Band-Gap-Engineered Architectures for High-Efficiency Multijunction Concentrator Solar Cells Richard R. King, A. Boca, W. Hong, X.-Q. Liu, D. Bhusari, D. Larrabee, K. M. Edmondson, D. C. Law, C. M. Fetzer, S. Mesropian, and N. H. Karam Spectrolab, Inc. A Boeing Company
24th European Photovoltaic Solar Energy Conference Sep. 21-25, 2009 Hamburg, Germany R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
1
Acknowledgments • Carl Osterwald, Keith Emery, Larry Kazmerski, Martha Symko-Davies, Fannie Posey-Eddy, Holly Thomas, Manuel Romero, John Geisz, Sarah Kurtz – NREL • Rosina Bierbaum – University of Michigan, Ann Arbor • Pierre Verlinden, John Lasich – Solar Systems, Australia • Kent Barbour, Russ Jones, Jim Ermer, Peichen Pien, Dimitri Krut, Hector Cotal, Mark Osowski, Joe Boisvert, Geoff Kinsey, Mark Takahashi, and the entire multijunction solar cell team at Spectrolab This work was supported in part by the U.S. Dept. of Energy through the NREL High-Performance Photovoltaics (HiPerf PV) program (ZAT-4-33624-12), the DOE Technology Pathways Partnership (TPP), and by Spectrolab.
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Outline contact AR
• Solar cell theoretical efficiency limits – Opportunities to change ground rules for higher terrestrial efficiency – Cell architectures capable of >70% in theory, >50% in practice
n+-GaInAs n-AlInP window n-GaInP emitter
Ce
p To
p-GaInP base
p-AlGaInP BSF p++-TJ n++-TJ
W
id
n-GaInP window n-GaInAs emitter p-GaInAs base
M
E e-
g
Tu
e dl id
ll
el nn
Ce
ll
p-GaInP BSF p-GaInAs step-graded buffer
• Metamorphic semiconductor materials – Control of band gap to tune to solar spectrum • High-efficiency terrestrial concentrator cells – Metamorphic (MM) and lattice-matched (LM) 3-junction solar cells with >40% efficiency – 4-junction MM and LM concentrator cells – Inverted metamorphic structure, semiconductor bonded technology (SBT) for MJ terrestrial concentrator cells
p++-TJ n++-TJ
Tu
el nn
nucleation
n+-Ge emitter p-Ge base and substrate
t Bo
Ju
m to
nc
t io
Ce
n
ll
contact
metal gridline
semiconductor bonded interface
2.0-eV AlGaInP cell 1 1.7-eV AlGaInAs cell 2 1.4-eV GaInAs cell 3 1.1-eV GaInPAs cell 4 0.75-eV GaInAs cell 5
• The solar resource and concentrator photovoltaic (CPV) system economics
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
3
High-Efficiency Multijunction Cell Architectures
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Maximum Solar Cell Efficiencies Measured Theoretical References C. H. Henry, “Limiting efficiencies of ideal single and multiple energy gap terrestrial solar cells,” J. Appl. Phys., 51, 4494 (1980). W. Shockley and H. J. Queisser, “Detailed Balance Limit of Efficiency of p-n Junction Solar Cells,” J. Appl. Phys., 32, 510 (1961). J. H. Werner, S. Kolodinski, and H. J. Queisser, “Novel Optimization Principles and Efficiency Limits for Semiconductor Solar Cells,” Phys. Rev. Lett., 72, 3851 (1994). R. R. King et al., "Band-Gap-Engineered Architectures for High-Efficiency Multijunction Concentrator Solar Cells," 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009. R. R. King et al., "40% efficient metamorphic GaInP / GaInAs / Ge multijunction solar cells," Appl. Phys. Lett., 90, 183516 (4 May 2007). M. Green, K. Emery, D. L. King, Y. Hishikawa, W. Warta, "Solar Cell Efficiency Tables (Version 27)", Progress in Photovoltaics, 14, 45 (2006). A. Slade, V. Garboushian, "27.6%-Efficient Silicon Concentrator Cell for Mass Production," Proc. 15th Int'l. Photovoltaic Science and Engineering Conf., Beijing, China, Oct. 2005. R. P. Gale et al., "High-Efficiency GaAs/CuInSe2 and AlGaAs/CuInSe2 Thin-Film Tandem Solar Cells," Proc. 21st IEEE Photovoltaic Specialists Conf., Kissimmee, Florida, May 1990. J. Zhao, A. Wang, M. A. Green, F. Ferrazza, "Novel 19.8%-efficient 'honeycomb' textured multicrystalline and 24.4% monocrystalline silicon solar cells," Appl. Phys. Lett., 73, 1991 (1998).
