Madrid, 7 th February 2008 Confidential 1 IBPOWER kick-off Meeting “Growth and Fabrication of Intermediate Band Solar Cells designed for concentration”

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Madrid, 7Madrid, 7thth February 2008 February 2008 ConfidentialConfidential

11

IBPOWER kick-off MeetingIBPOWER kick-off Meeting

“Growth and Fabrication of

Intermediate Band Solar Cells

designed for concentration”

Corrie Farmer and Colin Stanley

University of Glasgow

Madrid, 7Madrid, 7thth February 2008 February 2008 ConfidentialConfidential

22

Standard (Al,Ga)As heterojunction solar cell

GaAs reference/IBSC layer structureGaAs reference/IBSC layer structure

QD density ~1-2x1010 cm-2

Si -doping to give one electron per dot 10-50 layers of QDs

Donor impurities

QD QD WL

n+ -substrate

n+ -Al 0.2Ga 0.8As

n-GaAs

p+p+ -GaAs

n-metal contact

Metal contact on p+-GaAs layer

SiNx ARC, Al0.85Ga0.15As window layer

IBSC - InAs QD layers incorporated into n-GaAs “base”

Madrid, 7Madrid, 7thth February 2008 February 2008 ConfidentialConfidential

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Overview of device fabricationOverview of device fabrication

Cross-sectional schematic

Madrid, 7Madrid, 7thth February 2008 February 2008 ConfidentialConfidential

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Solar cell characteristics (one sun)Solar cell characteristics (one sun)

Good efficiency of GaAs reference cell.

Lower efficiency for prototype IBSC.

Reduced VOC.

Photocurrent from IBSC due to absorption of sub-

bandgap photons (2+2) with EIB-EVB<Ehf<Eg.

Photocurrent due to absorption of two sub-bandgap

photons (2+3), one with Ehf~ECB-EIB

IB

CB

VB

2 1

23

Madrid, 7Madrid, 7thth February 2008 February 2008 ConfidentialConfidential

55

Plans for next 6 monthsPlans for next 6 months

Design for concentration Minimize series resistance Increase the open circuit voltage, Voc

MBE growth of IBSC structure Maximize IB-CB separation (total In content per QD

layer) Maximize current produced by absorption of sub-

bandgap photons (total number of QD layers) Optimize spacer thickness between QD layers (coupled

or uncoupled QDs??)

Fabrication of solar cells using; ~5 μm thick electro-plated Au-grid for top electrode Optimal grid geometry Two-layer ARC Heat sink

Characterisation by PL/EL/FTPS using FTIR spectrometer 400 500 600 700 800

0

10

20

30

40

50

60

70

Day 0 Day 3 Day 6 Day 20 Day 20+ ZnS/MgF

2 ARC

Ref

lect

aan

ce (

%)

Wavelength (nm)

Stabilised uncapped Al0.9

Ga0.1

As Window Layer

1

o

LBoc J

Jn

q

TnkV

Madrid, 7Madrid, 7thth February 2008 February 2008 ConfidentialConfidential

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Further afield – strain balancing on InPFurther afield – strain balancing on InP

V M Ustinov et al., Semiconductors Vol. 31 (10), p1080, 1997

In(Al,Ga)AsInAs QD layer

In(Al,Ga)As layer with In fraction reduced below lattice-matched value

InAs QDs embedded in In0.53Ga0.47As on InP

InP

At 300 K;Eg(InP) = 1.35 eV, Eg(InAlAs) = 1.46 eV

In theory, this should permit an “unlimited” number of QD layers to be stacked one on top of the other

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