=Paper=
{{Paper
|id=Vol-1490/paper2
|storemode=property
|title=Optical trapping of air-borne light-absorbing particles with various laser beams
|pdfUrl=https://ceur-ws.org/Vol-1490/paper2.pdf
|volume=Vol-1490
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==Optical trapping of air-borne light-absorbing particles with various laser beams==
https://ceur-ws.org/Vol-1490/paper2.pdf
Computer Optics and Nanophotonics
Optical trapping of air-borne light-absorbing particles
with various laser beams
Porfirev A.P.
Samara State Aerospace University
Image Processing Systems Institute, Russian Academy of Sciences
Abstract. We demonstrate optical trapping carbon nanoparticle agglomerations
in the air employing photophoretic forces. Three types of laser beams were used
for optical trapping: a focused Hermite-Gaussian laser beam (TEM10), an
optical bottle beam and a hollow optical beam generated by Bessel beams
superposition. The experimental results for each of the laser beams types are
shown. Description of trapping features in each case is shown. Perspectives of
application for each type of laser beams for three-dimensional optical
manipulation are discussed.
Keywords: optical trapping, light-absorbing particles, Hermite-Gaussian beam,
optical bottle beam, hollow optical beam
Citation: Porfirev A.P. Optical trapping of air-borne light-absorbing particles
with various laser beams. Proceedings of Information Technology and
Nanotechnology (ITNT-2015), CEUR Workshop Proceedings, 2015; 1490: 9-
16. DOI: 10.18287/1613-0073-2015-1490-9-16
Introduction
The optical manipulation of micro- and nanoscale objects with a laser beam was
first demonstrated by A. Ashkin [1]. To date, this technique is widely used in the area
of biophotonics and micromechanics for the manipulation of micro- and nano-objects
[2-8]. Implementation of optical manipulation is possible in various environments
such as in liquids or air. The causes of trapping are different depending on the
medium and parameters of trapped objects. Therefore, the trapping of transparent
micro-objects in liquids is typically carried out due to the action of the gradient force
of a focused laser beam [9]. The trapping of light-absorbing micro-objects in air
occurs through the action of photophoretic forces [10]. In the latter case, there are two
phenomena present: positive photophoresis (particles move in a direction from the
light source) and negative photophoresis (particles move towards the light source)
[11].
This paper presents a comparison of the optical manipulation of light-absorbing
carbon nanoparticle agglomerations using laser beams of three types: 1) a focused
Hermite-Gaussian (HG) laser beam (TEM10); 2) an optical bottle beam (a beam with
dark regions of exactly zero intensity surrounded by regions of higher intensity) [12];
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Computer Optics and Nanophotonics Porfirev A.P. Optical trapping of air-borne…
and 3) a hollow optical beam that has zero intensity on the optical axis. Each of these
beams has certain features that allows one to perform various types of manipulation.
Optical manipulation with a Hermite-Gaussian laser beam (TEM10)
In [13], it was shown that it is possible to carry out the three-dimensional trapping
of non-spherical light-absorbing particles with a single focused Gaussian beam. This
is possible through the action of the photophoretic force resulting from a different
thermal accommodation coefficient that depends strongly on the surface state. In fact,
the trapping of particles occurs in a region near the laser beam focus. Thus, it is
possible to carry out independent multiple manipulation of light-absorbing particles
by forming a plurality of intensity peaks in the focal plane.
The Hermite-Gaussian mode is described by the following well known expression
[11]:
2
w 2x 2 y
Enm x, y, z i n m Hn Hn
w z w z w z
x2 y 2 ik x 2 y 2
exp 2 (1)
w z 2R z
z
exp i n m 1 arctg ,
z 0
12
kw2 z 2 z 2
where z0 , w z w 1 , R z z 1 ,
2 z0 z0
w is the Gaussian beam waist, R(z) is the Gaussian beam’s wavefront curvature
radius, z0 is the Rayleigh range, k is the wavenumber of light, Hn(x) is the Hermite
polynomial.
Such beams are propagation-invariant (up to scale); that is, they keep structure of
the transverse intensity distribution. Figure 1 shows the cross-section profiles of the
intensity distribution for the different orders Hermite-Gaussian beams. We see that
the order of a HG beam determines the number of generated intensity peaks, each of
which can be used as an optical trap to capture light-absorbing particles in gaseous
media.
a) b) c) d)
Fig. 1. – Cross-section profiles of the intensity distribution for Hermite-Gaussian laser beams:
(a) TEM10, (b) TEM20, (c) TEM11, (d) TEM22
In optical trapping and optical guiding experiments, we use a laser TEM 10 (λ = 457
nm, with a maximum output power of 2000 mW) (Fig. 8). An optical scheme of the
experimental setup shown in Figure 2a. A generated beam is focused horizontally by
a micro-objective MO (3.7×, NA=0.1) in the area inside the glass cuvette C
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containing a suspension of micro-particles. Observation of the particle trapping is
possible due to the scattered light recorded by the video camera Cam (Panasonic
HDC-SD800, 1920 × 1080 pixels). A neutral density filter F has been used to adjust
the power of the laser beam.
