In addition to the gradient force, the scattering of incident photons from the
sphere will exert an axial force on the sphere. This force points downstream in the
direction of travel of the light beam and is known as thescattering forceFscat.
For an optical tweezers or optical trap implementation, typically a microscope
objective is used to focus a collimated input light beam into an exit beam with a
tightly focused axially symmetric Gaussian intensity profile, as is shown in
Fig.11.2. A very strong electricfield gradient exists within the narrowest portion of
Low intensity
ray 1
High intensity
ray 2
Photon momentum
change of ray 1
Photon momentum
change of ray 2
Intensity
Position
Incident
photons
Force F 2
from ray 2
Force F 1
from ray 1
Intensity
distribution
Fig. 11.1 Basic Scattering force Fscat
geometric-optics principle of
optical tweezersaA
transverse intensity variation
gives a gradient force pointing
towards the region of highest
intensity;bScattering of
photons yields a forward
scattering force
x Particle displacement
Beam waist
Microscope
objective
Trap center
Gaussian input beam
Lateral force
Low
intensity
Low
intensity
High
intensity
Intensity profile
across beam face
Fig. 11.2 Exit beam from a
microscope objective with a
tightly focused axially
symmetric Gaussian intensity
profile
326 11 Biophotonics Technology Applications