Elastic theory for the deformation of a spherical dielectric biological object under electro-optical trapping

RSC Advances ◽  
2015 ◽  
Vol 5 (55) ◽  
pp. 44458-44462 ◽  
Author(s):  
Md. Mozzammel Haque

The shear modulus of a dielectric spherical particle is investigated using a combination of triangular (or square) electrodes and a single-beam optical tweezer.

Photonics ◽  
2020 ◽  
Vol 7 (4) ◽  
pp. 84
Author(s):  
Xi Liu ◽  
Song Hu ◽  
Yan Tang

As water is normally used as the immersion medium in optically trapped microsphere microscopy, the high-refractive-index barium titanate glass (BTG) microsphere shows a better imaging performance than the low-index polystyrene (PS) or melamine formaldehyde (MF) microsphere, but it is difficult to be trapped by single-beam optical trapping due to its overly high refractive index. In this study, coated BTG microspheres with a PS coating have been computationally explored for the combination of optical trapping with microsphere-assisted microscopy. The PS coating thickness affects both the optical trapping efficiency and photonic nanojet (PNJ) property of the coated BTG sphere. Compared to the uncoated BTG sphere, the coated BTG sphere with a proper PS coating thickness has a highly improved trapping efficiency which enables single-beam optical trapping, and a better PNJ with a higher optical intensity Imax and a narrower full width at half maximum (FWHM) corresponding to better imaging performance. These coated BTG spheres also have an advantage in trapping efficiency and imaging performance over conventional PS and MF spheres. The coated BTG microsphere is highly desirable for optically trapped microsphere super-resolution microscopy and potentially beneficial to other research areas, such as nanoparticle detection.


2015 ◽  
Vol 74 (8) ◽  
Author(s):  
Wan Nor Suhaila Wan Aziz ◽  
Shahrul Kadri Ayop ◽  
Sugeng Riyanto

In this paper, we review the recent applications of optical tweezer (OT) in studying the microrheology of variety of polymeric solution. Our aim is to expose optical tweezer research to the public and newcomer. This paper highlights and summarizes the advantages of optical tweezer as compared with the conventional method, introduces the benefit of nanocellulose and also presents an overview of the potential in the measurement of nanocellulose solution’s viscoelasticity by using optical trapping method.


2010 ◽  
Vol 19 (02) ◽  
pp. 371-378 ◽  
Author(s):  
P. YOUPLAO ◽  
T. PHATTARAWORAMET ◽  
S. MITATHA ◽  
C. TEEKA ◽  
P. P. YUPAPIN

We propose a novel system of an optical trapping tool using a dark-bright soliton pulse-propagating within an add/drop optical filter. The multiplexing signals with different wavelengths of the dark soliton are controlled and amplified within the system. The dynamic behavior of dark bright soliton interaction is analyzed and described. The storage signal is controlled and tuned to be an optical probe which can be configured as the optical tweezer. The optical tweezer storage is embedded within the add/drop optical filter system. By using some suitable parameters, we found that the tweezers storage time of 1.2 ns is achieved. Therefore, the generated optical tweezers can be stored and amplified within the design system. In application, the optical tweezers can be stored and trapped light/atom, which can be transmitted and recovered by using the proposed system.


1990 ◽  
Author(s):  
Rosemarie W. Steubing ◽  
Steve Cheng ◽  
William H. Wright ◽  
Yasuyuki Numajiri ◽  
Michael W. Berns

2018 ◽  
Vol 7 (4.30) ◽  
pp. 371
Author(s):  
Mohd Farid Mohamad Yusof ◽  
, Muhamad Safuan Mat Yeng ◽  
Shahrul Kadri Ayop

Calibration of axial quadrant photodetector (QPD) signal to the trapped bead position in an optical tweezer is important to measure the quantitative mechanical parameter in axial (laser propagation) direction. An alternative calibration based on the Stuck Bead Method (SBM) was proposed in this study. 3 µm polystyrene beads were stuck at the surface of glass coverslip and moved axially around the laser focus. QPD was used to obtain the position dependent intensity profile at three different laser powers (19.8 mW, 34.1 mW, 48.5 mW). The QPD signal-to-distance calibration value was consistent at 26 mV/µm for the used bead at the three laser powers. It was found that the calibration values are independent of laser powers and limited by the resolution of distance adjustment.


2014 ◽  
Vol 53 (8) ◽  
pp. 085107 ◽  
Author(s):  
Steven Ross ◽  
Mark F. Murphy ◽  
Francis Lilley ◽  
Michael J. Lalor ◽  
David R. Burton

Sign in / Sign up

Export Citation Format

Share Document