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© Fraunhofer
STARTSYSTEMGENERIERUNG FÜRFREIFORMFLÄCHEN
25.11.2016Britta Satzer1, Herbert Gross1,2
(1) Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany(2) Institute of Applied Physics, Friedrich-Schiller-University Jena, Germany
KoSimO Status Seminar
© Fraunhofer Britta Satzer, 25.11.2016
Generation of starting configurations withfreeform surfaces – Outline
� Motivation
� Work on different generation methods for several system types
� 3D-SMS
� Introduction
� Implementation within complex optical systems
� Conclusion
� Summary and Outlook
© Fraunhofer Britta Satzer, 25.11.2016
Motivation - Typical design approach for complex optical systems
� Starting system
� From lens databases, patents, literature
� Formulation of the merit function
� Optimization
Final Design
Optimization
Starting System
© Fraunhofer Britta Satzer, 25.11.2016
Motivation - Design for freeform optical systems
� Only few starting designs available
� Higher variety of possible system geometries
Starting System
?Final Design
Optimization
© Fraunhofer Britta Satzer, 25.11.2016
Work on different generation methods- for several system types
Methods Types
Classical TMA
Gaussian Brackets Spectrometer
Conic confocal +Lokal Expansion
Monolith
Thin-componenttheory +Li and Cen
Scheimpflug
Korsch Calculation Modular Off-Axis
Wavefront mapping Zoom
3D-SMS Illumination
Ray mapping …
…
KoSimO
Y. Zhong, C. Liu, N. Fitzgerald,
C. Bösel, J. Hartung
���� Benchmark
© Fraunhofer Britta Satzer, 25.11.2016
Work on different generation methods- Implementations
Methods Ways of Implementation
Classical
Gaussian Brackets� Macro
Conic confocal +Lokal Expansion
� Macro
Thin-componenttheory +Li and Cen
� Method
Korsch Calculation ���� Analysis tool
Wavefront mapping ���� Matlab tool
3D-SMS ���� Matlab tool
Ray mapping ���� Numerical method
…
KoSimO
Y. Zhong, C. Liu, N. Fitzgerald,
Christoph Bösel, Johannes Hartung
KoSimO
© Fraunhofer Britta Satzer, 25.11.2016
� Method: Design of two lens surfaces for the ideal image of two fieldpoints developed by Prof. Miñano
� KoSimO: 3D-SMS for Scheimpflug system
3D-SMS Simultaneous Multiple Surface method - Introduction
Map of spotsize
Ref.: Satzer B., et.al., “Using the 3D-SMS for finding starting configurations in imaging systems with freeform surfaces“, SPIE Proc. Vol. 9626 (2015)
© Fraunhofer Britta Satzer, 25.11.2016
3D-SMS within complex optical systems- Approach
Start design with extended Zernike DLL
Final system
Optimization
Optics Studio
Rotational symmetric starting system, start parameter, incl. OPLs
Analytic surface representation: Zernike
3D-SMS
Data fit with Zernike
v
MATLAB
Lens surfaces as discrete point set
DDE -Link
© Fraunhofer Britta Satzer, 25.11.2016
3D-SMS within complex optical systems- Implementation
Optics Studio
Matlab
System
Raytracing
� Ray path in intermediate distances
� Conventional SMS calculation
� Optimizations on matching thecorrect optical path length (OPL)
� Ray path in intermediate distances
� Conventional SMS calculation
� Optimizations on matching thecorrect OPL
DDE - Link
ReversedSystem
© Fraunhofer Britta Satzer, 25.11.2016
-3.25E-003
-2.67E-003
-2.10E-003
-1.53E-003
-9.53E-004
-3.79E-004
1.95E-004
7.69E-004
1.34E-003
1.92E-003
2.49E-003
-3.10E-003
-2.56E-003
-2.02E-003
-1.47E-003
-9.32E-004
-3.89E-004
1.54E-004
6.97E-004
1.24E-003
1.78E-003
2.32E-003
3D-SMS within complex optical systems- Results
� Rotational symetric object and image planes
� Scheimpflug system
3.110��
�3.110��
2.510��
�3.510��
0 0
Surface Sag [mm]
© Fraunhofer Britta Satzer, 25.11.2016
3D-SMS within complex optical systems- Conclusions I
Pros:
� The positions of two object and image points can be calculated directly.
� Starting configurations for more than one field point can consider tilted object- and image planes in the starting design like Scheimpflug systems.
Cons:
� No algorithm known yet on using SMS for more than two field points for full ray bundle.
� Approach requires high optimization effort (surface fit and ray tracing in complex system), which make the approach time consuming and dependent on the success of the optimization.
� Best positions are limited to close to the pupil plane.
© Fraunhofer Britta Satzer, 25.11.2016
3D-SMS within complex optical systems- Conclusions II
General:
� Implementation in complex systems causes inaccuracies, since the path of the light is not reversible due to higher order aberrations. This has been treated with optimizations routines.
� Generally good starting systems have only few variables to allow better optimization. Thus the fitted freeform terms should be selected to a minimum
© Fraunhofer Britta Satzer, 25.11.2016
Summary and Outlook
� Implementation of 8 different methods for generation of startingconfigartions
� Application to several system types
Outlook:
� Finalization of the method implementation
� Benchmark
� Systematic for design of freeform lenses