scholarly journals Positioning Accuracy in Holographic Optical Traps

Micromachines ◽  
2021 ◽  
Vol 12 (5) ◽  
pp. 559
Author(s):  
Frederic Català-Castro ◽  
Estela Martín-Badosa

Spatial light modulators (SLMs) have been widely used to achieve dynamic control of optical traps. Often, holographic optical tweezers have been presumed to provide nanometer or sub-nanometer positioning accuracy. It is known that some features concerning the digitalized structure of SLMs cause a loss in steering efficiency of the optical trap, but their effect on trap positioning accuracy has been scarcely analyzed. On the one hand, the SLM look-up-table, which we found to depend on laser power, produces positioning deviations when the trap is moved at the micron scale. On the other hand, phase quantization, which makes linear phase gratings become phase staircase profiles, leads to unexpected local errors in the steering angle. We have tracked optically trapped microspheres with sub-nanometer accuracy to study the effects on trap positioning, which can be as high as 2 nm in certain cases. We have also implemented a correction strategy that enabled the reduction of errors down to 0.3 nm.

2021 ◽  
Vol 9 ◽  
Author(s):  
Xing Li ◽  
Yuan Zhou ◽  
Yanan Cai ◽  
Yanan Zhang ◽  
Shaohui Yan ◽  
...  

Enabled by multiple optical traps, holographic optical tweezers can manipulate multiple particles in parallel flexibly. Spatial light modulators are widely used in holographic optical tweezers, in which Gaussian point (GP) trap arrays or special mode optical trap arrays including optical vortex (OV) arrays, perfect vortex (PV) arrays, and Airy beam arrays, etc., can be generated by addressing various phase holograms. However, the optical traps in these arrays are almost all of the same type. Here, we propose a new method for generating a hybrid optical trap array (HOTA), where optical traps such as GPs, OVs, PVs, and Airy beams in the focal plane are combined arbitrarily. Also, the axial position and peak intensity of each them can be adjusted independently. The energy efficiency of this method is theoretically studied, while different micro-manipulations on multiple particles have been realized with the support of HOTA experimentally. The proposed method expands holographic optical tweezers’ capabilities and provides a new possibility of multi-functional optical micro-manipulation.


2019 ◽  
Vol 9 (10) ◽  
pp. 2012 ◽  
Author(s):  
Rujia Li ◽  
Liangcai Cao

Phase-only Spatial Light Modulator (SLM) is one of the most widely used devices for phase modulation. It has been successfully applied in the field with requirements of precision phase modulation such as holographic display, optical tweezers, lithography, etc. However, due to the limitations in the manufacturing process, the grayscale-phase response could be different for every single SLM device, even varying on sections of an SLM panel. A diverse array of calibration methods have been proposed and could be sorted into two categories: the interferometric phase calibration methods and the diffractive phase calibration methods. The principles of phase-only SLM are introduced. The main phase calibration methods are discussed and reviewed. The advantages of these methods are analyzed and compared. The potential methods for different applications are suggested.


Author(s):  
H Mushfique ◽  
J Leach ◽  
R Di Leonardo ◽  
M J Padgett ◽  
J M Cooper

This paper describes techniques for generating and measuring fluid flow in microfluidic devices. The first technique is for the multi-point measurement of fluid flow in microscopic geometries. The flow sensing method uses an array of optically trapped microprobe sensors to map out the fluid flow. The optical traps are alternately turned on and off such that the probe particles are displaced by the flow of the surrounding fluid and then retrapped. The particles' displacements are monitored by digital video microscopy and directly converted into velocity field values. The second is a method for generating flow within a microfluidic channel using an optically driven pump. The optically driven pump consists of two counter-rotating birefringent vaterite particles trapped within a microfluidic channel and driven using optical tweezers. The transfer of spin angular momentum from a circularly polarized laser beam causes the particles to rotate at up to 10 Hz. The pump is shown to be able to displace fluid in microchannels, with flow rates of up to 200 m−3 s−1 (200 fL s−1). In addition a flow sensing method, based upon the technique mentioned above, is incorporated into the system in order to map the magnitude and direction of fluid flow within the channel.


2013 ◽  
Vol 787 ◽  
pp. 423-426
Author(s):  
Kai Xu ◽  
Jing Li ◽  
Gang Du ◽  
Chun Li Zhu ◽  
Peng Fei Li ◽  
...  

A microsphere trapped by optical tweezers moves according to the Brownian motion law, which can be described by the Langevin equation. Based on it, a quadrant photodiode (QD) is used to track the displacement of the microsphere with a diameter of 2.5um trapped by holographic optical tweezers, and power spectrum method is adopted to obtain radial trap stiffness. Experiments show that the trap stiffness increases with the increase of the laser power, and decreases as the distance between the optical trap and the inside bottom surface of the sample cell increases.


