Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.
Optical Tweezers Sarah Nichols March 17, 2004
Outline • Motivations • Operation • Layout • Successes and Difficulties • Future Directions
Why use optical tweezers? • Can manipulate living cells and organelles • Can measure stretching of large molecules such as DNA • Measure and manipulate mechanoenzymes and other physically acting molecules • Relatively cheap and easy to build a simple setup • Useful tool for learning various optics procedures and terms
How it works • dobject>>dbeam -> ray optics approximation is valid • Reflection and refraction create opposing forces on a dielectric object • If the beam is strong enough, the gradient force can overcome the scattering and gravitational forces • Rays from edge of lens are deflected most, so they have the biggest trapping impact Amendola, 2001
Components • 20 mW diode laser • 2 cylindrical lenses for shaping • Mirrors for redirection • 2 spherical lenses for resizing • Periscope to raise the beam • Dichroic mirror to direct beam into microscope • Microscope with 100x oil immersion objective, eyepiece removed • Camera connected to TV screen for viewing M1 Cylindrical lenses Laser Spherical lenses Periscope Microscope M2 Infinity-correcting lens
Layout Camera Filter Dichroic mirror Beam block Microscope
Optimization • Beam must be aligned to travel exactly vertically through microscope • For best trapping, beam should be spherical • Optimal beam size overfills the objective slightly FWHM 6 mm for our setup (Amendola, 2001) • Microscope objective does not collect light from infinity, so a lens should focus light 160 mm behind the objective • Trapping most easily achieved with moving objects; surfactants used in bead solutions
Results • Despite numerous alignments, beam was weak until very recently • Objective replacement improved beam strength • Weak trapping demonstrated for yeast cells (~ 5 um) as well as 5 and 10 um polystyrene spheres • With small yeast cells, can drag horizontally and vertically
Results Untrapped 5 um spheres Trapped sphere
Questions • Why is it easier to trap with yeast cells for a given size? (they exhibit more Brownian motion, but why?) • Why does overfilling rule not hold? “Optimal” FWHM size: 6 mm. Measured size: 6-6.5 mm. Trapping size: 4 mm. • Why does non-infinity correction make trapping harder?
Suggested Improvements • Clean lenses, replace mirrors • Replace diode laser for a less elliptical beam • Determine reason for cell/sphere distinctions • Mount a lens on a translation stage for beam steering with less intensity loss • Determine reason for failure to agree with predictions - pure intensity loss or other reasons? • Upgrade camera for digitized still and motion pictures
Acknowledgements Thanks to Dr. John Noé and Yiyi Deng for their help in adjusting to the vagaries of the system. Thanks also to Duke Scientific for their donation of microspheres to the Laser Teaching Center for testing. References P. Amendola. “Design and Construction of an Optimized Optical Tweezers.” Intel Science Talent Search Report (2001). Y. Deng, “Optical Tweezers”, http://laser.physics.sunysb.edu/~yiyi (2003). S. Smith et al., Am. J. Phys. 67, 26 (1999). Z. Ulanowski and I.K. Ludlow, Meas. Sci. Technol. 11, 1778 (2000).
Slide Setup Deng (2003)