae5d0 10.1039/C0SM01051K 10.1103/PhysRevLett.24.156 10.1126/science.1058591 10.1088/1464-4258/9/8/S12 10.1063/1.2183357 10.1039/c4sm00132j 10.1088/1464-4258/9/8/S16 10.1146/annurev.bb.23.060194.001335 10.1103/PhysRevE.79.041407 10.1016/S0006-3495(92)81860-X 10.1016/S0022-4073(02)00336-9 10.1364/JOSAB.21.001749 10.1103/PhysRevE.91.022313 10.1103/PhysRevE.65.041602 10.1364/JOSAB.9.001922 10.1364/BOE.3.001891 10.1063/1.1785844 10.1039/C8SM00326B |
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