P627 S13 L24 22Apr2013 Zimmermann Photovoltaics
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Transcript of P627 S13 L24 22Apr2013 Zimmermann Photovoltaics
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Photovoltaic
Energy Conversion
Frank Zimmermann
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Solar Electricity Generation
Consumes no fuel
No pollution
No greenhouse gases
No moving parts, little or no maintenance
Sunlight is plentiful & inexhaustible
Cost competitive with fossil fuels/nuclear. Cost
coming down every year.
Considerably cheaper than electricity from coal if cost
of carbon capture is factored in
Great promise for solving global warming and fossil
fuel depletion problems!
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Photovoltaics: Explosive Growth
Sustained growth of 30 – 50 % per year
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Extrapolation of historical PV
module prices
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Actual 2013 PV Module Cost:
~ 50 cents/Watt!
“Grid Parity” has been reached in India, Italy, Spain, and other
countries
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Challenges
Make solar cells more efficient
Theoretical energy conversion efficiency limit of single junction solar cell is 31%
Actual efficiencies are even lower: ≤ ~20%
Make solar cells cheaper
“Grid Parity” has been achieved in some countries, others are soon to follow
Require high reliability, long service life
Use only abundant, nontoxic materials
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Power reaching earth 1.37 KW/m2
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Solar cell – Working Principle
Operating diode in fourth quadrant generates power
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Semiconductor Bandgaps
Crystalline silicon is by far the most important PV material.
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Thin Film Solar Cells
Produced from polycrystalline thin films
Cheaper than single crystal silicon
High optical absorption coefficients
Bandgap suited to solar spectrum
Poly-Si
CdTe
CIGS (Copper-Indium-Gallium-Selenide)
Organic and Dye-Sensitized Solar Cells
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CuInSe2 (with Ga: “CIGS”)
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CIGS Solar Cell
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Band Diagram CIGS Solar Cell
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Organic Solar Cells
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Plasmon Resonances of Metal
Nanoparticles
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Plasmon Resonances of Metal
Nanoparticles
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Light Concentration using
Nanoparticle Plasmon Resonances
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Dye Sensitized Solar Cells
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Dye Sensitizer Molecules
N
N
N
N Pd
COOH
COOH
HOOC
COOH
N NNN Pd
O
HO
OHO
O
OH
OH
O
N N
NN
Pd
OH
OO
OH
1a 1b 2
N
N
N
N Pd
COOH
COOH
HOOC
COOH
N NNN Pd
O
HO
OHO
O
OH
OH
O
N N
NN
Pd
OH
OO
OH
1a 1b 2
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Dye Sensitized Solar Cells
EF
EF
Transparent
Conductive
Oxide
TiO2 Nanoparticles Electrolyte Counter
Electrode
Valence Band
Conduction Band
Fermi Level
I-/I3
-
Redox
Potential
Dye
1D
3D*
1D*
Energy Levels (Illuminated)
Photo
Voltageh
Injection
EFEF
Transparent
Conductive
Oxide
TiO2 Nanoparticles ElectrolyteCounter
Electrode
Valence Band
Conduction Band
Fermi Level
I-/I3
-
Redox
Potential
Dye
1D
3D*
1D*
Energy Levels (Dark)
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Efficiency Losses in Solar Cell
1 = Thermalization loss
2 and 3 = Junction and contact voltage loss
4 = Recombination loss
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Conversion Efficiency Limits
Thermodynamic limit:
Carnot efficiency: 1 − 𝑇𝑐
𝑇𝑠= 1 −
300𝐾
6000𝐾= 0.95
Ultimate efficiency (T = 0) for single junction: 45%
Detailed balance limit for single junction:
Shockley and Queisser (1961)
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Ultimate Efficiency
Sub-bandgap photons are not absorbed:
Carrier relaxation to band edges:
Photon energy exceeding bandgap is lost electron
hole
gap photon
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Ultimate Efficiency
Let Q(T) be the photon flux in blackbody radiation of
temperature T with photon energy ℎ > 𝐸𝑔:
𝑄 𝑇 = 2
𝑐2
2𝑑
𝑒ℎν/𝑘𝑇 − 1
∞
𝐸𝑔/ℎ
photon flux = number of photons / (unit area unit time)
The total energy flux in the blackbody radiation is:
𝐼𝑠 = 2ℎ
𝑐2
3𝑑
𝑒ℎν/𝑘𝑇 − 1
∞
0
Energy flux = energy / (unit area unit time)
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Ultimate Efficiency
Incident solar power: 𝑃in = 𝐴 𝐼s
Electrical output power: 𝑃out = 𝐴 𝐸g𝑄 𝑇s
Ultimate efficiency: ult =𝑃out
𝑃in=𝐸g𝑄(𝑇s)
𝐼s
• For 𝑇s = 6000 K, the ultimate efficiency is maximized for a band gap
of 𝐸g = 1.1 eV, reaching ult ≈ 45%.