95% 93%
Carnot eff. = 1 – T/Tsun T = 300 K, Tsun ≈ 5800 K Max. eff. of solar energy conversion = 1 – TS/E = 1 – (4/3)T/Tsun (Henry)
72%
Ideal 36-gap solar cell at 1000 suns
(Henry)
56% 50%
Ideal 3-gap solar cell at 1000 suns Ideal 2-gap solar cell at 1000 suns
(Henry) (Henry)
44% 43%
Ultimate eff. of device with cutoff Eg: (Shockley, Queisser) 1-gap cell at 1 sun with carrier multiplication (>1 e-h pair per photon) (Werner, Kolodinski, Queisser)
37%
Ideal 1-gap solar cell at 1000 suns
31% 30%
Ideal 1-gap solar cell at 1 sun (Henry) Detailed balance limit of 1 gap solar cell at 1 sun (Shockley, Queisser)
3-gap GaInP/GaInAs/Ge LM cell, 364 suns (Spectrolab) 41.6% 3-gap GaInP/GaInAs/Ge MM cell, 240 suns (Spectrolab) 40.7%
(Henry)
3-gap GaInP/GaAs/GaInAs cell at 1 sun (NREL) 33.8% 1-gap solar cell (silicon, 1.12 eV) at 92 suns (Amonix) 27.6% 1-gap solar cell (GaAs, 1.424 eV) at 1 sun (Kopin) 25.1% 1-gap solar cell (silicon, 1.12 eV) at 1 sun (UNSW) 24.7%
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Metamorphic (MM) 3-Junction Solar Cell
contact n+-GaInAs n-AlInP window n-GaInP emitter
Ce
p To
p-GaInP base
p-AlGaInP BSF p++-TJ n++-TJ
W
i
-E de
n-GaInP window n-GaInAs emitter p-GaInAs base
M
g
Tu
e dl id
ll
el nn
Ce
ll
p-GaInP BSF p-GaInAs step-graded buffer p++-TJ n++-TJ
n Tu
ne
nucleation
n+-Ge emitter p-Ge base and substrate
t Bo
l
n t io nc u J
m to
l Ce
l
contact
Lattice-Mismatched or Metamorphic (MM)
C urrent D ensity / Incident Intensity (A /W )
0.3
AR
MJ cell 0.25
subcell 1 subcell 2
0.2
subcell 3
0.15
0.1
0.05
0 0
0.5
1
1.5
2
2.5
3
3.5
Voltage (V)
• Metamorphic growth of upper two subcells, GaInAs and GaInP R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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External QE of LM and MM 3-Junction Cells 100
100 AM1.5D, low-AOD AM1.5G, ASTM G173-03 AM0, ASTM E490-00a
90
Current Density per Unit Wavelength (mA/(cm 2μm))
EQE, lattice-matched
80
EQE, metamorphic
80
70
70
60
60
50
50
40
40
30
30
20
20
10
10
0 300
500
700
900
1100
1300
1500
1700
External Quantum Efficiency (%)
90
0 1900
Wavelength (nm) R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Metamorphic (MM) 3-Junction Solar Cell Eg1 = Subcell 1 (Top) Bandgap (eV) .
