1995
DOI: 10.1103/physreve.52.6289
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Thermal fluctuations of the shapes of droplets in dense and compressed emulsions

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Cited by 54 publications
(36 citation statements)
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“…In other words, for the multiplication rule (16) to hold the optical thickness of e.g. the first layer should be much greater than that of the second one, while g (1) 1 (L 2 , τ ) ≃ 1 for the latter.…”
Section: Multiplication Rulementioning
confidence: 99%
See 1 more Smart Citation
“…In other words, for the multiplication rule (16) to hold the optical thickness of e.g. the first layer should be much greater than that of the second one, while g (1) 1 (L 2 , τ ) ≃ 1 for the latter.…”
Section: Multiplication Rulementioning
confidence: 99%
“…colloidal suspensions [1][2][3][4][5][6]10], particle gels and ceramic green bodies [11][12][13][14][15], emulsions [16][17][18], foams [19][20][21][22][23], granular [24,25], and biological [26][27][28] media. It has been demonstrated that DWS can be used to image macroscopic static and dynamic heterogeneities in turbid media [29][30][31][32][33][34][35].…”
Section: Introductionmentioning
confidence: 99%
“…2. Given the large size of the droplets we predominantly probe selfmotion and shape fluctuations [22,[28][29][30] while the contribution of collective motion to the dynamic multiple light scattering signal can be neglected. We can then express the measured and normalized intensity-intensity correlation function g 2 (t) as follows [28,30,31]:…”
Section: Methodsmentioning
confidence: 99%
“…curves tend toward zero for short times while for the liquid droplets we detect an upturn at short times. The former is a signature of droplet and fluid inertia [33] while the latter is characteristic for additional thermal fluctuations of the liquid droplet interface [22,29].…”
Section: Thermal Motion Probed By Dwsmentioning
confidence: 99%
“…The single-quantum optomechanical coupling can be found from the optical WGM detuning produced by the surface We note that in order to obtain this result, care needs to be taken to preserve the volume of the drop by adjusting the radius (i.e., the l = 0 monopole contribution to δR) [43]. Focusing on the l = 2,m = 0 mode, we then equate the average potential energy 2σ X 2 0 to half of the zero-point energyhω vib /4.…”
Section: B Optomechanical Coupling To Surface Modesmentioning
confidence: 99%