Advanced light management techniques for building integrated PV (BIPV)

Size: px
Start display at page:

Download "Advanced light management techniques for building integrated PV (BIPV)"

Transcription

1 Advanced light management techniques for building integrated PV (BIPV) A. Ingenito, J. C. O. Lizcano, O. Isabella, M. Zeman Delft University of Technology

2 Advanced light management Roadmap for decreasing costs of c-si PV Decrease wafer cell costs [1] Wafer accounts for more than 50% of the cell costs [2] Customized PV products [1] Building integrated PV (BIPV) combining building elements and PV functionality Oskomera Solar [1,3] Roadmap [1] International Technology Roadmap for Photovoltaic (ITRPV), (2013) [2] A. Goodrich et al. SOLMAT 114, (2013) [3] Predictions for the Solar Industry in 2014, IHS Whitepaper (2013) 2

3 Advanced light management in c-si Experimental demonstration of upper limit 4n 2 absorption enhancement [1] Front nano-texture (RIE) 2 µm DBR Ag (ref.) Bulk c-si 20 μm Thermal SiO 2 DBR A Si [-] μm Textured BS 2 µm Wavelength [nm] [1] A. Ingenito, O. Isabella, M. Zeman, ACS Photonics, 1, 3 (2014) 3

4 Advanced light management in c-si IBC c-si solar cells IBC structure EQE [-] V OC (mv) 635 J SC (ma/cm 2 ) 40.5 FF (%) R [-] 280 μm 0.2 η (%) Front side Wavelength [nm] A. Ingenito, O. Isabella, M. Zeman. Progress in Photovoltaics, DOI: /pip.2606 (2015) 4

5 Advanced light management in c-si Black IBC c-si solar cells for high yield and BIPV applications [1] Black modules are highly requested for residential PV [2] [1] H. Savin, P. Repo, G. von Gastrow, P. Ortega, E. Calle, M. Garín, Nature Nanotechnology, DOI: /nnano (2015) [2] Paul de Jong, Exasun, BJ-BC workshop, Freiburg, (2015) 5

6 Advanced light management Roadmap for decreasing costs of c-si PV Decrease wafer cell costs [1] Wafer accounts for more than 50% of the cell costs [2] Customized PV products [1] Building integrated PV (BIPV) combining building elements and PV functionality Oskomera Solar [1,3] Roadmap [1] International Technology Roadmap for Photovoltaic (ITRPV), (2013) [2] A. Goodrich et al. SOLMAT 114, (2013) [3] Predictions for the Solar Industry in 2014, IHS Whitepaper (2013) 6

7 Optical filters (OF) as coloured coatings OF for front and/or back side coloured PV Glass EVA x 10 Glass EVA 10 x ARC ARC Emitter c-si Emitter c-si c-si BSF 10 x BSF Rear coating EVA Al Al Glass 7

8 OF s requirements and materials Exploits interference effect Based on pairs of dielectric thin-films Stronger effect with high/low refractive refractive index mismatch Several materials can be used, among the others: MgF 2 SiO 2 TiO 2 Si x N y a-si:h SiO 2 Si x N y x pairs Features Non absorbing materials in spectral range of interest o [ ] nm for Front side o [ ] nm for Back side Reflectance above 80% at desired wavelength Substrate (Glass or wafer) Protected by glass/encapsulant 8

9 OF s optical modelling 1,00 0,90 0,80 0,70 0,60 0,50 0,40 0,30 0,20 0, D Ray tracing* 0, Reflectance profile 3. Color Coordinates SunRay software by dr. R. Santbergen 9

10 Selected colours for validation SiO 2 = 100 nm Si x N y = 100 nm SiO 2 = 90 nm Si x N y = 100 nm SiO 2 = 40 nm Si x N y = 110 nm PE-CVD 10

11 Optical filters (OF) as coloured coatings OF for front and/or back side coloured PV Glass EVA x 10 Glass EVA 10 x ARC ARC Emitter c-si Emitter c-si c-si BSF 10 x BSF Rear coating EVA Al Al Glass 11

12 Colour matrix (OF on glass and c-si solar cell) 10 x Glass EVA ARC EQE [-] ma/cm 2 Standard ARC (NO-OF) Coloured Wavelength [nm] 12

13 Colour matrix (OF on glass and c-si solar cell) Angular resilience 10 x Glass EVA ARC 13

14 Colour matrix (OF on c-si solar cell in glass) 10 x Glass EVA ARC EQE [-] ma/cm 2 Standard ARC (NO-OF) Coloured Wavelength [nm] 14

15 Colour matrix (OF on c-si solar cell in glass) Angular resilience 10 x Glass EVA ARC 15

16 Passive thermal control [1] for BIPV Preliminary study Glass +20 pairs EVA ARC Emitter c-si BSF Al Potential for Passively reducing module temperature Concurrently combining colour and thermal control [1] A. P. Raman, et al., Nature, 515, (2014) 16

17 Optical filters (OF) as coloured coatings OF for front and/or back side coloured PV Glass EVA x 10 Glass EVA 10 x ARC ARC Emitter c-si Emitter c-si c-si BSF 10 x BSF Rear coating EVA Al Al Glass 17

18 Distributed Bragg Reflector (DBR) DBR can act as both back reflector (BRs) and OF High R at SiO 2 / Si interface in the weak absorption region if Si 1.0 PCB 0.8 R Sim [-] Region of weak absorption in c-si DBR λ B Wavelength [nm] A. Ingenito, O. Isabella, M. Zeman, ACS Photonics, 1, 3 (2014) 18

19 Fabrication of DBR on textured surfaces DBR R, T [-] R 0.2 T Wavelength [nm] Co-depostion of 6 x a-si:h (80 nm) / a-sin x :H (180 nm) 19

20 Fabrication of DBR on textured surfaces DBR R, T [-] R? 0.2 R T T DBR Wavelength [nm] Co-depostion of 6 x a-si:h (80 nm) / a-sin x :H (180 nm) 20

21 DBR optimization for textured surface =54.7 X= Y*sin (90 - θ) = Y*0.57 A. Ingenito, S.L. Luxembourg, P. Spinelli, J. Liu, J. C. O. Lizcano, A. Weeber, O. Isabella, M. Zeman, IEEE JPV, accepted for publication (2015) 21

