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Design and optimization of compact
freeform lens array for laser beam splitting
Milan Maksimovic
Focal -Vision and Optics,
Enschede, The Netherlands
Brussels, Belgium, 14 - 17 April 2014
2
Outline
• Introduction: free-form optics and beam shaping
• Motivation: laser beam multiplexing
• Design Method
• Design Examples: simulations results and analysis
• Concluding remarks
3
Introduction
• Freeform optics: no rotational invariance, surfaces with arbitrary shape and regular or
irregular global or local structure:
• enhanced flexibility in design,
• boost in optical performances,
• combining multiplefunctionalities into single component,
• simplifying complex optical systems by reducing element count,
• lowering costs in manufacturing,
• reducing stray-light
• easing system integration and assembly
• Laser beam shaping (splitting) to achieve parallelism
• Lens array archives this purpose by the geometrical aperture splitting using the pupil division by
individual lenslets residing within sub-apertures
• Other optical elements are used and needed to obtain functions such as beam focusing,
combining or collimating
4
Motivation: design of 1x laser diode to 3x
fibers coupler
• High-power LD (elliptical) beam splitting into 3 fibers with equalized energy per
channel
• System components: Individual lenses
• Collimatorlens
• Single focusing lens element per spot
• Manufacturing cost high (number of components)
• Assembly tolerances (for many elements) are critical
5
Element representation:
• Low order aspheric + specific aperture on input
• Low order aspheric lenslet in the focusing lens array
Design and optimization (using standard software packageZemax):
• Custom merit function using real ray coordinates: explicit specification of in-out
relationship per each channel (spot)
• Pupil sampling (grid) define sampling rays f0r merit function
• Multi-parameter optimization
• Local optimizer (DLS or OD):
-> Initial starting point critical !
• Free-form surface representation:  
2 2
2 2 2
( )
( , ) ,
1 1 ( )
i i
i
c x y
z x y w x y
Kc x y

  
  

where c=1/R is base curvature, K is base conic
constant, wi is weight in expansion and Φ is suitable
basis function in expansion
Compact beam splitter: design method
6
Compact beam splitter: design method
Compact beam splitter with regular lens array: 1x3 (left) and 1x 5 (right)
Optical layouts for: collimator (left), single lenslet (center) and 1x3 lens array (right).
Fixed input parameters (example):
• Object and image distance : 50mm
• Entrance pupil diameter: 30mm
• Rectangular aperture of 10x30 mm
• Lens array 10x10 mm,
(replicated in vertical direction)
Merit Function based on
real ray position @ image plane!
Pupil sampling grid defines input
ray position sampling !
7
Different pupil sampling grids used
to compute merit function
Fibonacci sampling grid:
• Deterministic
algorithm based on
Fibonacci spiral
• Uniform and isotropic
resolution
• Equal area
(contribution) per each
grid point
8
Compact design of 1x3 beam splitter
using regular lens array
Composite Fibonacci pupil sampling grid used in merit function , layout with rays
generated in the merit function, 3D model and multi-spot surface plot in the image
pane (left to right respectively).
9
Compact design of 1x3 beam splitter
using regular lens array
Surface sag map (left) and cross-section (right) of lens array surface
Optimization with radius and conic as variables :
-> R=-22.9954mm and K=-2.1314
10
Compact beam splitter design using
general freeform surface
Extended Polynomial surface representation
Surface sag map (left) and sag cross-section (right)
(Extended Polynomial surface after the optimization with 150 variables)
2 2
2 2 2
,
( )
( , )
1 1 ( )
m n
mn
m n
c x y
z x y c x y
Kc x y

 
  

11
Compact beam splitter design using
general freeform surface
Merit function vs. number of variables used in optimization
with different size of pupil sampling grids:
0 50 100 150
0.5
1
1.5
2
2.5
3
Number ofVariables
MeritFunction
Extended Polynomial Representation
17 points per segment
51 points per segment
153 points pr segment
12
Compact beam splitter design using
general freeform surface
Zernike surface representation :
Surface sag map (left) and sag cross-section (right) of Zernike surface after the
optimization with 37 variables
2 2
2
2 2 2
1...8 1..37
( )
( , ) ( , )
1 1 ( )
i
i j j
i j
c x y
z x y r A Z
Kc x y
  
