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Fabrication and Optimisation of
Fly’s Eye UV LED Homogenizer
for DMDs
Advisor – Proof. Y. C. Lee
Advisee – Vikram sachan (N16057211)
2018 / 07 / 23
Outline
• Introduction of fly’s eye homogenizer and DMD.
• Zemax simulation of optical setup.
• Mold design and fabrication.
• Experimental results and conclusions.
• Introduction of fly’s eye homogenizer and DMD
1. What is Fly’s Eye Homogenizer.
2. Working principle.
3. Digital Micro mirror Devices (DMDs).
Fly’s Eye Homogenizer
• An optical beam homogenizer divides and redirects an incident beam to provide
uniform irradiation to a plane surface. The beam homogenizer is particularly
useful in an apparatus and method for uniform laser irradiation of materials.
Working of Fly’s Eye Homogenizer
Light
Source
Digital Micro mirror Devices (DMDs)
• The digital micro mirror device, or DMD, is a micro-opto-
electromechanical system (MOEMS).
• Zemax simulation of optical setup
1. Simulation (Zemax Optics Studio).
2. Available Lenses and Data.
3. Simulation Results (Merit function editor).
4. Simulation Results for collimation.
5. Simulation Results of Detector D1 (For UV LED) and
Detector D3 (For Homogenizer).
6. Fly’s Eye homogenizer Parameters.
Simulation (Zemax Optics Studio)
1. CBT-90_UV_Ray_Files_Zemax.dat file is used.
Fig. CBD – 90 – UV LED light source ( λ
= 405 nm & 120° divergence angle).Fig. A photograph of UV LED from Luminus.
Fig. UV LED light source intensity profile.
Fig. Angular distribution with normalized
intensity.
Fig. Zemax optics studio screenshot
showing way to insert UV led source file.
Available Lenses and Data
Aspherical
lens
Radius of
curvature
(Rleft) mm
Conic (Cleft) Thickness
mm
Radius of
curvature
(Rright)mm
Conic (Cright)
L1 99.637 0 25 -18.323 -0.798
L2 20.923 -0.640 21 0 0
L3 0 0 12 -10.462 -0.626
Table 1 – Aspherical Lens Data
L3
L2
L1
16.194mm
Simulation Results (Merit function editor)
Simulation Results
(For UV LED)
• Detector (D1)
Simulation Results for collimation
NSC Lightning Layout of Zemax Optics Studio
UV LED
L1 L2
L3
L4
D2
H
D3D1
Aspherical
lens
Radius of
curvature
(Rleft) mm
Conic (Cleft) Thickness
mm
Radius of
curvature
(Rright)mm
Conic (Cright)
L4 38.63 0 12.52 0 0
H 3.19858156 -0.5 11 3.19858156 -0.5
Detector (D3) – Fly’s Eye Homogenizer
Fig. Intensity Distribution –
a) False colour intensity distribution.
b) Cross-sectional view about Y axis(at
y=0).
c) Cross-sectional view about X axis axis(at
X=0).
• Mold design and fabrication
1. Solid works design of Homogenizer Mold and
Mold Assembly.
2. Molding, Curing and extraction process of
Homogenizer.
3. Confocal microlens profile Measurements.
Fly’s Eye Homogenizer Parameters
Microlens - 12X10
Solidworks Design of Homogenizer Mold
∅36
12mm
0.5mm
0.5mm
Mold Assembly
Fig. Solid works assembly view Fig. A photograph of steel mold assembly
with quartz plate (thickness = 10mm)
Molding Process -
1. PDMS
part A & B
4.
Vacuuming
process to
take
bubble out
2. Taken
1:1 by
weight
3. Mixed
well
around
5mins.
Curing Process
Curing parameters –
• Time Duration = 2hrs.
• Temperature
Gradually increase 25°C – 100°C then,
100°C – 25°C.
• Further cooling time after curing = 2hrs
Fig. Curing process
Fly’s Eye Homogenizer Separation from mold
PDMS
Microlens
array
Quartz
plate
10
Microlens
Fly’s Eye Homogenizer Mold
Confocal Microscope
Measurement for
replicated profile of
microlens arrays
Element 4X6
Confocal Microscope
Steel MoldFly’s Eye Homogenizer
Microlens Profile
Profile measurement under confocal microscope
• 1 microlens each time
• 50X
• Total no. of measurements
= 20.
• Time taken for each
measurement = 1hr
55mins (approximated).
