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 1High intensity
ray 2Photon momentum
change of ray 1Photon momentum
change of ray 2Intensity
PositionIncident
photonsForce F 2
from ray 2Force F 1
from ray 1Intensity
distributionFig. 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 displacementBeam waistMicroscope
objectiveTrap centerGaussian input beamLateral forceLow
intensityLow
intensityHigh
intensityIntensity profile
across beam faceFig. 11.2 Exit beam from a
microscope objective with a
tightly focused axially
symmetric Gaussian intensity
profile
326 11 Biophotonics Technology Applications