pv review - nov 2013 - the menon group · pdf filespace&charge®ion& 4. ......
TRANSCRIPT
Review of Photovoltaic Solar Cells
Op5cs for Energy Course 11/5/13 Liz Lund
Outline • Solar electricity produc5on • How Photovoltaics (PV) work • Types of PV • Emerging technologies
Solar Electricity Produc5on
hIp://www.nrel.gov/docs/fy13os5/54909.pdf
Renewables in US
~10% Renewable Energy in US Solar is a small frac5on 0.1%
Global vs. US Renewable Energy • Same trends for PV
global and in US • Wind and solar are
fastest growing renewables in US
• Wind 17% • Solar 86%
hIp://www.nrel.gov/docs/fy13os5/54909.pdf
Solar Growth is Exponen5al
Solar electricity genera5on grown by a factor of 9 (2000 to 2011)
Who’s Making It?
Where is it Installed?
Where in US?
States with extensive incen5ves lead PV deployment
Solar Prices
hIp://www.resilience.org/stories/2013-‐04-‐25/solar-‐energy-‐this-‐is-‐what-‐a-‐disrup5ve-‐technology-‐looks-‐like
99% cost drop since 1977
Solar becoming compe55ve with fossil fuel generated energy
Swanson’s Law: PV costs drop 20% for every doubling of shipped volume
$.50/waI
How Photovoltaics Work
Photovoltaic Solar Cells: Light In, Electricity Out
3 Necessary Func-ons:
1. Generate charge carriers from light semiconductor + sunlight
2. Separate charge carriers
p-‐n junc5on (diode)
3. Collect charge carriers to do electrical work carriers reach front and back contacts
Typical CZTS(Se) Solar Cell Stack
Glass
1 µm CZTS(Se)
Mo
300 nm ZnO
50 nm CdS
Ni/Al
50 nm i-‐ZnO
1
2
3
3
2
Front Contact
Back Contact
Absorber Layer
Transparent Conduc5ng Oxide
Solar Cell, Module, Array
Undoped Si Laice
“Missing” electron Hole
B Doped Si
p-‐Type extra holes
“Extra”electron
P Doped Si
n-‐Type extra electrons
B
Boron
Si
Silicon Phosphorous
P
n-‐ and p-‐type semiconductors
+ -‐
p-‐Type extra holes
n-‐Type extra electrons
-‐
-‐
-‐
-‐
+
+
+
+
1. n-‐ and p-‐type materials separate are neutral
2. Place materials together • Free electrons and holes
diffuse and recombine • Leave behind charged
nuclei (localized)
3. Create charged interface • Charge build-‐up repels
complete diffusion • At equilibrium, establish
space charge region 4. Built in voltage poten5al
• Diode behavior of pn junc5on
Space Charge Region
Making a Diode
The Band Gap: Energy barrier to genera5ng charge carriers
Atoms in a Crystal Energy Bands
Individual Atoms Discrete Energy
States
Energy
p
s
Energy Gap
Conduc5on Band
Valence Band
Band Diagram
EC
EV
Eg
hIp://pveduca5on.org/pvcdrom/pn-‐junc5on/band-‐gap
Conduc-on band (of states): Higher energy state Electrons are delocalized Free to move throughout crystal Formed from an5-‐bonding orbitals in crystal
Valence band (of states): Lower energy state Electrons are localized around atomic nuclei Formed from bonding orbitals in crystal
Genera5ng Charge Carriers-‐Absorp5on of Light
hIp://pveduca5on.org/pvcdrom/pn-‐junc5on/absorp5on-‐of-‐light
Semiconductor only absorbs light with energy equal or greater than the band gap (lower wavelength) Ideal band gap: 1.1 eV Lower band gaps give lower voltage (current losses)
Absorp5on Coefficient-‐PV Material Property
hIp://www.pveduca5on.org/pvcdrom/pn-‐junc5on/absorp5on-‐depth
Schockley-‐Quiesser Limit
η = 33.7% theore5cal maximum for single pn junc5on cell with no concentra5on PloIed with actual record efficiencies of different materials What limits this? (33% example) • 47% to heat. • 18% not absorbed. • 2% local recombina5on of holes
and electrons. Passing the Limit: Use mul5ple materials Have mul5ple pn junc5ons Concentrate sunlight Harvest heat also Use “quantum dots” to harvest excess photon energy
Device Parameters • JV Curve
• Jsc • Voc • Resistances
• Series-‐contact and current movement • Shunt-‐manufacturing defects
• Fill Factor • Max Powerpoint
• Efficiency • IQE • EQE
hIp://www.pveduca5on.org/pvcdrom/solar-‐cell-‐opera5on/light-‐generated-‐current
hIp://www.pveduca5on.org/pvcdrom/solar-‐cell-‐opera5on/iv-‐curve
JV Curve
Maximum power point
Series Resistance Slope of Line
Shunt Resistance Slope of Line
Types of PV
hIp://www.nrel.gov/ncpv/images/efficiency_chart.jpg NEED MORE BULLET POINTS
