Alta and Spectrum-splitting III-V Multijunction Solar Cells
Harry A. Atwater California Institute of Technology and Alta Devices
• • • • •
Ultrahigh Efficiency – Radiative Emission and Photon Recycling Full Spectrum Approach – Carrier Thermalization Holographic Spectrum Splitting Polyhedral Specular Reflector Light Trapping Filtered Concentrator
Harry Atwater
[email protected]
InterSolar July 9th, 2013
1
Inefficient use of spectrum is largest loss mechanism
Polman and Atwater, Nature Materials (2012). Harry Atwater
[email protected]
InterSolar July 9th, 2013
2
Multijunction Architectures Spectrum Splitting Independent Connect
Monolithic Series Connect
• • •
Lattice match or slight lattice mismatch -> constrains choice of subcell bandgaps Current matching reduces energy yield Fewer subcells (2-4)
Harry Atwater
[email protected]
InterSolar July 9th, 2013
• • • • •
More subcells (6-15) Almost optimal bandgaps Independent electrical connections More complex assembly Spectral splitting optics required
3
Full Spectrum Research History
Record cell design VHESC design
• • •
DARPA initiative for Very High Efficiency Solar Cells (VHESC) Dichroic filters DuPont, η=38.5% spectrum-splitting record (2010)
• • •
A. Barnett PVSC (2006); A. Barnett et al. Prog. in PV. (2009) Harry Atwater
[email protected]
InterSolar July 9th, 2013
Patented in 1987 Fraunhofer prototype showed 34.3% efficiency outdoor unconcentrated 2 single junction and 1 dual junction cell connected in series Patent WO 87/01512 B. Mitchell et al. Prog. Photovolt.: Res. Appl. (2010)
4
New Developments Commoditization of complexity ~ 1 m2 integrated optoelectronics: Visio 50” 1080p Flat Panel LCD à >106 pixels @ $500/m2 All perfect
Harry Atwater
[email protected]
InterSolar July 9th, 2013
5
New Developments Lower cost solar cells and cell assembly: • Epitaxial liftoff • Transfer printing • Pick-and-place assembly
Yoon et al, Rodgers Group, UIUC Nature (2010) Harry Atwater
[email protected]
InterSolar July 9th, 2013
6
New Developments • Single junction cells driven to high ERE • Cost of III-V cells driven toward flat plate $/m2 GaAs Epitaxial Liftoff
Harry Atwater
[email protected]
InterSolar July 9th, 2013
High Throughput GaAs Growth
7
Balance between Solar Absorption and Light Extraction high internal quantum efficiency (internal fluorescence yield) photons internally absorbed and re-radiated many times
IQE ~ 1 R~1 Conditions for high ERE: IQE~1 and R~1
Harry Atwater
[email protected]
InterSolar July 9th, 2013
8
Single crystal thin film GaAs solar cells and modules iPhone cover 1.1 W
Man portable charger
• Cell efficiency η = 28.8% @ 1 Sun AM 1.5G
ERE = 48%
• Module efficiency of 23.2% • IQE > 0.96 • Economical III-V flat plate ($1/Wp) PV System) Kayes et al, Alta Devices PVSC (2011, 2012) Harry Atwater
[email protected]
InterSolar July 9th, 2013
9
Premises • No conceptual or theoretical obstacle to >50% module efficiency • Multijunction solar cells most viable ultrahigh efficiency option to mitigate carrier thermalization (compared to MEG or hot carrier collection). • Lifted off III-V cells will be available from 0.74 – 2.0 eV with ERE 0.1-5% and costs of 1-5x Si cell $/m2. • Complex, large-area optoelectronics can be commoditized • Concentrating solar 2-axis tracking commercially available
Harry Atwater
[email protected]
InterSolar July 9th, 2013
10
Efficiency with Many Subcells
7/12/13 Harry Atwater
[email protected]
InterSolar July 9th, 2013
11
11
7 Junction Subcell Choices
In0.53Ga0.47As-
ERE# (Simulated)# 2.56%-
ERE# (Record)# 2%-
0.94#
In0.71Ga0.29As0.62P0.38-
0.33%-
5-
1.15# 1.42# 1.58# 1.84# 2.13#
In0.87Ga0.13As0.28P0.72GaAsAl0.1Ga0.9AsGa0.52In0.48PAl0.20Ga0.32In0.48P-
0.40%8.51%-5.8%0.19%0.08%-
548.5% 22.5%58%5-
Eg#(eV)#
III)V#Alloy#
0.74#
• • •
Single junction ELO cells lattice-matched to GaAs or InP Device modeling: average ERE = 0.3% and 90% of ideal Jsc
Warmann, et. al,, PVSC (2013)
Harry Atwater
[email protected]
