Advanced light management techniques for building integrated PV (BIPV)

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

Manual for solar cell optical simulation software: GENPRO4

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

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

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

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

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

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

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

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

Laser Applications for Photovoltaics Crystalline and Thin Film Technologies

Laser Applications for Photovoltaics Crystalline and Thin Film Technologies

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

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

Compact Multilayer Film Structure for Angle Insensitive. Color Filtering

High spatial resolution measurement of volume holographic gratings

OPTOELECTRONIC DESIGN OF MULTIJUNCTION WIRE-ARRAY SOLAR CELLS

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

Holographic Elements in Solar Concentrator and Collection Systems

POLYHEDRAL SPECULAR REFLECTOR

Available online at ScienceDirect. Energy Procedia 92 (2016 )

Agilent Cary Universal Measurement Spectrophotometer (UMS)

T-Solar Overview. * Patent-pending

RAPID CALCULATION OF THE BACKSHEET COUPLING GAIN USING RAY GROUPS

DETAILED MODELING OF COMPLEX BIPV SYSTEMS

Texturing industrial multicrystalline silicon solar cells

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

Thin film solar cell simulations with FDTD

Chapter 7. Widely Tunable Monolithic Laser Diodes

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

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

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

Microstructured surface design for omnidirectional antireflection coatings on solar cells

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

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

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

Session 1B Transparent Materials

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

ScienceDirect. The multi-busbar design: an overview

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

Unit 5.C Physical Optics Essential Fundamentals of Physical Optics

Fiber Optic Communication Systems. Unit-03: Properties of Light.

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

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

College Physics B - PHY2054C

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

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

LECTURE 13 THIN FILM INTERFERENCE. Instructor: Kazumi Tolich

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

Pasadena, CA USA ABSTRACT

Chapter 2: Wave Optics

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

HYPERSPECTRAL IMAGING THIN FILM APPLICATIONS. Dr. Wulf Grählert /

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

Diffraction Efficiency

Physics 202, Lecture 23

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

Geant4 Studies for the HPD-PET scintillators

Light and Electromagnetic Waves. Honors Physics

Specification of Thin Film Thickness Measuring Equipment

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

Available online at ScienceDirect. Energy Procedia 92 (2016 )

Light: Geometric Optics

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

Version 001 Interference jean (AP Phy MHS 2012) 1

MONOLITHIC NEAR INFRARED IMAGE SENSORS ENABLED BY QUANTUM DOT PHOTODETECTOR

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

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

Chapter 24. Wave Optics

LIGHT SCATTERING THEORY

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

Defect Repair for EUVL Mask Blanks

HOLOGRAPHIC SPECTRUM SPLITTING

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

Benefiting from Polarization: Effects at High-NA Imaging

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

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

Design of Hexagonal Micro Lenses Array Solar Concentrator

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.

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

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

FRAUNHOFER INSTITUTE FOR SOLAR ENERGY SYSTEMS ISE

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

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

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.

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

Reflectivity Calculation Program

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

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

INTERACTIVE SIMULATION OF SILICON SOLAR CELLS

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

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

4.5 Images Formed by the Refraction of Light

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

COLOR HELPS TO SELL VEHICLES

CS 348B Project Report Mingyu Gao, Jing Pu

MODULE 3. FACTORS AFFECTING 3D LASER SCANNING

Spectral Estimation of Skin Color with Foundation Makeup

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

10.4 Interference in Thin Films

Transcription:

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

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 2015 2020 [1,3] Roadmap [1] International Technology Roadmap for Photovoltaic (ITRPV), (2013) [2] A. Goodrich et al. SOLMAT 114,110 135 (2013) [3] Predictions for the Solar Industry in 2014, IHS Whitepaper (2013) 2

Advanced light management in c-si Experimental demonstration of upper limit 4n 2 absorption enhancement [1] Front nano-texture (RIE) 2 µm 1.0 0.8 DBR Ag (ref.) Bulk c-si 20 μm Thermal SiO 2 DBR A Si [-] 0.6 0.4 1.28 μm Textured BS 2 µm 0.2 0.0 400 600 800 1000 1200 Wavelength [nm] [1] A. Ingenito, O. Isabella, M. Zeman, ACS Photonics, 1, 3 (2014) 3

Advanced light management in c-si IBC c-si solar cells IBC structure 1.0 1.0 0.8 0.8 EQE [-] 0.6 0.4 V OC (mv) 635 J SC (ma/cm 2 ) 40.5 FF (%) 77.0 0.6 0.4 R [-] 280 μm 0.2 η (%) 19.8 0.2 Front side 0.0 0.0 300 450 600 750 900 1050 1200 Wavelength [nm] A. Ingenito, O. Isabella, M. Zeman. Progress in Photovoltaics, DOI: 10.1002/pip.2606 (2015) 4

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: 0.1038/nnano.2015.89 (2015) [2] Paul de Jong, Exasun, BJ-BC workshop, Freiburg, (2015) 5

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 2015 2020 [1,3] Roadmap [1] International Technology Roadmap for Photovoltaic (ITRPV), (2013) [2] A. Goodrich et al. SOLMAT 114,110 135 (2013) [3] Predictions for the Solar Industry in 2014, IHS Whitepaper (2013) 6

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

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 [300-1200] nm for Front side o [900-1200] nm for Back side Reflectance above 80% at desired wavelength Substrate (Glass or wafer) Protected by glass/encapsulant 8

