2021
DOI: 10.1364/aop.394888
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Optical tweezers — from calibration to applications: a tutorial

Abstract: Since their invention in 1986 by Arthur Ashkin and colleagues, optical tweezers have become an essential tool in several fields of physics, spectroscopy, biology, nanotechnology, and thermodynamics. In this Tutorial, we provide a primer on how to calibrate optical tweezers and how to use them for advanced applications. After a brief general introduction on optical tweezers, we focus on describing and comparing the various available calibration techniques. Then, we discuss some cutting-edge applications of opti… Show more

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Cited by 159 publications
(121 citation statements)
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References 541 publications
(852 reference statements)
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“…The experiments are carried out using a miniaturized dual-beam setup [ 47 , 48 , 49 ]. Briefly, two tightly focused counter-propagating laser beams (P = 200 mW, = 845 nm) create a single optical trap, modelled as an harmonic potential ( Figure 1 a).…”
Section: Methodsmentioning
confidence: 99%
“…The experiments are carried out using a miniaturized dual-beam setup [ 47 , 48 , 49 ]. Briefly, two tightly focused counter-propagating laser beams (P = 200 mW, = 845 nm) create a single optical trap, modelled as an harmonic potential ( Figure 1 a).…”
Section: Methodsmentioning
confidence: 99%
“…Extensions of Equation ( 1) to the three dimensional case, r = (x, y, z), which are relevant in many experimental situations using optical trapping techniques [52], are possible by a proper choice of the potential U(r, t) and a tensorial form of the memory kernel for particles of arbitrary shape [53]. Here, for the sake of simplicity we focus on the dynamics of a single coordinate of a spherical particle of radius a, which is confined by a harmonic potential U(x, t) = 1 2 κ(t)x(t) 2 , where κ(t) is the stiffness at time t of the corresponding restoring force.…”
Section: Modelmentioning
confidence: 99%
“…Furthermore, without loss of generality we choose constant values of the low and high-frequencies viscosities that are typical of viscoelastic fluids prepared in aqueous solution in semidilute regimes [42,62,66,70,71]: η 0 = 0.040 Pa s and η ∞ = 0.004 Pa s, which correspond to α = 9. The diameter of the colloidal particle is set to a = 0.5 µm, while the maximum and minimum values of the trap stiffness during the Stirling cycle are chosen as κ M = 5 pN µm −1 and κ m = 1 pN µm −1 , respectively, which are easily accessible with optical tweezers [52]. The temperatures of the reservoir during the hot and cold part of the cycle are T c = 5 • C and T h = 90 • C, which are selected in such a way that they are within the temperature range in which water, which is a common solvent component of many viscoelastic fluids, remains liquid.…”
Section: Numerical Solutionmentioning
confidence: 99%
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“…There are extensive reviews in the literature describing in detail different OT calibration methods ( Gieseler et al., 2020 ; N.B.V., unpublished data), and the advantages and disadvantages of all methods. Here, we describe one of the simplest calibration procedures based on the Stokes-Faxén law for the viscous drag force acting on a microsphere immersed within a fluid ( Nicholas et al., 2014 ; N.B.V., unpublished data).…”
Section: Before You Beginmentioning
confidence: 99%