22 DBR optimization for textured surface Influence of scaling factor on A Si ma / cm A Si [-] DBR 38.1 ma/cm Wavelength [nm] Wavelength [nm] A. Ingenito, S.L. Luxembourg, P. Spinelli, J. Liu, J. C. O. Lizcano, A. Weeber, O. Isabella, M. Zeman, IEEE JPV, accepted for publication (2015) 22

23 DBR optimization for textured surface Influence of scaling factor on λ B at DBR / air interface R DBR air [-] Light 0.2 DBR Wavelength [nm] 23

24 DBR (OF) as coloured coatings Application in glass/glass modules Coloured cell [1] Coloured module n-pasha cell [2] [1] A. Ingenito, S.L. Luxembourg, P. Spinelli, J. Liu, J. C. O. Lizcano, A. Weeber, O. Isabella, M. Zeman, IEEE JPV, accepted for publication (2015) [2] I. G. Romijn, A. Gutjahr, D. Saynova, J. Anker, E.J Kossen, K. Tool. Photovoltaics International, 2013, vol. 20. pp

25 Advanced light management for BIPV Experimental demonstration of advanced light management techniques for absorption enhancement in thin c-si absorbers Application of advanced light management for black IBC c-si solar cells with efficiency of 19.8% EQE [-] R [-] Design of OFs as colour-tuning coatings for front and/or rear side coloured PV Model validation Design and optical simulations of DBR on textured surfaces Concurrent colour and thermal control (on-going) Wavelength [nm] 25

26 Thank you! Acknowledgments: Martijn Tijssen Martijn van Sebille Stefan Luxembourg Pierpaolo Spinelli Funding: Agentschap NL

27 Outline Roadmap for decreasing the cost of c-si PV module Advanced light management techniques as possible solution to decrease LCOE Thin c-si solar cells Customized products as Building integrated PV Conclusions 2

28 DBR optimization for textured surface Ray tracing simulations Parameter space: a-si:h [40:10:140] nm a-sin x :H [70:10:240] nm Si SiO 2 DBR DBR = 6 x (a-si:h /a-sin x :H) [1] a-sin x :H [nm] J PH-T = ma/cm 2 [2] Textured a-si:h [nm] J ph T [ma/cm 2 ] [1] A. Ingenito, O. Isabella, M. Zeman, ACS Photonics, 1, 3, (2014) [2] J.C.O. Lizcano, MSC thesis, Optic Filters for BIPV applications (2014) 20

29 Color resilience against angle of incidence 13

30 Device level color matrix 14

31 Performance of a cell under colored glass Parameter Standard Green Yellow J PH [ma/cm 2 ] V OC [V] FF [-] iη[%]

32 Color resilience against angle of incidence 16

33 Color resilience against angle of incidence 17

34 DBR optimization for textured surface Losses analysis 6x a-si:h (80 nm) / a-sin x :H (180 nm) Max 6x a-si:h (120 nm) / a-sin x :H (270 nm) Min 38

35 DBR optimization for textured surface Influence of scaling factor on R and T R [-] DBR T [-] Wavelength [nm] Wavelength [nm] From DBR = 6 x a-si:h (80 nm) / a-sin x :H (180 nm) to scaled thicknesses A. Ingenito, S.L. Luxembourg, P. Spinelli, J. Liu, J. C. O. Lizcano, A. Weeber, O. Isabella, M. Zeman, IEEE JPV, accepted for publication (2015) 34

36 DBR optimization for textured surface Scaling factor = 1 Scaling factor = 1.5 A. Ingenito, S.L. Luxembourg, P. Spinelli, J. Liu, J. C. O. Lizcano, A. Weeber, O. Isabella, M. Zeman, IEEE JPV, accepted for publication (2015) 36

37 DBR optimization for textured surface Transmittance of optimized DBR T [-] 0.6 Measured 1.0 Measured 1.5 Sim? Wavelength [nm] DBR = 6 x a-si:h (80 nm) / a-sin x :H (180 nm) scaled of

38 Effect of Defect Removal Etching on surface morphology After DRE in TMAH 1% A F /A Proj =4.6 A F /A Proj = 2.7 Initial A F /A Proj = s 1 µm 30 s 1 µm A F /A Proj =2.1 A F /A Proj =1.6 0 s 1 µm Mask less RIE 45 s 1 µm 60 s 1 µm A. Ingenito, O. Isabella, M. Zeman, Progress in Photovoltaics, DOI: /pip.2606 (2014) 4

39 Effect of Defect Removal Etching TEM* analysis 0 s 15 s 30 s Damaged region 200 nm 200 nm 200 nm *TEM taken at 12

40 Effect of Defect Removal Etching QSSPC analysis 10-2 SiO 2 (a) Al 2 O 3 (b) 10-3 eff [s] n [cm -3 ] n [cm -3 ]

41 MST-textured* IBC c-si solar cell SiN Recombination MST-T Std Long wavelength scattering EQE [-] V OC (mv) J SC (ma/cm 2 ) FF (%) R [-] 0.2 η (%) Wavelength [nm] 30 s DRE 5 µm 10 µm A. Ingenito, O. Isabella, M. Zeman, Progress in Photovoltaics, DOI: /pip.2606 (2014) 17

42 Advanced light management in c-si 4n 2 absorption enhancement [1] Light R Light in-coupling R = 0 Light scattering Absorber (n) R b Ideally diffused light scattering [1] E.Yablonovitch J. Opt. Soc. Am. 72, Efficient back reflector R b = 1 4

Appendix A: Comparison of ray-tracing with Birandy and Sunrays programs

Appendix A: Comparison of ray-tracing with Birandy and Sunrays programs Comparison of ray-tracing with Birandy and Sunrays programs Appendix A: Comparison of ray-tracing with Birandy and Sunrays programs Comparison of ray-tracing programs Birandy and Sunrays In order to check

More information

Manual for solar cell optical simulation software: GENPRO4

Manual for solar cell optical simulation software: GENPRO4 Manual for solar cell optical simulation software: GENPRO4 Rudi Santbergen (r.santbergen@tudelft.nl) Photovoltaic Materials and Devices Delft University of Technology Version: February 2016 0. Introduction

More information

Light management in thin-film Si solar cells. Hitoshi Sai

Light management in thin-film Si solar cells. Hitoshi Sai 9th Aug. 2011 University of Southampton Light management in thin-film Si solar cells Hitoshi Sai Research Center for Photovoltaic Technology (RCPVT) National Institute of Advance Industrial Science & Technology

More information

Highly Transparent and Highly Passivating Silicon Nitride for Solar Cells. Yimao Wan The Australian National University (ANU) 23/10/2014