Classes of PV
• Thin Film – 1-‐2 um thick – “dirty” deposi5on methods – Op5cally thin-‐use op5cs to compensate – More defect tolerant – CIGS, CdTe, CZTS, a-‐Si – Deposit on flexible substrates
• Thick – 100’s of um thick – Typically c-‐Si – Must be very pure for carrier diffusion
• Monocrystalline – Con5nuous crystal laice – Expensive produc5on – Higher efficiencies in cells
• Polycrystalline – Many grains (um-‐cm size) – More grain boundaries=more defects – Most thin films
Projected Cell Produc5on Market Shares 2011
hIp://www.posterus.sk/?p=1247
• Energy Payback Time – 10% CIGS, 4% OPV …1 yr – c-‐Si …2.7 yrs
Technology 2004 2009 2012 Record Cell
Super Moncrystalline Silicon 16 19.3 20.1 25
Monocrystalline Silicon 12.8 15 16 25
Mulitcrystalline Silicon 12.5 14 14.5 20.4
CdTe 7.6 11 12.6 17.3
CIGS 10 12 13.3 20.3
µc-‐Si, a-‐Si n/a 8.5 10.2 12.5
a-‐Si (3-‐j) 6.7 8.3 9.7 12.5
a-‐Si (1-‐j) 6.5 6.7 7.5 10
Organic n/a 3.5 4.2 10.1
Commercial vs. Record % Efficiencies
Comparing PV Technologies
Emerging PV
hIp://www.nrel.gov/ncpv/images/efficiency_chart.jpg NEED MORE BULLET POINTS
Perovskite Solar Cells
hIp://news.sciencemag.org/physics/2013/09/flat-‐out-‐major-‐advance-‐emerging-‐solar-‐cell-‐technology
Dye-‐Sensi5zed Solar Cells
Organic/Inorganic Hybrid Cheap to make Life5me? 3 different materials: 1. Light absorp5on
Sensi5zing (organic) dye 2. Electron transport
Wide band-‐gap (inorganic) semiconductor
3. Hole transport/electron regenera5on Electrolyte
1
1
2
2 3
3
Hardin et al., Nature Photonics (2012)
Mul5-‐junc5on PV
Thin top layers absorb shorter wavelengths Longer wavelengths in boIom cell Tunnel diode allows current flow but electrical field isola5on of top and boIom cells Expensive to make Crystalline laice and currents must match-‐really difficult and constrains materials! Currently only used in space World Record: 43% with 5-‐tandem cell UNSW
Concentra5ng PV (CPV)
Focus light using mirrors, lenses Use small area, high efficiency cells
Addi-onal requirements • Non-‐imaging op5cs-‐focus on
radia5ve rather than image transfer • Trackers-‐2D east to west each day,
north to south each season • Cooling system
hIp://newenergynews.blogspot.com/2009/07/concentra5ng-‐photovoltaics.html hIp://amonix.com/content/low-‐energy-‐produc5on-‐costs-‐0
CPV cont’d Advantages • Very efficient, less space • Low water usage, advantage over
tradi5onal solar thermal concentrators (4 vs. 850 gal/MWhr)
• Lower cost of materials, majority of infrastructure is not PV
• Well-‐suited for large power plant arrays
• Nearing grid parity now!
Disadvantages • Requires direct sunlight • New technology-‐late to the funding game • Trackers are expensive
Suited for desert climates especially
Earth-‐Abundant Thin Films
Large-‐scale PV should use earth-‐abundant and industrially-‐available elements to avoid boIlenecks
“commodity elements”
Abundance in Earth’s Crust World Annual Produc-on (tons)
We use these currently We use these currently
Phillip Dale
PV materials cost-‐Red Herring
• First Solar: ‘Module shipping box cost higher than CdTe material cost’ • Glass for panel much more expensive than 1 cm3 semiconductor film (>100x) • Absolute semiconductor materials costs insignificant!
Typical Module = few hundred $
$$
Winning Argument-‐TW Scale-‐Up Poten5al
• Sulfur: byproduct of Cu, Zn ores & fossil fuel produc5on
• More cm3/kg from light elements
• Many sulfides have right EGap
Fthenakis, Ren. Sus. Ener. Rev. 13 2746 (2009)
In or Te produc9on limits: CIGSe & CdTe: ~150 GWP/yr
CZTS-‐CIGS with no Indium
• Kesterite structure (like chalcopyrite)
• EGap = 1.5 eV, direct gap
• First PV inves5ga5ons in late 1990’s – Katagiri – Friedlmeier
η = 11% for evaporated cells* (IBM)
Chen APL (2009) *Wang APL 97 143508 (2010)
Summary
• Photovoltaic solar cells needs 3 things – Genera5on of charge carriers-‐semiconductor with band gap
– Separa5on of carriers-‐pn junc5on – Collec5on of current to do electrical work
• Variety of technologies that get the job done • C-‐Si s5ll dominate the market • It’s geing cheaper faster