InterSolar July 9th, 2013
12
Full Spectrum Optical Designs
Atwater, et. al,, PVSC (2013)
Harry Atwater
[email protected]
InterSolar July 9th, 2013
13
Four-way Holographic Spectrum Splitting
• 8 lattice-matched subcells • Materials grown on GaAs and InP
• •
Commercially available gratings 3 x 4 gratings: tractable design problem
Escarra, et. al,, PVSC (2013)
Harry Atwater
[email protected]
InterSolar July 9th, 2013
14
Holographic Splitting Design Cycle
Harry Atwater
[email protected]
InterSolar July 9th, 2013
15
Power Efficiency Diffraction Efficiency Using simple gratings: • Not ideal “top-hat” spectral slices • 2nd order diffraction issues, especially for blue light • Optical efficiency: 77%
Harry Atwater
[email protected]
InterSolar July 9th, 2013
16
Two-axis Concentration @ 90% abs & 1% ERE 42.3% Stacked holographic optical elements Hollow trough compound parabolic concentrator (CPC) Height: 172 mm
Total concentration: 672X Solid Polymer CPCs Height: 72 mm relative losses from the CPCs (4%), reflections at interfaces (5%), electrical series resistance (2%), and DC-to-DC conversion (2%)
Four dual-junction cells: 1mm x 7.7mm Two-terminal module efficiency37.1%
Harry Atwater
[email protected]
InterSolar July 9th, 2013
17
Full Spectrum Optical Designs
Harry Atwater
[email protected]
InterSolar July 9th, 2013
18
Polyhedral Specular Reflector Eg (eV)
III-‐V Alloy
Substrate
2.15
Al0.20Ga0.32In0.48P
GaAs
1.84
Ga0.51In0.49P
GaAs
1.58
Al0.1Ga0.9As
GaAs
1.42
GaAs
GaAs
1.15
In0.87Ga0.13As0.28P0.72
InP
0.94
In0.71Ga0.29As0.62P0.38
InP
0.74
In0.53Ga0.47As
InP
Cell modeling: average ERE of 0.3% and 90% of ideal Jsc Eisler, et. al,, PVSC (2013) Harry Atwater
[email protected]
InterSolar July 9th, 2013
19
Subcell 7
Subcell 6
Subcell 5
Subcell 3 Subcell 4
Subcell 2
Subcell 1
Shortpass Filters Prevent Parasitic Loss
shortpass filters available near the applicable wavelengths; aperiodic alternating SiO2 and Nb2O3 multillayers. Harry Atwater
[email protected]
InterSolar July 9th, 2013
20
Polyhedral Specular Reflector Prototype Spectra
Optical Efficiency = 80.4%
Harry Atwater
[email protected]
InterSolar July 9th, 2013
21
Calculated Efficiencies with Concentrator
Imperfect filters & electrical losses.
• Tradeoff between concentration and optical efficiency • Higher index parallelepiped gives higher optical efficiency
ERE of 0.3% and Jsc 90% of ideal Harry Atwater
[email protected]
InterSolar July 9th, 2013
22
Polyhedral Specular Reflector Prototype
Proof of concept design incorporating 6 subcells
Harry Atwater
[email protected]
InterSolar July 9th, 2013
23
Full Spectrum Optical Designs
Harry Atwater
[email protected]
InterSolar July 9th, 2013
24
Light Trapped in a Textured Slab
High Concentration Optic
Angle Restrictor Omnidirectional Filter Multijuction Solar Cell
Reflector
Multijunction Solar Cells
Light trapped by total internal reflection and angle restrictor Light scatters in the slab until it enters solar cell or escapes. Kosten, et. al,, PVSC (2013) Harry Atwater
[email protected]
InterSolar July 9th, 2013
25
Light Trapping Filtered Concentrator • Low index slab allows for nearly omnidirectional filter performance • Initial designs give 45% receiver efficiency at ~150 suns • Estimated two-terminal module efficiency of 38% • Improved tracking accuracy enables much higher concentration and small efficiency boost
Harry Atwater
[email protected]
InterSolar July 9th, 2013
26
Full Spectrum Team
Cristofer Flowers
Dr. Matt Escarra
Emily Kosten
Harry Atwater
[email protected]
Emily C. Warmann Carissa Eisler
John Lloyd InterSolar July 9th, 2013
Sunita Darbe
27
Web Resources on Photonic Design in PV http://www.lmi.caltech.edu/
The "Light-‐Material InteracAons in Energy Conversion" Energy FronAer Research Center (LMI-‐EFRC) is a naAonal resource for fundamental opAcal principles and phenomena relevant to solar energy conversion, and for design of the opAcal properAes of materials and devices used for energy conversion.
