1. “Nanophotonics and Optical Control of Single Nanoparticles” Keonwoo Nam Moscow 2012 Supervisor: Professor A. A. Fedyanin Lomonosov Moscow State University, Faculty of Physics

2. Introduction to Optical Tweezers

3. OUTLINE  Brief History of Optical Tweezers  Principles of Optical Tweezers  Optical Trapping Forces  The Optical Tweezers Set up & The Experimental Method  Research Areas and Possible uses

4. What is… Optical Tweezers - one of the techniques, which use a highly focused beam to control and hold microscopic particles.

5. History  Johannes Kepler (1571-1630): noticed comet's tail always points away from the sun, because of the sun's radiation pressure.  James Maxwell (1831-1879): existence of the light pressure was demonstrated  P. N. Lebedev (1866-1912): measured the light pressure  Albert Einstein (1879-1955): confirmed that photons possess its own momentum  Arthur Compton (1892-1962:) showed the existence of the light momentum on his experimental work

6.  In 1970 A. Ashkin proved that light can grab and release nanometer particles by its momentum, using the light Quantum Theory.  In 1986, A. Ashkin proved that he could trap 10nm diameter dielectric particles only using gradient force  In 1987, A. Ashkin showed the damage-free manipulation on cells using an infrared laser Arthur Ashkin History

7. Types of OT  Single Beam Optical Tweezers  Dual beam Optical Tweezers  Holographic Optical Tweezers

8. Principles of OT  Exert a laser beam to the very small particle, the light will be reflected or refracted from the surface of the particle. The momentum of photon, refracted to the particle, will be changed and by the law of the conservation of the momentum, the force of the variation of momentum will be exerted to the small particle. (a) If the particle is to the left, say, of the center of the beam, it will refract more light from the right to the left, rather than vice versa. The net effect is to transfer momentum to the beam in this direction, so, by Newton’s third law, the particle will experience an equal and opposite force – back towards the center of the beam. In this example the particle is a dielectric sphere (b) Similarly, if the beam is tightly focused it is possible for the particle to experience a force that pushes back towards the laser beam. (c) We can also consider an energetic argument: when a polarizable particle is placed in an electric field, the net field is reduced. The energy of the system will be a minimum when the particle moves to wherever the field is highest – which is at the focus. Therefore, potential wells are created by local maxima in the fields. How optical tweezers work Optical tweezers: the next generation, Kishan Dholakia, 2002, physics world

9. Conditions of OT The Ray Optical Regime of Optical Tweezers Wonhoe Koo, Seoul, 2005 The Electromagnetic Regime of Optical Tweezers

10. Two Forces The Electromagnetic Regime of Optical Tweezers The Gradient Force

11. Two Forces The Gradient Force The Ray Optical Regime of Optical Tweezers Wonhoe Koo, Seoul, 2005

12. The Basic OT Set up A generic optical tweezers diagram with only the most basic components The Optical Tweezers, Wikipedia

13. Research areas  Study and manipulate particles such as atoms, molecules and small dielectric spheres (in range from  m to nm).  Force measurements of biological objects in piconewton range.  Biological investigations involving cells  Cutting and ablating biological objects (Cell fusion and DNA cutting)  Force measurements of cell structures and DNA coiling  Elasticity measurements of DNA

14. Thank you ^-^ Keonwoo Nam