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000875113 1001_ $$0P:(DE-Juel1)178787$$aRivera Moran, Jose Alejandro$$b0$$eFirst author
000875113 1112_ $$aZsigmondy Kolloquium 2020$$cDuesseldorf$$d2020-03-09 - 2020-03-11$$wGermany
000875113 245__ $$aNear interface diffusion of various kinds of colloidal particles
000875113 260__ $$c2020
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000875113 500__ $$a[1] P. Holmqvist , J. K. G. Dhont , P. R. Lang, J. Chem. Phys. 2007, 126, 044707 1-8.[2] P. Holmqvist , J. K. G. Dhont , P. R. Lang, Phys. Rev. E 2006, 74, 0214002 1-5.[3] M. Lisicki et al. al., Soft Matter 2014, 10, 4312-4323.[4] V . N . Michailidou et. al , Phys. Rev. Lett. 2009, 102, 068302.[5] Y. Liu et al. Soft Matter, 2015, 11, 7316.[6] A. J. Goldman, R. G. Cox and H. Brenner, Chem. Eng. Sci., 1967, 22, 637-651.[7] M. Lisicki et al. J. Chem. Phys. 2007, 136, 204704.[8] C. P. Hsu et al. PNAS 2018, 115 , No. 20, 5117-5122.[9] D. A. Woods and C. B. Dain, Soft Matter, 2014, 10 , 1071.[10] S. Bhattacharjee, C. H. Ko, M Elimelech, Langmuir , 1998, 14 , 3365-3375.
000875113 520__ $$aWhen suspended colloidal particles move in the ultimate vicinity of a flat solid interface, their mobility is smaller than in the bulk suspension due to a drag force caused by hydrodynamic interaction between the particle and the wall. Further, the friction acting on a particle depends on the direction of motion. Leading to different diffusion coefficients parallel, 
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000875113 7001_ $$0P:(DE-Juel1)159482$$aLiu, Yi$$b1
000875113 7001_ $$0P:(DE-HGF)0$$aHsu, Chiao-Peng$$b2$$eCollaboration author
000875113 7001_ $$0P:(DE-HGF)0$$aLucio, Isa$$b3
000875113 7001_ $$0P:(DE-Juel1)130789$$aLang, Peter R.$$b4
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