Highly Transparent and Highly Passivating Silicon Nitride for Solar Cells. Yimao Wan The Australian National University (ANU) 23/10/2014 Highly Transparent and Highly Passivating Silicon Nitride for Solar Cells Yimao Wan The Australian National University (ANU) 23/10/2014 2 Outline Motivation Reviews of SiNx properties Process development

More information

Thin silicon solar cells with SiО х /SiN x Bragg mirror rear surface reflector

Thin silicon solar cells with SiО х /SiN x Bragg mirror rear surface reflector PACS 42.79.Bh, 78.66.Db, 84.6.Jt Thin silicon solar cells with О х / x Bragg mirror rear surface reflector I.I. Ivanov 1, T.V. ychyporuk 2, V.A. Skryshevsky 1, M. Lemiti 2 1 Taras Shevchenko Kyiv ational

More information

Theoretical Investigation of Light Trapping in Polycrystalline Silicon Thin-Film Solar Cells

Theoretical Investigation of Light Trapping in Polycrystalline Silicon Thin-Film Solar Cells Available online at www.sciencedirect.com Energy Procedia 25 (2012 ) 43 49 PV Asia Pacific Conference 2011 Theoretical Investigation of Light Trapping in Polycrystalline Silicon Thin-Film Solar Cells Cangming

More information

The Role of Simulation in Photovoltaics: From Solar Cells To Arrays. Ricardo Borges, Kurt Mueller, and Nelson Braga Synopsys, Inc.

The Role of Simulation in Photovoltaics: From Solar Cells To Arrays. Ricardo Borges, Kurt Mueller, and Nelson Braga Synopsys, Inc. The Role of Simulation in Photovoltaics: From Solar Cells To Arrays Ricardo Borges, Kurt Mueller, and Nelson Braga Synopsys, Inc. 1 PV System Challenges Improving PV efficiency Optimizing for design performance

More information

Decoupled front/back dielectric textures for flat ultra-thin c-si solar cells

Decoupled front/back dielectric textures for flat ultra-thin c-si solar cells Delft University of Technology Decoupled front/back dielectric textures for flat ultra-thin c-si solar cells Isabella, Olindo; Vismara, Robin; Ingenito, Andrea; Rezaei, Nasim; Zeman, Miro DOI 10.1364/OE.24.00A708

More information

CHARACTERIZATION OF BIFACIAL SILICON SOLAR CELLS AND MODULES: A NEW STEP

CHARACTERIZATION OF BIFACIAL SILICON SOLAR CELLS AND MODULES: A NEW STEP CHARACTERIZATION OF BIFACIAL SILICON SOLAR CELLS AND MODULES: A NEW STEP C. Duran, P. Hering, T. Buck, K. Peter International Solar Energy Research Center, ISC Konstanz ev., Rudolf Diesel Str 15, D-78467,

More information

Broadband and Wide Angle Antireflection Coatings for Solar Cell Applications Dr. Mohammed A. Hussein, Dr. Ali H. Al-Hamdani, Nibras S.

Broadband and Wide Angle Antireflection Coatings for Solar Cell Applications Dr. Mohammed A. Hussein, Dr. Ali H. Al-Hamdani, Nibras S. Broadband and Wide Angle Antireflection Coatings for Solar Cell Applications Dr. Mohammed A. Hussein University of Technology Dr. Ali H. Al-Hamdani Energy and Renewable Energy Technology Center/ University

More information

Laser Applications for Photovoltaics Crystalline and Thin Film Technologies

Laser Applications for Photovoltaics Crystalline and Thin Film Technologies LASERS & MATERIAL PROCESSING I OPTICAL SYSTEMS I INDUSTRIAL METROLOGY I TRAFFIC SOLUTIONS I DEFENSE & CIVIL SYSTEMS Laser Applications for Photovoltaics Crystalline and Thin Film Technologies Back contact

More information

Laser Applications for Photovoltaics Crystalline and Thin Film Technologies

Laser Applications for Photovoltaics Crystalline and Thin Film Technologies LASERS & MATERIAL PROCESSING I OPTICAL SYSTEMS I INDUSTRIAL METROLOGY I TRAFFIC SOLUTIONS I DEFENSE & CIVIL SYSTEMS Laser Applications for Photovoltaics Crystalline and Thin Film Technologies Back contact

More information

The Effect of Electrical Properties by Texturing Surface on GaAs Solar Cell Efficiency

The Effect of Electrical Properties by Texturing Surface on GaAs Solar Cell Efficiency American J. of Engineering and Applied Sciences 2 (1):189-193, 29 ISSN 1941-72 29 Science Publications The Effect of Electrical Properties by Texturing Surface on GaAs Solar Cell Efficiency 1 H. Abdullah,

More information

Comparison of periodic and random structures for scattering in thinfilm microcrystalline silicon solar cells

Comparison of periodic and random structures for scattering in thinfilm microcrystalline silicon solar cells Comparison of periodic and random structures for scattering in thinfilm microcrystalline silicon solar cells M. Peters a,b, K. Forberich a, C. Battaglia c, A. G. Aberle a, B. Bläsi b a Solar Energy Research

More information

Compact Multilayer Film Structure for Angle Insensitive. Color Filtering

Compact Multilayer Film Structure for Angle Insensitive. Color Filtering 1 Compact Multilayer Film Structure for Angle Insensitive Color Filtering Chenying Yang, Weidong Shen*, Yueguang Zhang, Kan Li, Xu Fang, Xing Zhang, and Xu Liu * E-mail: adongszju@hotmail.com

More information

High spatial resolution measurement of volume holographic gratings

High spatial resolution measurement of volume holographic gratings High spatial resolution measurement of volume holographic gratings Gregory J. Steckman, Frank Havermeyer Ondax, Inc., 8 E. Duarte Rd., Monrovia, CA, USA 9116 ABSTRACT The conventional approach for measuring

More information

OPTOELECTRONIC DESIGN OF MULTIJUNCTION WIRE-ARRAY SOLAR CELLS

OPTOELECTRONIC DESIGN OF MULTIJUNCTION WIRE-ARRAY SOLAR CELLS OPTOELECTRONIC DESIGN OF MULTIJUNCTION WIRE-ARRAY SOLAR CELLS Daniel B. Turner-Evans 1, Michael D. Kelzenberg 1, Chris T. Chen 1, Emily C. Warmann 1, Adele C. Tamboli 1, and Harry A. Atwater 1,2 1 Thomas