• Ultimate efficiency can only be achieved if there is perfect
absorption of blackbody radiation at 𝑇 = 𝑇s and the cell
temperature 𝑇c = 0.
• It does not take into account carrier recombination, which must
occur at 𝑇c > 0.
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Detailed Balance Limit
For finite cell temperature, need to take into account
carrier recombination.
Use the principle of detailed balance (Shockley and
Queisser, 1961).
First consider solid angle of sun, as seen from earth:
sun
solar cell
(area A)
solid angle
• = 6.85 × 10−5 steradians
(no concentration)
• may be greatly enhanced
using solar concentrators
(lenses, parabolic reflectors).
• Set 𝜃 = 0 from here on (normal
incidence).
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Detailed Balance Limit
Incident solar power (= absorbed power)
𝑃s = 𝐴 𝐼s
# of e-h pairs created (given by # of absorbed photons):
𝐹s = 𝐴 𝑄(𝑇s)
Now consider solar cell in thermal equilibrium, i.e.,
surrounded by a box at 𝑇 = 𝑇c:
𝐹c = 2 𝐴 𝑄(𝑇c) = recombination rate 𝑇c 𝑇c
both sides
e-h pair creation rate =
“detailed balance”
𝐹𝑐 = 𝐹𝑐 0 (zero voltage)
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Detailed Balance Limit
From the Fermi distribution: (β =1
𝑘𝐵𝑇 )
𝑛 = 1
𝑒β(𝐸𝑐−μ𝑛)+1 ≈ 𝑒−𝛽 𝐸𝑐−μ𝑛 𝑝 = 1 −
1
𝑒β(𝐸𝑣−μ𝑝)+1
≈ 𝑒𝛽 𝐸𝑣−μ𝑝
thus 𝑛 𝑝 = 𝑒−𝛽𝐸𝑔 𝑒𝛽𝑞𝑉 (𝑞𝑉 = μ𝑛 − μ𝑝)
and 𝐹𝑐 𝑉 = 𝐹𝑐 0 𝑒𝛽𝑞𝑉
electron density
hole density
V
𝐸𝑐
𝐸𝑣 μ𝑝
μ𝑛
Apply a voltage V across the junction:
recombination rate:
𝐹𝑐 𝑉 ∝ 𝑛 𝑝
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Detailed Balance Limit
Photocurrent:
𝑖 = 𝑞 𝐹𝑠 − 𝐹𝑐 𝑉 = 𝑞 𝐹𝑠 − 𝐹𝑐 0 𝑒𝛽𝑞𝑉
number of e-h pairs created
recombination rate
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Detailed Balance Limit
Output power: 𝑃out = 𝑖𝑉 = 𝑞 𝐹𝑠 − 𝐹𝑐 0 𝑒𝛽𝑞𝑉 𝑉
Maximize output power: set 𝑑(𝑖𝑉)
𝑑𝑉= 0, solve for 𝑉max
𝑖max = 𝑖(𝑉max)
Maximum output power: 𝑃max = 𝑖max𝑉max
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Detailed Balance
Limit
maximum efficiency:
max =𝑃max
𝑃s=𝑖max𝑉max
𝐴𝐼sΩ/𝜋
re-write in terms of ultimate efficiency ult =𝐸g𝐹s
𝑃s and
short-circuit current 𝑖sh = 𝑖 0 = 𝑞 𝐹s − 𝐹c(0) ≈ 𝑞𝐹s :
max = ult 𝑞 𝑉oc
𝐸g 𝑉max
𝑉oc 𝑖max
𝑖sh
reduction of 𝑉oc from zero-temperature value 𝐸g
𝑞
“fill factor”
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Detailed Balance Limit
In the limit 𝑇𝑐 → 0, the efficiency max → ult
This is an idealized result. In real life, < max due to
non-radiative recombination, contact resistance,
reflection losses, etc.
ult 31% for 6000 K blackbody
(no concentration)
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Strategies to Exceed Shockley-
Queisser Efficiency Limit:
Multi-junction cells (“Tandem cells”)
Multiple electron-hole pairs per photon
Intermediate-band solar cells
Quantum-dot solar cells
Thermophotovoltaic cells
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Multiple Junctions: Tandem Cells
Current output matched for individual cells
Ideal efficiency for infinite stack is 86.8%
GaInP/GaAs/Ge tandem cells (efficiency 40%)
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Triple Junction Solar Cell
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Triple Junction Solar Cell
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Triple Junction Solar Cell
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Multi-Junction Solar Cells
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Multiple E-H pairs
Many E-H pairs created by incident photon
through impact ionization of hot carriers
Theoretical efficiency is 85.9%
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Intermediate-Band PV cell
Intermediate band created by:
• Impurity levels
• Quantum dot states (“quantum dot solar cell”)
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Thermophotovoltaic Cell
Filter passes photons of energy equal to bandgap of solar cell material
Emitter radiation matched with spectral sensitivity of cell
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Thermophotovoltaic Cells
Theoretical efficiency almost twice of ordinary
photocell
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Comparison and history of
PV conversion efficiencies