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Photovoltaics for the Terawatt Challenge

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Photovoltaics for the Terawatt Challenge Christiana Honsberg Department of Electrical Computer and Energy Engineering Director, QESST ERC Arizona State University – PowerPoint PPT presentation

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Title: Photovoltaics for the Terawatt Challenge


1
Photovoltaics for the Terawatt Challenge
  • Christiana HonsbergDepartment of Electrical
    Computer and Energy Engineering
  • Director, QESST ERCArizona State University

2
Outline
  • Terawatt Challenge
  • What is it?
  • Photovoltaics for the TW challenges
  • Importance of rapid growth
  • Recent milestones in PV
  • But what about ..
  • Myths of photovoltaics land area efficiency
    energy payback time materials availability time
    to impact duck curves, etc
  • Future prospects
  • Education

3
Terawatt Challenge
  • Terawatt Challenge Encapsulates the dichotomy
    surrounding energy essential for improved
    quality of life, but also tied among the most
    serious global challenges.

4
Terawatt Challenge
  • Why is compound annual growth rate important?

5
Terawatt Challenge
  • In the nearly two decades since the TW challenge
    paper, renewables have reached multiple
    milestones
  • In US, renewable compound annual growth rate 4.8
    from 2000-2012 (NREL data)

NREL,2012 Renewable Energy Data Book
6
Photovoltaic Milestones
  • Germany, Spain, Italy have yearly installed PV
    capacity gt yearly increase in electricity demand.
  • In Germany, PV is 50 of summer peak electricity
    demand

7
Learning Curves for Photovoltaics
  • PV learning curves show compound annual growth
    rate (CAGR) of 30 over the last several decades
  • Extending the growth rates shows ability of PV
    (renewables more generally if these are included)
    to make a substantial impact on electricity
    generations

8
Potential for PV in the US
9
Photovoltaic Milestones
  • ASU reached 50 of total electricity supplied
    by PV

10
Arizona Context
11
Photovoltaics FAQ
  • Energy payback time
  • Land use
  • Cost
  • What do you do at night for power?
  • Materials availability
  • For silicon, limitation is silver in grids, which
    cause a limitation at 2 TW
  • Availability subject to efficiency, thickness

12
Duck Curves
  • Power after sun goes down a concern for
    utilities.
  • Can mitigate by load management.

13
PV for the Terawatt Challenge
  • PV technology must be high efficiency, efficient
    use of materials, scalable, reliable, and enable
    path for future improvements
  • High efficiency overcome limits thin

14
Present State of PV efficiencies
15
Fraction of Efficiency Achieved
16
Types of PV Systems
  • Optical configuration of photovoltaic systems
    One-sun or flat plate concentrating systems
    tracking

17
Scope of QESST ERC
18
Multiple Junction (Tandem) Solar Cells
  • Concentration or stacking multiple solar cells
    increases efficiency
  • To reach gt50 efficiency, need ideal bandgap
    6-stack tandem, (assuming 75 of detailed
    balance limit).
  • Hard to get compatible materials with the right
    bandgaps.

APS Tutorial Nanostructured Photovoltaics
C.Honsberg 18
19
What do efficiency calculations tell us?
  • Approaches to high efficiency
  • Concentrate sunlight. One sun 1kW/m2, max
    concentration 46,000.
  • No entropy penalty for concentrating sunlight,
    but etendue limits to acceptance angle and
    concentration.
  • Optically split solarspectrum (i.e. tandem)
  • No entropy penalty
  • Efficiency controlled by existence of materials
  • Beneficially circumventone of the assumptionsin
    thermodynamics

20
Tandem Solar Cells
  • Key issue for III-Vs need precisely controlled
    band gaps which are lattice matched
  • Missing low band gap material
  • Approaches
  • Lattice matched Ge-GaAs-GaInP
  • MetamorphicGe-GaInAs-GaInP
  • Metamorphic GaInAs-GaAs-GaInP
  • Band gaps for 4-tandem arepoorly lattice
    matched5 band gapsand six band-gaps are better
    matched

21
Ge-based tandem solar cells
  • Metamorphic solar cell reached 40.7 at 200X.

22
Carrier-Selective Contacts
  • Carrier-selective contacts enable ideal VOC

23
CSC Implementation a-Si/c-Si solar cell
  • Demonstrated 746 mV on 50 µm wafers

24
InAs QDs on GaAsSb barriers
  • InAs QDs achieved on GaAsSb material
  • Increasing Sb composition decreases QD size and
    increases QD density

InAs QDs on GaAs (5 ML) / GaAs1-xSbx (5nm) buffer
layers with x 23, with density 2.6 x 106 cm-2
InAs QDs on GaAs
25
Experimental GaAsSb/InAs QD material
  • Doping of QD layers to control occupancy of the
    QD.

GaAsSb/GaAs interface
26
Tandem Solar Cells
  • Monolithic III-V tandem solar cells Series
    connected three junctions
  • High efficiency used in high concentration,
    two-axis tracking systems
  • High concentration meanssmall area (and lower
    cost) needed for solarcells
  • Trade balance of systemsand solar cell cost.

27
Experimental GaAsSb/InAs QD material
28
Path for Continual Improvement
  • Ideal solar cell consists of a light-trapped,
    thin solar cell
  • Nanostructured surfaces allow light trapping and
    advanced concepts (e.g., multiple exciton
    devices)

29
Student Led Pilot Line
  • Silicon pilot line capabilities for interaction
    among students, industry and researchers
  • 10 Fulton Undergraduate Research Initiative
    Projects
  • 2 honors thesis
  • 4 capstone projects

30
  • Questions?
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