More information

Length Scale Dependence of Periodic Textures for Photoabsorption Enhancement in Ultra-thin Silicon Foils and Thick Wafers

Length Scale Dependence of Periodic Textures for Photoabsorption Enhancement in Ultra-thin Silicon Foils and Thick Wafers Length Scale Dependence of Periodic Textures for Photoabsorption Enhancement in Ultra-thin Silicon Foils and Thick Wafers K Kumar 1, A Khalatpour 2, G Liu 1, J Nogami 1* and N P Kherani 1, 2 1 Department

More information

Holographic Elements in Solar Concentrator and Collection Systems

Holographic Elements in Solar Concentrator and Collection Systems Holographic Elements in Solar Concentrator and Collection Systems Raymond K. Kostuk,2, Jose Castro, Brian Myer 2, Deming Zhang and Glenn Rosenberg 3 Electrical and Computer Engineering, Department University

More information

POLYHEDRAL SPECULAR REFLECTOR

POLYHEDRAL SPECULAR REFLECTOR 32 C h a p t e r 3 POLYHEDRAL SPECULAR REFLECTOR The goal of the Full Spectrum Photovoltaics Project was to design and prototype a 50% module efficiency photovoltaic system. Of the three designs we initially

More information

Available online at ScienceDirect. Energy Procedia 92 (2016 )

Available online at  ScienceDirect. Energy Procedia 92 (2016 ) Available online at www.sciencedirect.com ScienceDirect Energy Procedia 92 (2016 ) 109 115 6th International Conference on Silicon Photovoltaics, SiliconPV 2016 Simulation-based efficiency gain analysis

More information

Agilent Cary Universal Measurement Spectrophotometer (UMS)

Agilent Cary Universal Measurement Spectrophotometer (UMS) Agilent Cary Universal Measurement Spectrophotometer (UMS) See what you ve been missing Date: 13 th May 2013 TRAVIS BURT UV-VIS-NIR PRODUCT MANAGER AGILENT TECHNOLOGIES 1 Agenda Introducing the Cary 7000

More information

T-Solar Overview. * Patent-pending

T-Solar Overview. * Patent-pending T-Solar T-Solar Overview The T-Solar system combines our best photovoltaic measurement technology into a system designed specifically for measuring textured samples. Based on the established M-2000 rotating

More information

RAPID CALCULATION OF THE BACKSHEET COUPLING GAIN USING RAY GROUPS

RAPID CALCULATION OF THE BACKSHEET COUPLING GAIN USING RAY GROUPS RAPID CALCULATION OF THE BACKSHEET COUPLING GAIN USING RAY GROUPS Andrea Pfreundt, Max Mittag, Martin Heinrich, Ulrich Eitner Fraunhofer Institute for Solar Energy Systems ISE Heidenhofstraße 2, 79110

More information

DETAILED MODELING OF COMPLEX BIPV SYSTEMS

DETAILED MODELING OF COMPLEX BIPV SYSTEMS DETAILED MODELING OF COMPLEX BIPV SYSTEMS Johannes Eisenlohr, Wendelin Sprenger, Helen Rose Wilson, Tilmann E. Kuhn PVPMC 2016 Freiburg, October 25 th Fraunhofer Institute for Solar Energy Systems ISE

More information

Texturing industrial multicrystalline silicon solar cells

Texturing industrial multicrystalline silicon solar cells Solar Energy 76 (2004) 277 283 www.elsevier.com/locate/solener Texturing industrial multicrystalline silicon solar cells D.H. Macdonald a, *, A. Cuevas a, M.J. Kerr a, C. Samundsett a, D. Ruby b, S. Winderbaum

More information

Presented at the 32nd European PV Solar Energy Conference and Exhibition, June 2016, Munich, Germany

Presented at the 32nd European PV Solar Energy Conference and Exhibition, June 2016, Munich, Germany Presented at the 32nd European PV Solar Energy Conference and Exhibition, - June 16, Munich, Germany GENUINE BIFACIAL SIMULATION AND OPTIMIZATION OF AN MC-SILICON PERC SOLAR CELL Nico Wöhrle, Aina Alapont

More information

Thin film solar cell simulations with FDTD

Thin film solar cell simulations with FDTD Thin film solar cell simulations with FDTD Matthew Mishrikey, Prof. Ch. Hafner (IFH) Dr. P. Losio (Oerlikon Solar) 5 th Workshop on Numerical Methods for Optical Nano Structures July 7 th, 2009 Problem

More information

Chapter 7. Widely Tunable Monolithic Laser Diodes

Chapter 7. Widely Tunable Monolithic Laser Diodes Chapter 7 Widely Tunable Monolithic Laser Diodes We have seen in Chapters 4 and 5 that the continuous tuning range λ is limited by λ/λ n/n g, where n is the index change and n g the group index of the

More information

A graphical user interface for multivariable analysis of silicon solar cells using scripted PC1D simulations

A graphical user interface for multivariable analysis of silicon solar cells using scripted PC1D simulations Available online at www.sciencedirect.com ScienceDirect Energy Procedia 38 (2013 ) 72 79 SiliconPV: March 25-27, 2013, Hamelin, Germany A graphical user interface for multivariable analysis of silicon

More information

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics

More information

Enhanced light absorption in thin film silicon solar cells with Fourier-series based periodic nanostructures

Enhanced light absorption in thin film silicon solar cells with Fourier-series based periodic nanostructures Enhanced light absorption in thin film silicon solar cells with Fourier-series based periodic nanostructures Xiaowei Guo, 1,* Dashuai Wang, 1 Bang Liu, 1 Shaorong Li, 1 and Xing Sheng 2 1 School of optoelectronic

More information

Microstructured surface design for omnidirectional antireflection coatings on solar cells

Microstructured surface design for omnidirectional antireflection coatings on solar cells JOURNAL OF APPLIED PHYSICS 102, 103105 2007 Microstructured surface design for omnidirectional antireflection coatings on solar cells Weidong Zhou, a Meng Tao, b Li Chen, and Hongjun Yang Department of

More information

Structural color printing based on plasmonic. metasurfaces of perfect light absorption

Structural color printing based on plasmonic. metasurfaces of perfect light absorption Supplementary Information Structural color printing based on plasmonic metasurfaces of perfect light absorption Fei Cheng 1, Jie Gao 1,*, Ting S. Luk 2, and Xiaodong Yang 1,* 1 Department of Mechanical