 

  
  
 
13
Compact beam splitter design using
irregular lens array
Motivation/ Application: different power ratio per spot!
Beam splitter 1x3 design with irregular lens array: layout (left) and 3D model (right)
Surface intensity plot in the entrance pupil (left) and multi-spot surface intensity
plot in the image plane (right)
14
Compact beam splitter design using irregular
lens array: smoothing using image
processing technique
Surface sag map of irregular lens
array after smoothing
Sharp transitions removal:
Gaussian filter followed by Median filter
in the transition region (local smoothing!)
15
Compact beam splitter design using
irregular lens array: CAD model smoothing
CAD model post-processing
• heuristic approach
• CAD surface representation often implies less
accurate ray tracing!
• Iterative procedure: (Zemax->CAD->Zemax)
Example of successful design iteration:
16
Concluding remarks
• We demonstrated feasibility of freeform design of compact beam splitting element
that combines both functions of collimation and beam splitting into one (both regular
and irregular structure is possible)
• Design relaying on multi-parameter optimization + custom design merit function based
on real ray coordinates at target location works, but:
• Standard free-form surfaces often fail to produce design directly and with small number
of variables-> inefficient design process!
• Open questions: optimal free-form representation
• Pupil sampling method based on Fibonacci grid (highly structured grid and having
features usually associated with random grids) improves convergence in local
optimization procedure
• Designs often require post-processing for manufacturing constraints (smoothing)
• Application of local filtering techniques borrowed from image processing produce
smoothed versions of surfaces with discontinuities
• Possible applications of similar designs are in laser fiber coupling and off-axis multi-spot
generation where power splitting ratio can be arbitrarily predefined.
17
Thank you for the attention!

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Design and optimization of compact freeform lens array for laser beam splitting SPIE 9131 6 2014