Fig. Microlens
height view
Confocal Microscope
Aspheric Function plot
R
Z
R
Fig. Aspherical Lens
Fig. Matlab plot of aspheric function for given data
Zemax output data
Comparison of 2x2 element of side L and side R
Left Side (L) Right Side (R)
Comparison of 2x11 element of side L and side R
Left Side (L) Right Side (R)
Comparison of 5x6 element of side L and side R
Left Side (L) Right Side (R)
Comparison of 9x2 element of side L and side R
Left Side (L) Right Side (R)
Comparison of 9x11 element of side L and side R
Left Side (L) Right Side (R)
• Experimental results and conclusions
1. Experimental Setup.
2. Description of optical setup.
3. Experimental results comparison with simulation.
4. Conclusion.
5. Future Work
Experimental setup
Optical System
Detector
Experimental results
Measurement parameters –
Pitch = 0.05mm
Speed = 1mm/s
Time elapsed = 28hrs (approx.)
Fig. (a) shows contour display of intensity. (b) Intensity distribution of UV LED light at homogenization plane
A photograph of
actual UV light
Intensity at
homogenization
plane
Experimental results Comparison with Simulation
Fig. (a) Cross-sectional intensity distribution
at axis X = 0.
Fig. (a) Cross-sectional intensity distribution
at axis Y = 0.
Experiment
Simulation
Conclusion
• This work proposes a modification in the digital micro mirror device
(DMD). Since, fabrication of homogenizers by laser micro-machining
system is quite expensive to use and it is one-time fabrication only.
Using molding method for the manufacturing of fly’s eye UV LED
homogenizer is the cheapest way of manufacturing homogenizers. Once
the homogenizer steel mold is fabricated, we can produce any number
of homogenizers by using mold.
• The UV light used by the micro mirror devices will become more
collimated and flat top intensity distribution of UV light, hence the
quality of micro-machining of any substance will improve significantly.
Future Work
• PDMS Microlens profile irregularities after Demolding
process can be fixed by changing the fabricated mold
design.
• A different set of lens can be used to get more collimated
light from UV LED that decreases intensity slope and make it
more flat-top profile.
Future Work
• Better collimation angle can be achieved by using
different set of aspherical lenses.
Laser Beam Homogenizer
Laser Beam Homogenizer

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Laser Beam Homogenizer

  • 1. Fabrication and Optimisation of Fly’s Eye UV LED Homogenizer for DMDs Advisor – Proof. Y. C. Lee Advisee – Vikram sachan (N16057211) 2018 / 07 / 23
  • 2. Outline • Introduction of fly’s eye homogenizer and DMD. • Zemax simulation of optical setup. • Mold design and fabrication. • Experimental results and conclusions.
  • 3. • Introduction of fly’s eye homogenizer and DMD 1. What is Fly’s Eye Homogenizer. 2. Working principle. 3. Digital Micro mirror Devices (DMDs).
  • 4. Fly’s Eye Homogenizer • An optical beam homogenizer divides and redirects an incident beam to provide uniform irradiation to a plane surface. The beam homogenizer is particularly useful in an apparatus and method for uniform laser irradiation of materials.
  • 5. Working of Fly’s Eye Homogenizer Light Source
  • 6. Digital Micro mirror Devices (DMDs) • The digital micro mirror device, or DMD, is a micro-opto- electromechanical system (MOEMS).
  • 7. • Zemax simulation of optical setup 1. Simulation (Zemax Optics Studio). 2. Available Lenses and Data. 3. Simulation Results (Merit function editor). 4. Simulation Results for collimation. 5. Simulation Results of Detector D1 (For UV LED) and Detector D3 (For Homogenizer). 6. Fly’s Eye homogenizer Parameters.
  • 8. Simulation (Zemax Optics Studio) 1. CBT-90_UV_Ray_Files_Zemax.dat file is used. Fig. CBD – 90 – UV LED light source ( λ = 405 nm & 120° divergence angle).Fig. A photograph of UV LED from Luminus.
  • 9. Fig. UV LED light source intensity profile. Fig. Angular distribution with normalized intensity. Fig. Zemax optics studio screenshot showing way to insert UV led source file.
  • 10. Available Lenses and Data Aspherical lens Radius of curvature (Rleft) mm Conic (Cleft) Thickness mm Radius of curvature (Rright)mm Conic (Cright) L1 99.637 0 25 -18.323 -0.798 L2 20.923 -0.640 21 0 0 L3 0 0 12 -10.462 -0.626 Table 1 – Aspherical Lens Data L3 L2 L1
  • 12. Simulation Results (For UV LED) • Detector (D1)
  • 13. Simulation Results for collimation
  • 14. NSC Lightning Layout of Zemax Optics Studio UV LED L1 L2 L3 L4 D2 H D3D1 Aspherical lens Radius of curvature (Rleft) mm Conic (Cleft) Thickness mm Radius of curvature (Rright)mm Conic (Cright) L4 38.63 0 12.52 0 0 H 3.19858156 -0.5 11 3.19858156 -0.5
  • 15. Detector (D3) – Fly’s Eye Homogenizer Fig. Intensity Distribution – a) False colour intensity distribution. b) Cross-sectional view about Y axis(at y=0). c) Cross-sectional view about X axis axis(at X=0).