10 μm
a) b)
Fig. 2. – Optical manipulation experiment: (a) an experimental setup: L is a laser TEM 10
(λ=457 nm), F is a neutral density filter, MO is a micro-objective (3.7×, NA=0.1), C is a glass
cuvette, Cam is a video camera Panasonic HDC-SD800 (1920 × 1080 pixels); (b) carbon
nanoparticle agglomerations used in experiment
To demonstrate the optical trapping and holding of absorbing particles, we used
carbon nanoparticle agglomeration. The typical size of the agglomerations ranged to
up to tens of micrometers (Figure 2b). The particles were sprayed with a syringe
pump. Therefore, the particles initially had a significant acceleration directed to the
bottom of the cuvette. The particles settled in the bottom of the cuvette under the
influence of gravity. Some of them were trapped in the area of the laser beam. The
guiding of the trapped particles was carried out by moving the micro-objective, which
can be moved in three mutually perpendicular directions. As a result, movement of
the focused laser beam results in movement of the trapped micro-particles.
Figure 3 shows the movement stage of two carbon nanoparticle agglomerations,
each of which was trapped in the various intensity peaks of the HG TEM 10 laser
beam. In this case, we carried out a controlled movement of the optically trapped
micro-objects.
y
x MO C
x
a) 20 μm b) z 5 mm
c)
5 mm
d)
5 mm
Fig. 3. – Optical trapping and guiding two carbon nanoparticle agglomerations with a Hermite-
Gaussian TEM10 laser beam: (a) trapped particles (denoted by white arrows); (b)-(d) movement
stages of particles in plane xz
Thus, the structure of the HG beams allows simultaneous, parallel three-
dimensional movement of several trapped light-absorbing micro-particles. The
particles retain their relative position when moving in the space. These beams offer
new opportunities for the controlled, multiple simultaneous manipulation of light-
absorbing non-spherical micro-objects. For example, it is possible to transport an
array of light-absorbing particles, while their original location relative to each other
will remain. Furthermore, this technique does not require the additional modulators to
create multiple optical traps.
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Optical manipulation with optical bottle beams
Photophoresis phenomenon causes a light-absorbing object to move in a direction
from the more heated to the less heated side of object. This makes it impossible to
trap spherical micro-objects with a single Gaussian beam. The so-called optical bottle
beams allow stable three-dimensional trapping of light-absorbing micro-particles to
be carried out in gaseous media. An optical bottle beam is a beam with dark regions
of exactly zero intensity surrounded by regions of higher intensity. For generation
optical bottle beams, we used the method based on the formation of Bessel beams
superposition [15]. This method enabled an optical bottle beam to be formed with a
predetermined shape, such as a double optical bottle or optical bottle with a triangular
profile of the intensity distribution.
For the experiments with optical bottle beams, we used the particles presented in
Figure 2b. Figure 4 shows the optical scheme of the experimental setup. The laser
beam is transformed by the diffractive optical element DOE focused in the area inside
glass cuvette by the micro-objective MO (3.7×, NA = 0.1). Observation was carried
out by a lens L3. Adjustment of the output power of the laser beam allows us to vary
intensity of formed traps and, therefore, change the values of the photophoretic forces
acting on the trapped particles.
Fig. 4. – Experimental setup: L is a solid-state laser (λ=532 nm), M1, M2 are mirrors, L1, L2,
L3 are lenses, DOE is a diffractive optical elements that forms an optical bottle beam, BS is a
beam splitter, LED is illuminating light-emitted diode, MO is a micro-objective (3.7×, NA =
0.1), C is glass cuvette, Cam is a CCD video camera
Figure 5 illustrates a typical trapping single carbon nanoparticle agglomeration
with a single optical bottle. It can be seen that the trapped agglomeration remains in
the optical trap during its transfer. We moved the optical trap by moving the focusing
micro-objective MO, similar to experiments with a Hermite-Gaussian TEM10 laser
beam. For this experiment, we have managed to move the agglomeration along the
beam axis at distance of about 340 µm. The estimated value of the power within the
boundaries of the optical bottle is about 16 mW.