2.1 3-junction Eg1/ Eg2/ 0.67 eV cell efficiency 240 suns (24.0 W/cm2), AM1.5D (ASTM G173-03), 25oC 2 Ideal efficiency -- radiative recombination limit
MM 40.7%
1.9
LM 40.1%
1.8 54%
1.7 52%
1.6
50% 48%
1.5
46% 44%
1.4
42%
40%
1.3 1.0
1.1
1.2
1.3
1.4
38%
1.5
1.6
Eg2 = Subcell 2 Bandgap (eV) Disordered GaInP top subcell
Ordered GaInP top subcell
• Metamorphic GaInAs and GaInP subcells bring band gap combination closer to theoretical optimum R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Record 40.7%-Efficient Concentrator Solar Cell
Spectrolab Metamorphic GaInP/ GaInAs/ Ge Cell Voc Jsc FF Vmp
= = = =
2.911 V 3.832 A/cm2 87.50% 2.589 V
• First solar cell of any type to reach over 40% efficiency
Efficiency = 40.7% ± 2.4% 240 suns (24.0 W/cm2) intensity 0.2669 cm2 designated area 25 ± 1°C, AM1.5D, low-AOD spectrum
Ref.: R. R. King et al., "40% efficient metamorphic GaInP / GaInAs / Ge multijunction solar cells," Appl. Phys. Lett., 90, 183516, 4 May 2007.
Concentrator cell light I-V and efficiency independently verified by J. Kiehl, T. Moriarty, K. Emery – NREL R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Metamorphic (MM) 3-Junction Cells –– Inverted 1.0-eV GaInAs Subcell
Ge or GaAs substrate
Ge or GaAs substrate
Growth Direction
cap
1.9 eV (Al)GaInP subcell 1 1.4 eV GaInAs subcell 2 graded MM buffer layers
1.0 eV GaInAs subcell 3
Growth on Ge or GaAs substrate, followed by substrate removal from sunward surface R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Inverted Metamorphic (IMM) 3-Junction Cell 1.6
3-junction 1.9 eV/ Eg2/ Eg3 cell efficiency 2
o
Eg2 = Subcell 2 Bandgap (eV) .
500 suns (50 W/cm ), AM1.5D (ASTM G173-03), 25 C X
Ideal efficiency -- radiative recombination limit
1.5
1.4
53% 52% 51%
1.3
50% 48%
1.2 46%
1.1 44%
1 0.5
0.6
0.7
0.8
0.9
1.0
1.1
1.2
1.3
Eg3 = Subcell 3 Bandgap (eV)
• Raising band gap of bottom cell from 0.67 for Ge to ~1.0 eV for IMM GaInAs raises theoretical 3J cell efficiency R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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4-Junction Upright Metamorphic (MM) Terrestrial Concentrator Cell
metal gridline
1.8-eV (Al)GaInP cell 1 1.55-eV AlGaInAs cell 2 1.2-eV GaInAs cell 3 transparent buffer
0.67-eV Ge cell 4 and substrate
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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4-Junction Cell Optimum Band Gap Combinations 1.7
4-junction 1.9 eV/ Eg2/ Eg3/ 0.67 eV cell efficiency
Eg2 = Subcell 2 Bandgap (eV) .