More information

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics

More information

Innovative Photon Management for Smart Control of Light. Shawn-Yu Lin Device Thrust Leader RPI Constellation Professor (The Future-Chips)

Innovative Photon Management for Smart Control of Light. Shawn-Yu Lin Device Thrust Leader RPI Constellation Professor (The Future-Chips) Innovative Photon Management for Smart Control of Light Shawn-Yu Lin Device Thrust Leader RPI Constellation Professor (The Future-Chips) 1 Light, Visual Experience & Innovation Sun light Vacuumtube technology

More information

Session 1B Transparent Materials

Session 1B Transparent Materials Session 1B Transparent Materials Andrew Martin UPenn, February 2014 2014 J.A. Woollam Co., Inc. www.jawoollam.com 1 Overview Transparent substrates & films Cauchy equation Common complexities Evaluating,

More information

Textbook Reference: Physics (Wilson, Buffa, Lou): Chapter 24

Textbook Reference: Physics (Wilson, Buffa, Lou): Chapter 24 AP Physics-B Physical Optics Introduction: We have seen that the reflection and refraction of light can be understood in terms of both rays and wave fronts of light. Light rays are quite compatible with

More information

ScienceDirect. The multi-busbar design: an overview

ScienceDirect. The multi-busbar design: an overview Erschienen in: Energy Procedia ; 43 (2013). - S. 86-92 Available online at www.sciencedirect.com ScienceDirect Energy Procedia 43 (2013 ) 86 92 4 th Workshop on Metallization for Crystalline Silicon Solar

More information

6-1 LECTURE #6: OPTICAL PROPERTIES OF SOLIDS. Basic question: How do solids interact with light? The answers are linked to:

6-1 LECTURE #6: OPTICAL PROPERTIES OF SOLIDS. Basic question: How do solids interact with light? The answers are linked to: LECTURE #6: OPTICAL PROPERTIES OF SOLIDS Basic question: How do solids interact with light? The answers are linked to: Properties of light inside a solid Mechanisms behind light reflection, absorption

More information

Unit 5.C Physical Optics Essential Fundamentals of Physical Optics

Unit 5.C Physical Optics Essential Fundamentals of Physical Optics Unit 5.C Physical Optics Essential Fundamentals of Physical Optics Early Booklet E.C.: + 1 Unit 5.C Hwk. Pts.: / 25 Unit 5.C Lab Pts.: / 20 Late, Incomplete, No Work, No Units Fees? Y / N 1. Light reflects

More information

Fiber Optic Communication Systems. Unit-03: Properties of Light. https://sites.google.com/a/faculty.muet.edu.pk/abdullatif

Fiber Optic Communication Systems. Unit-03: Properties of Light. https://sites.google.com/a/faculty.muet.edu.pk/abdullatif Unit-03: Properties of Light https://sites.google.com/a/faculty.muet.edu.pk/abdullatif Department of Telecommunication, MUET UET Jamshoro 1 Refractive index Department of Telecommunication, MUET UET Jamshoro

More information

Design of wideband graded-index antireflection coatings at oblique light incidence

Design of wideband graded-index antireflection coatings at oblique light incidence Design of wideband graded-index antireflection coatings at oblique light incidence Zhang Jun-Chao( ) a)b), Fang Ming( ) a), Jin Yun-Xia( ) a), and He Hong-Bo( ) a) a) Key Laboratory of Material Science

More information

MODELING AND SIMULATION OF OPTICAL CHARACTERISTICS IN A TEXTURED A-SI THIN FILM SOLAR CELL USING THE TRANSFER MATRIX METHOD

MODELING AND SIMULATION OF OPTICAL CHARACTERISTICS IN A TEXTURED A-SI THIN FILM SOLAR CELL USING THE TRANSFER MATRIX METHOD Annals of the Academy of Romanian Scientists Series on Science and Technology of Information ISSN 2066-8562 Volume 10, Number 1/2017 15 MODELING AND SIMULATION OF OPTICAL CHARACTERISTICS IN A TEXTURED

More information

College Physics B - PHY2054C

College Physics B - PHY2054C Young College - PHY2054C Wave Optics: 10/29/2014 My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building Outline Young 1 2 3 Young 4 5 Assume a thin soap film rests on a flat glass surface. Young Young

More information

Quokka version 2: selective surface doping, luminescence. modeling and data fitting

Quokka version 2: selective surface doping, luminescence. modeling and data fitting Quokka version 2: selective surface doping, luminescence modeling and data fitting Andreas Fell 1 *, Keith R. McIntosh 2, Malcolm Abbott 2, Daniel Walter 1 1 Australian National University, Canberra, Australia

More information

Announcements. Final exam day events (Friday, May 12, 10:00am to 12:00pm)

Announcements. Final exam day events (Friday, May 12, 10:00am to 12:00pm) Announcements Final exam day events (Friday, May 12, 10:00am to 12:00pm) 50-point multiple choice end-material test (covering material from chapters 33-36). (You get a free 8-point question!) 200 point

More information

LECTURE 13 THIN FILM INTERFERENCE. Instructor: Kazumi Tolich

LECTURE 13 THIN FILM INTERFERENCE. Instructor: Kazumi Tolich LECTURE 13 THIN FILM INTERFERENCE Instructor: Kazumi Tolich Lecture 13 2 17.4 Thin film interference Interference of reflected light waves Thin films of air The colors of soap bubbles and oil slicks 17.4

More information

Simulating Nanoscale Optics in Photovoltaics with the S-Matrix Method. Dalton Chaffee, Xufeng Wang, Peter Bermel

Simulating Nanoscale Optics in Photovoltaics with the S-Matrix Method. Dalton Chaffee, Xufeng Wang, Peter Bermel ABSTRACT Simulating Nanoscale Optics in Photovoltaics with the S-Matrix Method Dalton Chaffee, Xufeng Wang, Peter Bermel In the push to build high-efficiency solar cells with less materials, thin-film

More information

Pasadena, CA USA ABSTRACT

Pasadena, CA USA ABSTRACT Silicon Solar Cell Light-Trapping Using Defect Mode Photonic Crystals Kelsey A. Whitesell* a, Dennis M. Callahan a, Harry Atwater a a Thomas J. Watson Lab. of Applied Physics, MS 8-95, California Institute

More information

Chapter 2: Wave Optics

Chapter 2: Wave Optics Chapter : Wave Optics P-1. We can write a plane wave with the z axis taken in the direction of the wave vector k as u(,) r t Acos tkzarg( A) As c /, T 1/ and k / we can rewrite the plane wave as t z u(,)

More information

Optimal Design of Graded Refractive Index Profile for Broadband Omnidirectional Antireflection Coatings Using Genetic Programming

Optimal Design of Graded Refractive Index Profile for Broadband Omnidirectional Antireflection Coatings Using Genetic Programming Progress In Electromagnetics Research, Vol. 145, 39 48, 2014 Optimal Design of Graded Refractive Index Profile for Broadband Omnidirectional Antireflection Coatings Using Genetic Programming Yongxiang

More information

HYPERSPECTRAL IMAGING THIN FILM APPLICATIONS. Dr. Wulf Grählert /

HYPERSPECTRAL IMAGING THIN FILM APPLICATIONS. Dr. Wulf Grählert / Dr. Wulf Grählert +49 351 / 83391 3406 wulf.graehlert@iws.fraunhofer.de Motivation Coating processes: thin film application process stability What s about Monitoring? Random sampling? Real time analysis?