2021 ◽  
Vol 9 ◽  
Author(s):  
Andrew B. Matheson ◽  
Tania Mendonca ◽  
Graham M. Gibson ◽  
Paul A. Dalgarno ◽  
Amanda J. Wright ◽  
...  

Microrheology with optical tweezers (MOT) measurements are usually performed using optical traps that are close to isotropic across the plane being imaged, but little is known about what happens when this is not the case. In this work, we investigate the effect of anisotropic optical traps on microrheology measurements. This is an interesting problem from a fundamental physics perspective, but it also has practical ramifications because in 3D all optical traps are anisotropic due to the difference in the intensity distribution of the trapping laser along axes parallel and perpendicular to the direction of beam propagation. We find that attempting viscosity measurements with highly anisotropic optical traps will return spurious results, unless the axis with maximum variance in bead position is identified. However, for anisotropic traps with two axes of symmetry such as traps with an elliptical cross section, the analytical approach introduced in this work allows us to explore a wider range of time scales than those accessible with symmetric traps. We have also identified a threshold level of anisotropy in optical trap strength of ~30%, below which conventional methods using a single arbitrary axis can still be used to extract valuable microrheological results. We envisage that the outcomes of this study will have important practical ramifications on how all MOT measurements should be conducted and analyzed in future applications.


Author(s):  
Serge Monneret ◽  
Federico Belloni ◽  
Olivier Soppera

In this paper, we combine holographic multiple optical tweezers with a three-dimensional microfluidic system to create a versatile microlaboratory. In order to determine cells local and/or temporal response to stimuli, and therefore draw their map of sensitivity, one convenient way is to apply antigen-covered latex beads in order to bind to plasma membrane, by means of optical tweezers. Using multiple optical traps could improve the efficiency of the measurements, but also their versatility. Therefore, we have developed a complete system based on holographic optical tweezers to realise multiple-point interactions between beads and cells with control of the stimulation places, timing, and durations. As we plan to use our system to study biological events in the hour timescale, we have to keep beads and cells separated, in order to prevent unwanted beads to circulate freely in the sample and bind to the target cell during the experiment. We then introduced microstereolithography as a 3D micro-manufacturing approach to the rapid prototyping of three-dimensional fluidic microchambers of complex shapes inside the sample, comprising wells, channels and walls to inject beads locally and keep them separated from cells in our assays. We demonstrated the possibility for microSL to easily and rapidly (typically one hour) fabricate small and three-dimensional observation chambers with customized design of the flow channels, including fluidic reservoirs of typically 500–1500 μm diameter, 5–12 mm height, in order to facilitate manual filling. Several shapes of reservoirs designed to keep beads and cells separated in liquid samples have been realized and successfully tested. Some of them included up to 3 reservoirs, in order to allow co-distribution of different types of beads. Each reservoir typically contained 2–10 μl of solution holding the beads, with a horizontal outlet of 100–200 μm in diameter which allows beads to deposit locally on the microscope cover glass placed under the reservoir outlet. Limited extension of beads under the outlet on the glass has been confirmed, and the ability of the polymeric structures to confine beads in a restricted area has been demonstrated. In the following we present examples of manipulations by multiple holographic optical tweezers consisting at first in extracting several beads from such an area by going through an aperture designed in the structure, making them travel to the target cell, and finally depositing on its outer membrane.


Author(s):  
Shi-Qiang Li ◽  
Xuewu Xu ◽  
Rasna Maruthiyodan Veetil ◽  
Parikshit Moitra ◽  
Xinan Liang ◽  
...  

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Rodolphe Boudot ◽  
James P. McGilligan ◽  
Kaitlin R. Moore ◽  
Vincent Maurice ◽  
Gabriela D. Martinez ◽  
...  

Abstract We show that micro-machined non-evaporable getter pumps (NEGs) can extend the time over which laser cooled atoms can be produced in a magneto-optical trap (MOT), in the absence of other vacuum pumping mechanisms. In a first study, we incorporate a silicon-glass microfabricated ultra-high vacuum (UHV) cell with silicon etched NEG cavities and alumino–silicate glass (ASG) windows and demonstrate the observation of a repeatedly-loading MOT over a 10 min period with a single laser-activated NEG. In a second study, the capacity of passive pumping with laser activated NEG materials is further investigated in a borosilicate glass-blown cuvette cell containing five NEG tablets. In this cell, the MOT remained visible for over 4 days without any external active pumping system. This MOT observation time exceeds the one obtained in the no-NEG scenario by almost five orders of magnitude. The cell scalability and potential vacuum longevity made possible with NEG materials may enable in the future the development of miniaturized cold-atom instruments.


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