2
1.6
o
500 suns (50 W/cm ), AM1.5D (ASTM G173-03), 25 C X Ideal efficiency -- radiative recombination limit
1.5 58%
1.4 56%
1.3 54%
1.2
50% 38%
46%
1.1 34%
42%
1 0.8
0.9
1.0
1.1
1.2
1.3
1.4
1.5
Eg3 = Subcell 3 Bandgap (eV)
• Lowering band gap of subcells 2 and 3, e.g., with MM materials, gives higher theoretical 4J cell efficiency R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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5-Junction Inverted Metamorphic (IMM) Cells
gro Ge o wt r G h s aA ub s str ate metal gridline
2.0-eV AlGaInP cell 1 1.7-eV AlGaInAs cell 2 1.4-eV GaInAs cell 3 transparent buffer
1.1-eV GaInAs cell 4 transparent buffer
0.75-eV GaInAs cell 5 R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Semiconductor-Bonded Technology (SBT) Terrestrial Concentrator Cell • Wafer bonding for multijunction solar cells – Low band gap cells for MJ cells using high-quality, lattice-matched materials – Epitaxial exfoliation and substrate removal – Formation of latticeengineered substrate for later MJ cell growth – Bonding of high-band-gap and low-band-gap cells after 1.4-eV GaInAs cell 3 growth 1.7-eV conductance AlGaInAs cellof 2 – Electrical semiconductor-bonded 2.0-eV AlGaInP cell 1 interface – Surface effects forGe GaAs or semiconductor-togrowth substrate semiconductor bonding
semiconductor bonded interface
GaAs or Ge metal gridline growth substrate GaAs or Ge growth substrate 2.0-eV AlGaInP cell 1 2.0-eV AlGaInP cell 1 1.7-eV AlGaInAs cell 2 1.7-eV AlGaInAs cell 2 1.4-eV GaInAs cell 3 1.4-eV GaInAs cell 3 1.1-eV GaInPAs cell 4 0.75-eV GaInAs cell 5
InP growth substrate
15
6-Junction Solar Cells
cap
(Al)GaInP Cell 1
2.0 eV
wide-Eg tunnel junction
GaInP Cell 2 (low Eg) 1.78 eV wide-Eg tunnel junction
AlGa(In)As Cell 3 1.50 eV
0.1
0.08 MJ cell 0.06
subcell 1 subcell 2 subcell 3
0.04
subcell 4 subcell 5
0.02
subcell 6 0 0
1
2
tunnel junction
GaInNAs Cell 5 0.98 eV tunnel junction
Ga(In)As buffer nucleation
Ge Cell 6 and substrate 0.67 eV back contact
4
5
6
7
AM1.5D, ASTM G173-03, 1000 W/m2 1.4 Utilization efficiency of photon energy 1-junction cell 3-junction cell 1.2 6-junction cell
700 Intensity per Unit Photon Energy (W/m 2 . eV)
Ga(In)As Cell 4 1.22 eV
3
Voltage (V)
wide-Eg tunnel junction
600 500
1
400
0.8
300
0.6
200
0.4
100
0.2
0
.
AR
AR
0.12
Photon utilization efficiency
contact
Current Density / Incident Intensity (A/W )
0.14
0 0
0.5
1
1.5 2 2.5 Photon Energy (eV)
3
3.5
4
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Modeled Terrestrial Concentrator Cell Efficiency Detailed balance limit efficiency Radiative recombination only Series res. and shadowing, optimized grid spacing Normalized to experimental efficiency
60%
3J 4J
Efficiency (%)
55%
50%
4J 3J
45%
4J
40%
3J
3J & 4J MM solar cells 35% 1
500
10 100 1000 10000 Incident Intensity (suns) (1 sun = 0.100 W/cm2)
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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High-Efficiency Multijunction Cell Results
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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LM and MM 3-Junction Cell Cross-Section contact
contact
AR
AR n+-Ga(In)As n-AlInP window n-GaInP emitter T
GaInP top cell
p-GaInP base
p-AlGaInP BSF
Wide-bandgap tunnel junction
p++-TJ n++-TJ
W
E eid
n-GaInP window n-Ga(In)As emitter
Ga(In)As middle cell
p-Ga(In)As base
p-GaInP BSF
Tunnel junction Buffer region
p++-TJ
M
id
g
e C
T el nn u T
e dl
e nn Tu
el C
p++-TJ n++-TJ
l
p-Ge base and substrate
M
id
d
el nn u T
g
le
el C
l
p-GaInP BSF p-GaInAs step-graded buffer
m tto o B
l
n tio nc
n-Ga(In)As buffer
n+-Ge emitter
W
E eid
n-GaInP window n-GaInAs emitter p-GaInAs base
u lJ
el C
op
p-GaInP base
p-AlGaInP BSF
n++-TJ
nucleation
Ge bottom cell
op
n+-GaInAs n-AlInP window n-GaInP emitter
ll
l Ce
l
contact
Lattice-Matched (LM)
p++-TJ n++-TJ
nucleation
n+-Ge emitter p-Ge base and substrate
e nn Tu
lJ
n io ct n u
m tto o B
Ce
ll
contact
Lattice-Mismatched or Metamorphic (MM)
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
19
New World Record 41.6% Multijunction Solar Cell • 41.6% efficiency demonstrated for 3J lattice-matched Spectrolab cell, a new world record • Highest efficiency for any type of solar cell measured to date • Independently verified by National Renewable Energy Laboratory (NREL) • Standard measurement conditions (25°C, AM1.5D, ASTM G173 spectrum) at 364 suns (36.4 W/cm2) • Lattice-matched cell structure similar to C3MJ cell, with reduced grid shadowing as planned for C4MJ cell
Ref.: R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009.