More information

Microstructured anti-reflection surface design for the omni-directional solar cells

Microstructured anti-reflection surface design for the omni-directional solar cells Microstructured anti-reflection surface design for the omni-directional solar cells Li Chen, Hongjun Yang, Men Tao and Weidong Zhou Department of Electrical Engineering, NanoFAB Center, University of Texas

More information

Diffraction Efficiency

Diffraction Efficiency Diffraction Efficiency Turan Erdogan Gratings are based on diffraction and interference: Diffraction gratings can be understood using the optical principles of diffraction and interference. When light

More information

Physics 202, Lecture 23

Physics 202, Lecture 23 Physics 202, Lecture 23 Today s Topics Lights and Laws of Geometric Optics Nature of Light Reflection and Refraction Law of Reflection Law of Refraction Index of Reflection, Snell s Law Total Internal

More information

Polarizing properties of embedded symmetric trilayer stacks under conditions of frustrated total internal reflection

Polarizing properties of embedded symmetric trilayer stacks under conditions of frustrated total internal reflection University of New Orleans ScholarWorks@UNO Electrical Engineering Faculty Publications Department of Electrical Engineering 3-1-2006 Polarizing properties of embedded symmetric trilayer stacks under conditions

More information

Geant4 Studies for the HPD-PET scintillators

Geant4 Studies for the HPD-PET scintillators F. Ciocia, a A. Braem, b E. Chesi, b, a1 C. Joram, b L. Lagamba, a E. Nappi, a J. Séguinot, b I. Vilardi a and P. Weilhammer b a Physics Dept. and INFN Section of Bari, Via Orabona 4, Bari, Italy b CERN

More information

Light and Electromagnetic Waves. Honors Physics

Light and Electromagnetic Waves. Honors Physics Light and Electromagnetic Waves Honors Physics Electromagnetic Waves EM waves are a result of accelerated charges and disturbances in electric and magnetic fields (Radio wave example here) As electrons

More information

Specification of Thin Film Thickness Measuring Equipment

Specification of Thin Film Thickness Measuring Equipment of Thin Film Thickness Measuring Equipment A. Application: Major application is for solar cell thin film thickness measurement for films such as CIGS, CdS, ITO, ZnO etc. deposited on substrates such as

More information

ECE 595, Section 10 Numerical Simulations Lecture 33: Introduction to Finite- Difference Time-Domain Simulations. Prof. Peter Bermel April 3, 2013

ECE 595, Section 10 Numerical Simulations Lecture 33: Introduction to Finite- Difference Time-Domain Simulations. Prof. Peter Bermel April 3, 2013 ECE 595, Section 10 Numerical Simulations Lecture 33: Introduction to Finite- Difference Time-Domain Simulations Prof. Peter Bermel April 3, 2013 Recap from Monday Numerical ODE solvers Initial value problems

More information

Available online at ScienceDirect. Energy Procedia 92 (2016 )

Available online at  ScienceDirect. Energy Procedia 92 (2016 ) Available online at www.sciencedirect.com ScienceDirect Energy Procedia 92 (2016 ) 505 514 6th International Conference on Silicon Photovoltaics, SiliconPV 2016 Increased light harvesting by structured

More information

Light: Geometric Optics

Light: Geometric Optics Light: Geometric Optics The Ray Model of Light Light very often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization, but

More information

X-Ray Diffraction Analysis of III-V Superlattices: Characterization, Simulation and Fitting

X-Ray Diffraction Analysis of III-V Superlattices: Characterization, Simulation and Fitting X-Ray Diffraction Analysis of III-V Superlattices: Characterization, Simulation and Fitting Enlong Liu Xiangyu Wu Abstract Three samples of III-V semiconductor superlattice (SL) are investigated by X-ray

More information

Version 001 Interference jean (AP Phy MHS 2012) 1

Version 001 Interference jean (AP Phy MHS 2012) 1 Version 001 Interference jean AP Phy MHS 01) 1 This print-out should have 11 questions. Multiple-choice questions may continue on the next column or page find all choices before answering. sound m Concept

More information

MONOLITHIC NEAR INFRARED IMAGE SENSORS ENABLED BY QUANTUM DOT PHOTODETECTOR

MONOLITHIC NEAR INFRARED IMAGE SENSORS ENABLED BY QUANTUM DOT PHOTODETECTOR MONOLITHIC NEAR INFRARED IMAGE SENSORS ENABLED BY QUANTUM DOT PHOTODETECTOR PAWEŁ E. MALINOWSKI, E. GEORGITZIKIS, J. MAES, M. MAMUN, O. ENZING, F. FRAZZICA, J.VAN OLMEN, P. DE MOOR, P. HEREMANS, Z. HENS,

More information

Modeling of Surface Reflectance of Acid Textured Multicrystalline Silicon Wafer for Solar Cell Application

Modeling of Surface Reflectance of Acid Textured Multicrystalline Silicon Wafer for Solar Cell Application International Journal of Electronics and Computer Science Engineering 1065 Available Online at www.ijecse.org ISSN- 2277-1956 Modeling of Surface Reflectance of Acid Textured Multicrystalline Silicon Wafer

More information

( ) n ; t = n! $ m 2 = & ' ; t = n. 2n soap film. Solution: " t = & 7.45 ( 10)7 m =

( ) n ; t = n! $ m 2 = & ' ; t = n. 2n soap film. Solution:  t = & 7.45 ( 10)7 m = Section 10.1: Interference in Thin Films Tutorial 1 Practice, page 507 1. The second soap film is thicker. The longer wavelength of the second film means the film at that point must be thicker for constructive

