2019
DOI: 10.1364/aop.11.000577
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Perspective on light-induced transport of particles: from optical forces to phoretic motion

Abstract: Propulsive effects of light, which often remain unnoticed in our daily-life experience, manifest themselves on spatial scales ranging from subatomic to astronomical. Light-mediated forces can indeed confine individual atoms, cooling their effective temperature very close to absolute zero, as well as contribute to cosmological phenomena such as the formation of stellar planetary systems. In this review, we focus on the transport processes that light can initiate on small spatial scales. In particular, we discus… Show more

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Cited by 113 publications
(74 citation statements)
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References 571 publications
(758 reference statements)
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“…Among the numerous artificial analogs, colloidal heat engines are, perhaps, the simplest (1). Directed motion is extracted either by imposing temperature gradients or isothermally, through a ratcheting mechanism (1,4). In the latter case, time-varying potentials can give the required effect (5).…”
Section: Introductionmentioning
confidence: 99%
“…Among the numerous artificial analogs, colloidal heat engines are, perhaps, the simplest (1). Directed motion is extracted either by imposing temperature gradients or isothermally, through a ratcheting mechanism (1,4). In the latter case, time-varying potentials can give the required effect (5).…”
Section: Introductionmentioning
confidence: 99%
“…In self-phoresis, a particle propels with a velocity that is proportional to a selfgenerated gradient via a phoretic mobility coefficient [10]. Self-thermophoresis, whereby motion is induced by the asymmetric heating of light-absorbing Janus particles [11], is particularly interesting due to the unique properties of light as a source of self-propulsion [12]. Here, the propulsion velocity is V ¼ −D T ∇T, where both the thermophoretic mobility D T [13] and the self-generated thermal gradient are independent of particle size [14].…”
mentioning
confidence: 99%
“…The standing wave phase can be changed in time, moving the interference pattern, in different ways, e.g., [ 9 , 52 ]: One of the laser beams can be moved by mechanically moving a mirror [ 7 ]; the phase of one of the laser beams can be controlled with an electro-optical modulator; or a frequency mismatch between the counterpropagating beams controlled by acousto-optical modulators produces a phase . Of course all these methods are amenable to an imperfect control and fluctuations.…”
Section: Noise In a Moving Optical Latticementioning
confidence: 99%