• Incorporating high-efficiency 3J metamorphic cell structure + further improvements in grid design → strong potential to reach 42-43% champion cell efficiency
Concentrator cell light I-V and efficiency independently verified by C. Osterwald, K. Emery – NREL
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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41.6% Solar Cell Eff., Voc vs. Concentration 44
Efficiency
42
0.96
Voc fit, 100 to 1000 suns 40
0.94
FF
38
0.92
36
0.90
34
0.88
32
0.86
30
0.84
28
0.82
26
0.80
24
0.78 1000.0
0.1
1.0
10.0
100.0
Fill Factor (unitless)
Efficiency (%) and Voc x 10 (V)
41.6%
Voc x 10
0.98
Incident Intensity (suns) (1 sun = 0.100 W/cm2)
• At peak 41.6% efficiency → 364 suns, Voc = 3.192 V, FF = 0.887 • Efficiency still >40% at 820 suns, at 940 suns efficiency is 39.8% • Diode ideality factor of 1.0 for all 3 junctions fits Voc well from 100 to 1000 suns R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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41.6% Solar Cell LIV Curves vs. Concentration Current Density / Incident Intensity (A/W)
0.16
41.6%
0.14 Inc. Intensity (suns) 2 1 sun = 0.100 W/cm
0.12
2.6
0.1
6.6
0.08
17.6 59.8
0.06 127.3 364.2
0.04
604.8
0.02
940.9
0 0
0.5
1
1.5
2
2.5
3
3.5
Voltage (V)
• At peak 41.6% efficiency → 364 suns, Voc = 3.192 V, FF = 0.887 • Series resistance causes drop in Vmp above 400 suns, Voc continues to increase • Efficiency still >40% at 820 suns, at 940 suns efficiency is 39.8% R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
22
Best Research Cell Efficiencies
Chart courtesy of Larry Kazmerski, NREL R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Spectrolab Cell Generations in DOE TPP Program 43% C4MJ
Production Cell Efficiency (%)
43
• Terrestrial concentrator cell efficiency
42
40%
41
• Goals in Technology Pathways Partnership (TPP)
40
38.5%
39
37%
38
37.5%
37 36 2007
2008
2009
2010
2015
Year R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Spectrolab C1MJ, C2MJ, and C3MJ Cell Products ηAVG = 38.2%
C1MJ
35%
C2MJ
30%
C3MJ
ηAVG = 37.5%
25%
ηAVG = 36.9%
20% 15% 10% 5%
39.5%
39.0%
38.5%
38.0%
37.5%
37.0%
36.5%
36.0%
35.5%
35.0%
34.5%
0% 34.0%
% of Population
40%
Efficiency η at Max. Power R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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Prototype 3J Metamorphic Cell Builds Corrected LIV Data for Prototype 3J Metamorphic (MM) 5%-In Cells 10 runs, 22 wafers, 205 cells
40.8%
40.5%
40.2%
39.9%
39.6%
39.3%
39.0%
38.7%
38.4%
38.1%
37.8%
37.5%
37.2%
36.9%
36.6%
36.3%
36.0%
35.7%
5% 3J-MM
3J MM Cell Efficiency Bin Average Std. dev.