More information

Chapter 24. Wave Optics

Chapter 24. Wave Optics Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics

More information

LIGHT SCATTERING THEORY

LIGHT SCATTERING THEORY LIGHT SCATTERING THEORY Laser Diffraction (Static Light Scattering) When a Light beam Strikes a Particle Some of the light is: Diffracted Reflected Refracted Absorbed and Reradiated Reflected Refracted

More information

Huamao Huang, Jinyong Hu, and Hong Wang. 1. Introduction

Huamao Huang, Jinyong Hu, and Hong Wang. 1. Introduction e Scientific World Journal, Article ID 837586, 6 pages http://dx.doi.org/10.1155/2014/837586 Research Article Light-Output Enhancement of GaN-Based Light-Emitting Diodes with Three-Dimensional Backside

More information

Defect Repair for EUVL Mask Blanks

Defect Repair for EUVL Mask Blanks Defect Repair for EUVL Mask Blanks A.Barty, S.Hau-Riege, P.B.Mirkarimi, D.G.Stearns, H.Chapman, D.Sweeney Lawrence Livermore National Laboratory M.Clift Sandia National Laboratory E.Gullikson, M.Yi Lawrence

More information

HOLOGRAPHIC SPECTRUM SPLITTING

HOLOGRAPHIC SPECTRUM SPLITTING 10 C h a p t e r 2 HOLOGRAPHIC SPECTRUM SPLITTING To move beyond the efficiency limits of single-junction solar cells, junctions of different bandgaps must be used to avoid losses from lack of absorption

More information

1. (25pts) Answer the following questions. Justify your answers. (Use the space provided below and the next page)

1. (25pts) Answer the following questions. Justify your answers. (Use the space provided below and the next page) . (25pts) Answer the following questions. Justify your answers. (Use the space provided below and the next page) a). An object (an arrow) is placed as shown in front of each of the following optical instruments.

More information

Benefiting from Polarization: Effects at High-NA Imaging

Benefiting from Polarization: Effects at High-NA Imaging Benefiting from Polarization: Effects at High-NA Imaging Bruce W. Smith L. Zavyalova, A. Estroff, Y. Fan, A. Bourov Rochester Institute of Technology P. Zimmerman International SEMACH and Intel J. Cashmore

More information

PHY 112: Light, Color and Vision. Lecture 11. Prof. Clark McGrew Physics D 134. Review for Exam. Lecture 11 PHY 112 Lecture 1

PHY 112: Light, Color and Vision. Lecture 11. Prof. Clark McGrew Physics D 134. Review for Exam. Lecture 11 PHY 112 Lecture 1 PHY 112: Light, Color and Vision Lecture 11 Prof. Clark McGrew Physics D 134 Review for Exam Lecture 11 PHY 112 Lecture 1 From Last Time Lenses Ray tracing a Convex Lens Announcements The midterm is Thursday

More information

SILICON PHOTONICS WAVEGUIDE AND ITS FIBER INTERCONNECT TECHNOLOGY. Jeong Hwan Song

SILICON PHOTONICS WAVEGUIDE AND ITS FIBER INTERCONNECT TECHNOLOGY. Jeong Hwan Song SILICON PHOTONICS WAVEGUIDE AND ITS FIBER INTERCONNECT TECHNOLOGY Jeong Hwan Song CONTENTS Introduction of light waveguides Principals Types / materials Si photonics Interface design between optical fiber

More information

Design of Hexagonal Micro Lenses Array Solar Concentrator

Design of Hexagonal Micro Lenses Array Solar Concentrator ISSN: 235-328 Design of Hexagonal Micro Lenses Array Solar Concentrator Alaa Bader Hassan, Sabah Ali Hussein Department of Physics, College of Education Ibn Al-Haitham for Pure Sciences, University of

More information

Mirror Example Consider a concave mirror radius -10 cm then = = Now consider a 1 cm candle s = 15 cm from the vertex Where is the image.

Mirror Example Consider a concave mirror radius -10 cm then = = Now consider a 1 cm candle s = 15 cm from the vertex Where is the image. Mirror Example Consider a concave mirror radius -10 cm then r 10 f = = = 5 cm 2 2 Now consider a 1 cm candle s = 15 cm from the vertex Where is the image 1 s 2 1 = = r s 1 1 2 + = = s s r 1 1 = 0.13333

More information

Light. Electromagnetic wave with wave-like nature Refraction Interference Diffraction

Light. Electromagnetic wave with wave-like nature Refraction Interference Diffraction Light Electromagnetic wave with wave-like nature Refraction Interference Diffraction Light Electromagnetic wave with wave-like nature Refraction Interference Diffraction Photons with particle-like nature

More information

OPTICAL ABSORPTION ENHANCEMENT IN SOLAR CELLS VIA 3D PHOTONIC CRYSTAL STRUCTURES

OPTICAL ABSORPTION ENHANCEMENT IN SOLAR CELLS VIA 3D PHOTONIC CRYSTAL STRUCTURES Progress In Electromagnetics Research M, Vol. 17, 1 11, 2011 OPTICAL ABSORPTION ENHANCEMENT IN SOLAR CELLS VIA 3D PHOTONIC CRYSTAL STRUCTURES J.-Y. Chen R&D Planning Division Office of Strategy and R&D

More information

FRAUNHOFER INSTITUTE FOR SOLAR ENERGY SYSTEMS ISE

FRAUNHOFER INSTITUTE FOR SOLAR ENERGY SYSTEMS ISE FRAUNHOFER INSTITUTE FOR SOLAR ENERGY SYSTEMS ISE Mirror qualification for concentrating solar collectors Anna Heimsath Head of Team Concentrating Collectors Fraunhofer Institute for Solar Energy Systems

More information

Layered media and photonic crystals. Cord Arnold / Anne L Huillier

Layered media and photonic crystals. Cord Arnold / Anne L Huillier Layered media and photonic crystals Cord Arnold / Anne L Huillier Definition A photonic crystal is a periodic arrangement of a dielectric material that exhibits strong interaction with light Variation

More information

MODELING LED LIGHTING COLOR EFFECTS IN MODERN OPTICAL ANALYSIS SOFTWARE LED Professional Magazine Webinar 10/27/2015

MODELING LED LIGHTING COLOR EFFECTS IN MODERN OPTICAL ANALYSIS SOFTWARE LED Professional Magazine Webinar 10/27/2015 MODELING LED LIGHTING COLOR EFFECTS IN MODERN OPTICAL ANALYSIS SOFTWARE LED Professional Magazine Webinar 10/27/2015 Presenter Dave Jacobsen Senior Application Engineer at Lambda Research Corporation for

More information

Mirror Example Consider a concave mirror radius r = -10 cm then. Now consider a 1 cm candle s = 15 cm from the vertex Where is the image.

