2006
DOI: 10.1103/physrevlett.96.238101
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Surface Plasmon Radiation Forces

Abstract: We report the first experimental observation of momentum transfer from a surface plasmon to a single dielectric sphere. Using a photonic force microscope, we measure the plasmon radiation forces on different polystyrene beads as a function of their distance from the metal surface. We show that the force magnitude at resonance is strongly enhanced compared to a nonresonant illumination. Measurements performed as a function of the probe particle size indicate that optical manipulation by plasmon fields has a str… Show more

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Cited by 270 publications
(215 citation statements)
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References 34 publications
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“…A special feature of the BS detection compared to the FS case is that the same lens is used both for trapping and for collecting the scattering light. In the literature, the use of the BS light for position and force detection is mentioned [26][27][28][29][30][31] but, contrary to the FS light detection, has not been discussed extensively.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…A special feature of the BS detection compared to the FS case is that the same lens is used both for trapping and for collecting the scattering light. In the literature, the use of the BS light for position and force detection is mentioned [26][27][28][29][30][31] but, contrary to the FS light detection, has not been discussed extensively.…”
Section: Introductionmentioning
confidence: 99%
“…This occurs, for example, in biophysical applications where one of the two faces of a sample holder needs to be coated with some specific material 26 or in plasmonics applications where a plasmon wave needs to be coupled to one of the faces of the holder. 28 Furthermore, the BS mode of operation makes it easier to combine the optical trap with other techniques such as atomic force microscopy, which requires access to one side of the holder. A special feature of the BS detection compared to the FS case is that the same lens is used both for trapping and for collecting the scattering light.…”
Section: Introductionmentioning
confidence: 99%
“…Figure 3a,c shows the schematic of the corresponding experiment using the total internal reflection at a glass prism. For this numerical experiment, we use parameters corresponding to real experiments manipulating particles with evanescent fields (for example see refs [57][58][59][60][61][62]. Namely, we consider radiation with the wavelength l ¼ 650 nm, a gold particle (e p ¼ À 12.2 þ 3i, m p ¼ 1) in water (e ¼ 1.77, m ¼ 1), and near-critical total internal reflection (the angle of incidence is y ¼ 51°¼ y c þ 1.5°) from the interface between heavy flint glass (e 1 ¼ 3.06, m 1 ¼ 1) and water.…”
Section: Article Nature Communications | Doi: 101038/ncomms4300mentioning
confidence: 99%
“…1), [6]. The relaxation time τ is also directly related to the "corner frequency" that is found in the frequency-response curve (power spectrum) commonly used for analyzing optical-tweezers experiments f c = (πτ ) −1 [10,11]. Note that, from the power spectrum, it is possible to extract only the corner frequency f c , which is a function of KD, and these two parameters cannot be extracted separately as in our formalism.…”
Section: Theoretical Backgroundmentioning
confidence: 99%