Isc (A) 7.601 0.135
Voc (V) 3.090 0.022
FF 0.845 0.009
Eff 39.6% 0.8%
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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4-Junction Lattice-Matched Cell AR
AR cap
(Al)GaInP Cell 1
1.9 eV
wide-Eg tunnel junction
AlGa(In)As Cell 2 1.6 eV wide-Eg tunnel junction
Ga(In)As Cell 3 1.4 eV tunnel junction
Ga(In)As buffer nucleation
Ge Cell 4 and substrate 0.67 eV
Current Density / Incident Intensity (A/W )
0.25
contact
MJ cell subcell 1
0.2
subcell 2 subcell 3 0.15
subcell 4
0.1
0.05
0 0
1
back contact
2
3
4
5
Voltage (V)
• Current density in spectrum above Ge cell 4 is divided 3 ways among GaInAs, AlGa(In)As, GaInP cells •Lower current and I2R resistive power loss R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
27
100
1600
90
1400
80 1200
70
AlGaInP subcell 1 1.95 eV GaInAs subcell 3 1.39 eV All subcells
60 50
AlGaInAs subcell 2 1.66 eV Ge subcell 4 0.72 eV AM1.5D ASTM G173-03
40
1000 800 600
30 400
20 200
10 0 300
Intensity Per Unit Wavelength (W/(m2μ m))
External Quantum Efficiency (%)
Measured 4-Junction Cell Quantum Efficiency
0
500
700
900 1100 1300 Wavelength (nm)
1500
1700
1900
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
28
Light I-V Curves Record Efficiency Cells Current Density / Inc. Intensity (A/W) .
0.16 0.14 0.12 0.10 3J Conc. Cell
0.08
3J Conc. Cell
Metamorphic V oc Jsc /inten. V mp FF conc. area
0.06 0.04
Lattice-matched
2.911 0.1596 2.589 0.875 240 0.267
LM, 822 suns
3.192 V 0.1467 A/W 2.851 V 0.887 364 suns 0.317 cm2
Eff. 40.7%
41.6%
AM1.5D, low -AOD spectrum
0.02
3J Conc. Cell
3.251 0.1467 2.781 0.841 822 0.317
4J Cell 4.398 V 0.0980 A/W 3.950 V 0.856 500 suns 0.208 cm2
40.1%
AM1.5D, ASTM G173-03
4J Conc. Cell
36.9%
AM1.5D, ASTM G173-03
Independently confirmed meas. 25°C
AM1.5D, ASTM G173-03 Prelim. meas. 25°C
0.00 0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
Voltage (V)
• Light I-V curves for 3-junction upright MM (40.7%), 3J lattice-matched (41.6%), 3J lattice-matched at 822 suns (39.1%), and 4J lattice-matched cell (36.9%) R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
29
The Solar Resource and CPV Economics
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
30
The Solar Resource
5 6
Ref.: http://rredc.nrel.gov/solar/old_data/ nsrdb/redbook/atlas/
• Entire US electricity demand can be provided by concentrator PV arrays using 37%-efficient cells on: 150 km x 150 km area of land
or or
ten 50 km x 50 km areas similar division across US
R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
31
Concentrator Photovoltaic (CPV) Electricity Generation
CPV cost superiority 40% cell efficiency
CPV cost superiority 50% cell efficiency
Map source: http://www.nrel.gov/gis/images/map_csp_us_annual_may2004.jpg
Higher multijunction cell efficiency has a huge impact on the economics of CPV, and on the way we will generate electricity. R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
32
Summary • Urgent global need to address carbon emission, climate change, and energy security concerns → renewable electric power can help • Theoretical solar conversion efficiency – Examining built-in assumptions points out opportunities for higher PV efficiency – Multijunction architectures, up/down conversion, quantum structures, intermediate bands, hot-carrier effects, solar concentration → higher η – Theo. solar cell η > 70%, practical η > 50% achievable
• Metamorphic multijunction cells have begun to realize their promise – Metamorphic semiconductors offer vastly expanded
of band gaps
– 40.7% metamorphic GaInP/ GaInAs/ Ge 3J cells demonstrated – First solar cells of any type to reach over 40% efficiency
• New world record efficiency of 41.6% demonstrated – Highest efficiency yet measured for any type of solar cell – 41.6% efficiency independently verified at NREL (364 suns, 25°C, AM1.5D)
• Solar cells with efficiencies in this range can transform the way we generate most of our electricity, and make the PV market explode R. R. King et al., 24th European Photovoltaic Solar Energy Conf., Hamburg, Germany, Sep. 21-25, 2009
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