OF s optical modelling 1,00 0,90 0,80 0,70 0,60 0,50 0,40 0,30 0,20 0,10 1. 2-D Ray tracing* 0,00 390 440 490 540 590 640 690 740 790 2. Reflectance profile 3. Color Coordinates SunRay software by dr. R. Santbergen 9

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

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

Colour matrix (OF on glass and c-si solar cell) 10 x Glass EVA ARC 1.0 0.8 EQE [-] 0.6 0.4 0.2-3.5 ma/cm 2 Standard ARC (NO-OF) Coloured 0.0 400 600 800 1000 1200 Wavelength [nm] 12

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

Colour matrix (OF on c-si solar cell in glass) 10 x Glass EVA ARC 1.0 0.8 EQE [-] 0.6 0.4-1.8 ma/cm 2 Standard ARC (NO-OF) Coloured 0.2 0.0 400 600 800 1000 1200 Wavelength [nm] 14

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

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, 540-544 (2014) 16

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

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 [-] 0.6 0.4 0.2 Region of weak absorption in c-si DBR λ B 0.0 400 600 800 1000 1200 1400 Wavelength [nm] A. Ingenito, O. Isabella, M. Zeman, ACS Photonics, 1, 3 (2014) 18

Fabrication of DBR on textured surfaces 1.0 0.8 DBR R, T [-] 0.6 0.4 R 0.2 T 0.0 400 600 800 1000 1200 Wavelength [nm] Co-depostion of 6 x a-si:h (80 nm) / a-sin x :H (180 nm) 19

Fabrication of DBR on textured surfaces 1.0 0.8 DBR R, T [-] 0.6 0.4 R? 0.2 R T T DBR 0.0 400 600 800 1000 1200 Wavelength [nm] Co-depostion of 6 x a-si:h (80 nm) / a-sin x :H (180 nm) 20

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

DBR optimization for textured surface Influence of scaling factor on A Si 1.0 39.0 ma / cm 2 0.8 A Si [-] 0.6 0.4 0.2 0.8 1.0 1.2 1.5 1.7 DBR 38.1 ma/cm 2 0.0 400 600 800 1000 Wavelength [nm] 1000 1050 1100 1150 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

DBR optimization for textured surface Influence of scaling factor on λ B at DBR / air interface 0.8 1.0 1.2 1.5 1.7 R DBR air [-] 1.0 0.8 0.6 0.4 0.8 1.0 1.2 1.5 1.7 0.8 1 1.2 1.5 1.7 Light 0.2 DBR 0.0 400 600 800 1000 1200 1400 Wavelength [nm] 23

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. 33-40 24

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 [-] 1.0 0.8 0.6 0.4 0.2 1.0 0.8 0.6 0.4 0.2 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) 0.0 0.0 300 450 600 750 900 1050 1200 Wavelength [nm] 25

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

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

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] 230 210 190 170 150 130 110 90 J PH-T = 6.1 10-3 ma/cm 2 [2] Textured 70 40 60 80 100 120 140 a-si:h [nm] J ph T [ma/cm 2 ] 0.005 0.01 0.05 0.1 0.5 1.0 1.5 2.0 [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

Color resilience against angle of incidence 13

Device level color matrix 14

Performance of a cell under colored glass Parameter Standard Green Yellow J PH [ma/cm 2 ] 39.90 38.04 38.13 V OC [V] 0.684 0.683 0.683 FF [-] 0.784 0.786 0.786 iη[%] 21.41 20.42 20.46 15

Color resilience against angle of incidence 16

Color resilience against angle of incidence 17

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

DBR optimization for textured surface Influence of scaling factor on R and T 1.0 1.0 R [-] 0.8 0.6 0.4 0.8 1.0 1.2 1.5 1.7 DBR 0.8 0.6 0.4 T [-] 0.2 0.2 400 600 800 1000 1200 Wavelength [nm] 0.0 400 600 800 1000 1200 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

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

DBR optimization for textured surface Transmittance of optimized DBR 1.0 0.8 T [-] 0.6 Measured 1.0 Measured 1.5 Sim? 0.4 0.2 0.0 400 600 800 1000 1200 Wavelength [nm] DBR = 6 x a-si:h (80 nm) / a-sin x :H (180 nm) scaled of 1.5 37

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 =5.2 15 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:10.1002/pip.2606 (2014) 4

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

Effect of Defect Removal Etching QSSPC analysis 10-2 SiO 2 (a) Al 2 O 3 (b) 10-3 eff [s] 10-4 10-5 10 14 10 15 n [cm -3 ] 10 14 10 15 n [cm -3 ]

MST-textured* IBC c-si solar cell SiN Recombination 1.0 0.8 MST-T Std 1.0 0.8 Long wavelength scattering EQE [-] 0.6 0.4 V OC (mv) 634 640 J SC (ma/cm 2 ) 40.5 41.0 FF (%) 77.0 76.9 0.6 0.4 R [-] 0.2 η (%) 19.8 20.2 0.2 0.0 0.0 300 450 600 750 900 1050 1200 Wavelength [nm] 30 s DRE 5 µm 10 µm A. Ingenito, O. Isabella, M. Zeman, Progress in Photovoltaics, DOI:10.1002/pip.2606 (2014) 17

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. 72,899 1982 Efficient back reflector R b = 1 4