Mirror Example Consider a concave mirror radius r = -10 cm then. Now consider a 1 cm candle s = 15 cm from the vertex Where is the image. Mirror Example Consider a concave mirror radius r = -0 cm then r 0 f 5 cm 2 2 Now consider a cm candle s = 5 cm from the vertex Where is the image s 2 r s 2 s s r 0.3333 5 5 f s' 0.333 M ' s 7.5 Magnification

More information

Diffraction Gratings as Anti Reflective Coatings Noah Gilbert. University of Arizona ngilbert .arizona.edu Phone: (520)

Diffraction Gratings as Anti Reflective Coatings Noah Gilbert. University of Arizona   ngilbert .arizona.edu Phone: (520) Diffraction Gratings as Anti Reflective Coatings Noah Gilbert University of Arizona Email: ngilbertemail.arizona.edu Phone: (520)304 4864 Abstract: Diffraction gratings with sub wavelength spatial frequencies

More information

Reflectivity Calculation Program

Reflectivity Calculation Program Reflectivity Calculation Program This optional program allows calculation of the reflectivity spectrum at any incidence angle from the wavelength distribution of the sample n and k values. Additionally,

More information

Reduced surface roughness of solid thin films prepared by alternating-bias, radio-frequency magnetron sputtering

Reduced surface roughness of solid thin films prepared by alternating-bias, radio-frequency magnetron sputtering 2174 J. Opt. Soc. Am. B/ Vol. 20, No. 10/ October 2003 R. Rabady and I. Avrutsky Reduced surface roughness of solid thin films prepared by alternating-bias, radio-frequency magnetron sputtering Rabi Rabady

More information

Supplementary Figure 1: Schematic of the nanorod-scattered wave along the +z. direction.

Supplementary Figure 1: Schematic of the nanorod-scattered wave along the +z. direction. Supplementary Figure 1: Schematic of the nanorod-scattered wave along the +z direction. Supplementary Figure 2: The nanorod functions as a half-wave plate. The fast axis of the waveplate is parallel to

More information

INTERACTIVE SIMULATION OF SILICON SOLAR CELLS

INTERACTIVE SIMULATION OF SILICON SOLAR CELLS INTERACTIVE SIMULATION OF SILICON SOLAR CELLS A.R. Burgers J.J. van Wijk W.C. Sinke Netherlands Energy Research Foundation ECN P. O. Box 1 1755 ZG Petten The Netherlands Phone: +31-224-564115 Fax: +31-224-563214

More information

Bifacial PV cell with reflector for stand-alone mast for sensor powering purposes

Bifacial PV cell with reflector for stand-alone mast for sensor powering purposes Downloaded from orbit.dtu.dk on: Mar 19, 219 Bifacial PV cell with reflector for stand-alone mast for sensor powering purposes Jakobsen, Michael Linde; Thorsteinsson, Sune; Poulsen, Peter Behrensdorff;

More information

Study of Air Bubble Induced Light Scattering Effect On Image Quality in 193 nm Immersion Lithography

Study of Air Bubble Induced Light Scattering Effect On Image Quality in 193 nm Immersion Lithography Study of Air Bubble Induced Light Scattering Effect On Image Quality in 193 nm Immersion Lithography Y. Fan, N. Lafferty, A. Bourov, L. Zavyalova, B. W. Smith Rochester Institute of Technology Microelectronic

More information

4.5 Images Formed by the Refraction of Light

4.5 Images Formed by the Refraction of Light Figure 89: Practical structure of an optical fibre. Absorption in the glass tube leads to a gradual decrease in light intensity. For optical fibres, the glass used for the core has minimum absorption at

More information

1.Rayleigh and Mie scattering. 2.Phase functions. 4.Single and multiple scattering

1.Rayleigh and Mie scattering. 2.Phase functions. 4.Single and multiple scattering 5 November 2014 Outline 1.Rayleigh and Mie scattering 2.Phase functions 3.Extinction 4.Single and multiple scattering Luca Lelli luca@iup.physik.uni-bremen.de Room U2080 Phone 0421.218.62097 Scattering

More information

COLOR HELPS TO SELL VEHICLES

COLOR HELPS TO SELL VEHICLES COLOR HELPS TO SELL VEHICLES Like/Dislike decisions made in seconds 40% of buyers will choose a different vehicle if their color choice is not available. Emotional connection with owner 1 VEHICLE DESIGN

More information

CS 348B Project Report Mingyu Gao, Jing Pu

CS 348B Project Report Mingyu Gao, Jing Pu CS 348B Project Report Mingyu Gao, Jing Pu mgao12@stanford.edu, jingpu@stanford.edu Introduction In this project, we plan to render silicon wafers with the signature of rainbow colors on the reflecting

More information

MODULE 3. FACTORS AFFECTING 3D LASER SCANNING

MODULE 3. FACTORS AFFECTING 3D LASER SCANNING MODULE 3. FACTORS AFFECTING 3D LASER SCANNING Learning Outcomes: This module discusses factors affecting 3D laser scanner performance. Students should be able to explain the impact of various factors on

More information

Spectral Estimation of Skin Color with Foundation Makeup

Spectral Estimation of Skin Color with Foundation Makeup Spectral Estimation of Skin Color with Foundation Makeup M. Doi 1, R. Ohtsuki, and S. Tominaga 3 1 Department of Telecommunications and Computer Networks, Faculty of Information and Communication Engineering,

More information

Council for Optical Radiation Measurements (CORM) 2016 Annual Technical Conference May 15 18, 2016, Gaithersburg, MD

Council for Optical Radiation Measurements (CORM) 2016 Annual Technical Conference May 15 18, 2016, Gaithersburg, MD Council for Optical Radiation Measurements (CORM) 2016 Annual Technical Conference May 15 18, 2016, Gaithersburg, MD Multispectral measurements of emissive and reflective properties of displays: Application

More information

10.4 Interference in Thin Films

10.4 Interference in Thin Films 0. Interference in Thin Films You have probably noticed the swirling colours of the spectrum that result when gasoline or oil is spilled on water. And you have also seen the colours of the spectrum shining

More information