  • 16. • Mold design and fabrication 1. Solid works design of Homogenizer Mold and Mold Assembly. 2. Molding, Curing and extraction process of Homogenizer. 3. Confocal microlens profile Measurements.
  • 17. Fly’s Eye Homogenizer Parameters Microlens - 12X10
  • 18. Solidworks Design of Homogenizer Mold ∅36 12mm 0.5mm 0.5mm
  • 19. Mold Assembly Fig. Solid works assembly view Fig. A photograph of steel mold assembly with quartz plate (thickness = 10mm)
  • 20. Molding Process - 1. PDMS part A & B 4. Vacuuming process to take bubble out 2. Taken 1:1 by weight 3. Mixed well around 5mins.
  • 21. Curing Process Curing parameters – • Time Duration = 2hrs. • Temperature Gradually increase 25°C – 100°C then, 100°C – 25°C. • Further cooling time after curing = 2hrs Fig. Curing process
  • 22. Fly’s Eye Homogenizer Separation from mold PDMS Microlens array Quartz plate 10 Microlens Fly’s Eye Homogenizer Mold
  • 23. Confocal Microscope Measurement for replicated profile of microlens arrays Element 4X6 Confocal Microscope Steel MoldFly’s Eye Homogenizer Microlens Profile
  • 24. Profile measurement under confocal microscope • 1 microlens each time • 50X • Total no. of measurements = 20. • Time taken for each measurement = 1hr 55mins (approximated). Fig. Microlens height view Confocal Microscope
  • 25. Aspheric Function plot R Z R Fig. Aspherical Lens Fig. Matlab plot of aspheric function for given data Zemax output data
  • 26. Comparison of 2x2 element of side L and side R Left Side (L) Right Side (R)
  • 27. Comparison of 2x11 element of side L and side R Left Side (L) Right Side (R)
  • 28. Comparison of 5x6 element of side L and side R Left Side (L) Right Side (R)
  • 29. Comparison of 9x2 element of side L and side R Left Side (L) Right Side (R)
  • 30. Comparison of 9x11 element of side L and side R Left Side (L) Right Side (R)
  • 31. • Experimental results and conclusions 1. Experimental Setup. 2. Description of optical setup. 3. Experimental results comparison with simulation. 4. Conclusion. 5. Future Work
  • 34. Experimental results Measurement parameters – Pitch = 0.05mm Speed = 1mm/s Time elapsed = 28hrs (approx.) Fig. (a) shows contour display of intensity. (b) Intensity distribution of UV LED light at homogenization plane A photograph of actual UV light Intensity at homogenization plane
  • 35. Experimental results Comparison with Simulation Fig. (a) Cross-sectional intensity distribution at axis X = 0. Fig. (a) Cross-sectional intensity distribution at axis Y = 0. Experiment Simulation
  • 36. Conclusion • This work proposes a modification in the digital micro mirror device (DMD). Since, fabrication of homogenizers by laser micro-machining system is quite expensive to use and it is one-time fabrication only. Using molding method for the manufacturing of fly’s eye UV LED homogenizer is the cheapest way of manufacturing homogenizers. Once the homogenizer steel mold is fabricated, we can produce any number of homogenizers by using mold. • The UV light used by the micro mirror devices will become more collimated and flat top intensity distribution of UV light, hence the quality of micro-machining of any substance will improve significantly.
  • 37. Future Work • PDMS Microlens profile irregularities after Demolding process can be fixed by changing the fabricated mold design. • A different set of lens can be used to get more collimated light from UV LED that decreases intensity slope and make it more flat-top profile.
  • 38. Future Work • Better collimation angle can be achieved by using different set of aspherical lenses.

Editor's Notes

  1. Datafile downloaded from luminious website.
  2. Curing done describe
  3. where the optic axis is presumed to lie in the z direction, and {\displaystyle z(r)} is the sag—the z-component of the displacement of the surface from the vertex, at distance {\displaystyle r} from the axis. The coefficients {\displaystyle \alpha _{i}} describe the deviation of the surface from the axially symmetric quadric surface specified by {\displaystyle R} and {\displaystyle \kappa }.
  4. When a stage is moved to a position and then returned to its original position, some motion is lost due to the lead screw mechanism. This loss is known as backlash = 3um, running parallism = 10um. Resolution 2um/pulse. Positioning accuracy = 7um.
  5. Molding cheapest Dmd quality improve.