Harry Atwater
[email protected]
InterSolar July 9th, 2013
28
Plenty of Room at the Top • PV designs with 6-15 high radiative efficiency lifted off subcells to mitigate carrier thermalization
• Three designs with 37-40% realistic two-terminal module efficiency potential with available components Support gratefully acknowledged
Harry Atwater
[email protected]
InterSolar July 9th, 2013
29
Supporting Slides
Harry Atwater
[email protected]
InterSolar July 9th, 2013
30
Complexity? Death by a thousand cuts
Tied down by many small problems
Harry Atwater
[email protected]
InterSolar July 9th, 2013
31
Two-way Holographic Splitting U. Minnesota
U. Arizona
•
•
•
Two multiplexed volume phase gratings 100 suns concentration, 2 cells, η≈45% from detailed balance
• •
Holograms to split concentrated light 28% efficiency expected GaAs and Si subcells
D. Zhang, et al., Proc. SPIE (2012).
Harry Atwater
[email protected]
InterSolar July 9th, 2013
32
Photovoltaic Cavity Concentrator
• Hollow Cavity • Array of Single Junction Cells • Filters (Rugate or Multilayer
U. Ortabasi
Harry Atwater
[email protected]
US Patent Application US20030213514 A1, May 17th 2002
InterSolar July 9th, 2013
33
Efficiency with Many Subcells
Contours: 90% optical efficiency and 95% electrical system efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
34
Efficiency with Many Subcells
Contours: 90% optical efficiency and 95% electrical system efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
35
Efficiency with Many Subcells
Contours: 90% optical efficiency and 95% electrical system efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
36
Efficiency with Many Subcells
Contours: 90% optical efficiency and 95% electrical system efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
37
Efficiency with Many Subcells
Contours: 90% optical efficiency and 95% electrical system efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
38
Tracking Accuracy
• • •
Performance of holograms sensitive to incident angle Concentrator has acceptance angle of +/- 2° Tracking accuracy of +/- 1.5° (1500x) necessary
Harry Atwater
[email protected]
InterSolar July 9th, 2013
39
Calculated Efficiencies with Concentrator
• Tradeoff between concentration and optical efficiency • Higher index parallelepiped gives higher optical efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
40
Free carrier absorption Imperfect mirror
Optical Efficiency
Parasitic Absorption Losses
Parallelepiped Refractive Index
Parasitic Losses (%)
• Free carrier absorption in GaAs cell ~8-10% • >70% efficiency filters to obtain greater than 90% optical efficiency
Harry Atwater
[email protected]
InterSolar July 9th, 2013
41
Textured Slab Multipass Optical Model sin2θ/n2=probability of escape per pass
θ= restrictor acceptance angle n=slab refractive index
h≈w
f = fraction of light on correct cell (1/# of cells) 0.7/0.93 eV
1.23/1.06 eV
1.6/1.42 eV
2.25/1.84 eV
w
• • • •
Assume slab as thick as cells are wide, ideal filters Absorption on the first pass = f On the second pass = (1- f)(1- sin2θ/n2)f, etc. Overall absorption
Harry Atwater
[email protected]
f = 1− (1− f )(1− sin 2 θ / n 2 )
InterSolar July 9th, 2013
42
Achieving Efficient Light Absorption Acceptance Angle for Glass Slab!
>90% light directed to correct cells
27.3˚!
40.4˚!
52.6˚!
66.5˚!
2-4 multijunction subcells give high optical efficiency with a glass slab and reasonable acceptance angle Harry Atwater
[email protected]
InterSolar July 9th, 2013
43
Reducing Slab Escape 2 cells 2 cells 90% light abs. 3 cells 3 cells 4 cells 4 cells
Acceptance angle