The methods described in [16], allow optical bottle arrays to form. The use of
optical bottle arrays enables the boundary of trapping to be increased without
changing the size of the traps themselves. As shown in [17], if the dimensions of the
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formed light traps and trapped micro-objects do not match, it is impossible to achieve
stable trapping of micro-objects because they move uncontrollably inside the trap.
a) d)
y y
z 100 μm z 100 μm
b) e)
y y
z 100 μm z 100 μm
c) f)
y y
z 100 μm z 100 μm
Fig. 5. – Experimental demonstration of trapping and guiding the carbon nanoparticles
agglomeration with a single optical bottle. The black arrow points to the agglomeration
Optical manipulation with hollow optical beams
Hollow optical beams (HOBs) are optical beams with zero axial intensity along the
propagation axis. These beams have diffraction-free properties on a limited interval
along the optical axis. Due to such a configuration, the HOBs are universal optical
traps to trapping both transparent and opaque micro-particles [18, 19].
There are various methods of forming such HOBs that have a predetermined cross-
sectional shape [20-24]. Changing the cross-sectional shape of the beams can change
the shape of the region in which trapped particles will be moved.
In optical trapping experiments with HOBs, we used a solid-state laser L (λ = 532
nm, with a maximum output power of 500 mW) (Figure 6). The laser beam was
expanded with a telescope (L1 with f1 = 15 mm and L2 with f2 = 35 mm) to illuminate
the DOE formed HOB. An airborne absorbing particle in a cuvette is trapped in the
area of minimum intensity of the generated HOB. Observation of the particle trapping
was possible due to the scattered light recorded by the video camera Cam (MDCE-5,
1280 × 1024 pixels). The particles were imaged through a micro-objective MO (8×,
NA=0.2).
To demonstrate the optical trapping and holding of absorbing particles, we used
carbon nanoparticle agglomeration as in the experiments described above (Figure 2b).
Figure 7 shows the motion stages of a carbon nanoparticle agglomeration trapped by
the HOB with an intensity distribution in the form of a regular pentagon contour. It
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can be clearly seen that the particle is also moved in a limited volume. At the time
when the trapped particles remain inside the region of minimum intensity of the
formed HOB, other particles settle on the bottom of the cuvette under the influence of
gravity. Trapped particles do not leave the boundaries of the HOB because
photophoretic force push them away from the region of maximum intensity in the
region on the optical axis of the beam.
Fig. 6. – Experimental setup: L is a solid-state laser (λ=532 nm), L1, L2 are lenses, DOE is a
diffractive optical elements that forms a hollow optical beam, MO is a micro-objective (8×,
NA=0.2), C is glass cuvette, Cam is a CCD video camera MDCE-5 (1280 × 1024 pixels)
a) b)
c) d)
e) f)
Fig. 7. – Optical trapping and holding of light-absorbing particles with HOB formed by DOE
The use of additional focusing optics enables the generation of converging HOBs,
which have predetermined intensity distribution. It is therefore possible to form a
complex spatial configuration of the optical beams. Each of these beams can be used
to hold the particles in the region of desired size and shape. This ‘storage’ of micro-
particles can be used for contactless transport of microscopic objects. Furthermore,
they can be used to study the interaction of various micro-objects trapped in a limited
volume.
Conclusion
The paper describes the various ways to manipulate air-borne light-absorbing
microscopic objects in air with laser beams of different types. The results of trapping
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Computer Optics and Nanophotonics Porfirev A.P. Optical trapping of air-borne…
and manipulation experiments for each of laser beam types are shown. It is shown
that:
1) With the use of Hermite-Gaussian beams, it is possible to achieve stable
multiple trapping and guiding of light-absorbing non-spherical particles in generated
separate intensity peaks;
2) With the use of optical bottle beams, it is possible to achieve stable trapping and
guiding of the same particles at distances of hundreds of times their own dimensions;
3) With the use of hollow optical beams with a predetermined shape, trapping and
holding light-absorbing particles can be carried out inside an area of predetermined
shape within the area given shape, the dimensions of which exceed by ten times the
particles’ size.
None of these cases d require high-power lasers (enough power about 10-20 mW),
due to the fact that photophoretic forces exceed the radiation pressure forces at the
order of atmospheric pressure. [20].
Acknowledgements
This work was supported by the Ministry of Education and Science of the Russian
Federation and Russian Foundation for Basic Research Grants No. 14-07-97038,
No. 14-07-31291, No. 14-07-00177.
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