  • 1. 1 Design and optimization of compact freeform lens array for laser beam splitting Milan Maksimovic Focal -Vision and Optics, Enschede, The Netherlands Brussels, Belgium, 14 - 17 April 2014
  • 2. 2 Outline • Introduction: free-form optics and beam shaping • Motivation: laser beam multiplexing • Design Method • Design Examples: simulations results and analysis • Concluding remarks
  • 3. 3 Introduction • Freeform optics: no rotational invariance, surfaces with arbitrary shape and regular or irregular global or local structure: • enhanced flexibility in design, • boost in optical performances, • combining multiplefunctionalities into single component, • simplifying complex optical systems by reducing element count, • lowering costs in manufacturing, • reducing stray-light • easing system integration and assembly • Laser beam shaping (splitting) to achieve parallelism • Lens array archives this purpose by the geometrical aperture splitting using the pupil division by individual lenslets residing within sub-apertures • Other optical elements are used and needed to obtain functions such as beam focusing, combining or collimating
  • 4. 4 Motivation: design of 1x laser diode to 3x fibers coupler • High-power LD (elliptical) beam splitting into 3 fibers with equalized energy per channel • System components: Individual lenses • Collimatorlens • Single focusing lens element per spot • Manufacturing cost high (number of components) • Assembly tolerances (for many elements) are critical
  • 5. 5 Element representation: • Low order aspheric + specific aperture on input • Low order aspheric lenslet in the focusing lens array Design and optimization (using standard software packageZemax): • Custom merit function using real ray coordinates: explicit specification of in-out relationship per each channel (spot) • Pupil sampling (grid) define sampling rays f0r merit function • Multi-parameter optimization • Local optimizer (DLS or OD): -> Initial starting point critical ! • Free-form surface representation:   2 2 2 2 2 ( ) ( , ) , 1 1 ( ) i i i c x y z x y w x y Kc x y         where c=1/R is base curvature, K is base conic constant, wi is weight in expansion and Φ is suitable basis function in expansion Compact beam splitter: design method
  • 6. 6 Compact beam splitter: design method Compact beam splitter with regular lens array: 1x3 (left) and 1x 5 (right) Optical layouts for: collimator (left), single lenslet (center) and 1x3 lens array (right). Fixed input parameters (example): • Object and image distance : 50mm • Entrance pupil diameter: 30mm • Rectangular aperture of 10x30 mm • Lens array 10x10 mm, (replicated in vertical direction) Merit Function based on real ray position @ image plane! Pupil sampling grid defines input ray position sampling !
  • 7. 7 Different pupil sampling grids used to compute merit function Fibonacci sampling grid: • Deterministic algorithm based on Fibonacci spiral • Uniform and isotropic resolution • Equal area (contribution) per each grid point
  • 8. 8 Compact design of 1x3 beam splitter using regular lens array Composite Fibonacci pupil sampling grid used in merit function , layout with rays generated in the merit function, 3D model and multi-spot surface plot in the image pane (left to right respectively).
  • 9. 9 Compact design of 1x3 beam splitter using regular lens array Surface sag map (left) and cross-section (right) of lens array surface Optimization with radius and conic as variables : -> R=-22.9954mm and K=-2.1314
  • 10. 10 Compact beam splitter design using general freeform surface Extended Polynomial surface representation Surface sag map (left) and sag cross-section (right) (Extended Polynomial surface after the optimization with 150 variables) 2 2 2 2 2 , ( ) ( , ) 1 1 ( ) m n mn m n c x y z x y c x y Kc x y       
  • 11. 11 Compact beam splitter design using general freeform surface Merit function vs. number of variables used in optimization with different size of pupil sampling grids: 0 50 100 150 0.5 1 1.5 2 2.5 3 Number ofVariables MeritFunction Extended Polynomial Representation 17 points per segment 51 points per segment 153 points pr segment
  • 12. 12 Compact beam splitter design using general freeform surface Zernike surface representation : Surface sag map (left) and sag cross-section (right) of Zernike surface after the optimization with 37 variables 2 2 2 2 2 2 1...8 1..37 ( ) ( , ) ( , ) 1 1 ( ) i i j j i j c x y z x y r A Z Kc x y              
  • 13. 13 Compact beam splitter design using irregular lens array Motivation/ Application: different power ratio per spot! Beam splitter 1x3 design with irregular lens array: layout (left) and 3D model (right) Surface intensity plot in the entrance pupil (left) and multi-spot surface intensity plot in the image plane (right)
  • 14. 14 Compact beam splitter design using irregular lens array: smoothing using image processing technique Surface sag map of irregular lens array after smoothing Sharp transitions removal: Gaussian filter followed by Median filter in the transition region (local smoothing!)
  • 15. 15 Compact beam splitter design using irregular lens array: CAD model smoothing CAD model post-processing • heuristic approach • CAD surface representation often implies less accurate ray tracing! • Iterative procedure: (Zemax->CAD->Zemax) Example of successful design iteration:
  • 16. 16 Concluding remarks • We demonstrated feasibility of freeform design of compact beam splitting element that combines both functions of collimation and beam splitting into one (both regular and irregular structure is possible) • Design relaying on multi-parameter optimization + custom design merit function based on real ray coordinates at target location works, but: • Standard free-form surfaces often fail to produce design directly and with small number of variables-> inefficient design process! • Open questions: optimal free-form representation • Pupil sampling method based on Fibonacci grid (highly structured grid and having features usually associated with random grids) improves convergence in local optimization procedure • Designs often require post-processing for manufacturing constraints (smoothing) • Application of local filtering techniques borrowed from image processing produce smoothed versions of surfaces with discontinuities • Possible applications of similar designs are in laser fiber coupling and off-axis multi-spot generation where power splitting ratio can be arbitrarily predefined.
  • 17. 17 Thank you for the attention!