3. The use of π-conjugated organic materials in the production of electronic devices
Light weight
Flexible
Low-cost production
http://www.youtube.com/watch?v=TDuP8PtDJbE&feature=related
Motivation : Why Organic ?
7. Van der Waals forces instead of
covalent bonding between polymers
• narrow bands with low delocalization
Conjugated molecules tend to
change their geometry upon charging
• electron-phonon coupling
Electron-phonon coupling leading to a deformation of the lattice
structure of the semiconductor
• Lattice
• Electron
• Electron-phonon coupling
Hamiltonian
composed of
components
for
Charge transport Energy
12. rst is the fraction of singlet excitons,
q is the efficiency of radiative decay of these singlet excitons
Understanding Efficiency
circuitexternalin theflowingelectrons#
devicehewithin teventsformationexciton#
13. Organic Photovoltaics
Source : KonarkaC. W. Tang, Appl. Phys. Lett. 1985, 48, 183
Major Milestone :
Tang reported single
heterojunction device OPV
in 1985 with a power
efficiency of 1%
High optical absorption
coefficients of organic
molecules thinner solar
cells
14. Photon
Absorption ~1fs
ηa
Exciton
Formation
~100fs to 1ns
Exciton Diffusion
~ 1ns
ηED
Exciton Breakup
~ 100 fs
Charge transport
ηCT
Charge
Collection ~1 us
ηCC
OPVs : Device Physics
A
N
O
D
E
C
A
T
H
O
D
E
-
+
LUMO
HOMO
Light
External Quantum Efficiency(EQE) = ηa ηED ηEB ηCT ηCC
DONOR ACCEPTOR
15. Characterization
IV Characteristics
η = maximum
deliverable
electrical
power(VM ×JM)
to the incident
light power(Pinc)
FF = Fill Factor
VOC = Open Circuit
Voltage
JSC= Short Circuit
Current
16. Materials,
• Printing
– Screen Printing
– Stamping
• Spraying
• Spin Coating
• Vaporization
Acceptors
PCPDTBT,
MEH-PPV,
P3HT, PTB1
Donors
PCDTBT,
PCBM,
PSBTBT
Electrode
Al, Ca, Ag
Transparent
Electrode
PEDOT:PSS,
ITO
Krebs F. C., Solar Energy Materials & Solar Cells 93 (2009) 394–412
Processes
17. Organic Solar Cell Architectures
Planar Heterojunction
Typically exciton diffusion length = 10 nm
Layer width limited
But atleast should be 100 nm to absorb light
completely
Glass
Transparent Electrode
Donor Layer
Acceptor Layer
Metal Electrode Bulk Heterojunction
Ordered
Heterojunction
18. Now, actual Solar Cells can be complex…
Stacking improves efficiency
Adding more
layers for hole
injection and
electron
injection adds
to the cells
efficiency
19. Tandem Cell is better
Tandem Cell
Jsc = 7.8 mA/cm2, Voc = 1.24 V, FF =
0.67, and ηe = 6.5%
www.sciencemag.org SCIENCE VOL 317 13 JULY 2007 pp. 223-225
21. State of the art :
• Spin coating
– Can coat large areas with
high speed
– Redissolution
– Patterning not possible as
• Vapour Evaporation
– Layer by layer without
chemical interaction in
vacuum
– Non uniform, requires
UHV, expensive,
contamination, LOS
• Vapour Deposition
– Better control through gas
flow rate and temperature
– Uniformity and not
contaminated
22. State of the art : Photocrosslinking
Photolysis of FPA gives singlet nitrene
which inserts into C-H bonds of polymers
to form crosslinks
Effective crosslinker conc is low !!
23. FPA Methodology
Roll 2 Roll Manufacturing
DUV
Solvent
Wash
Spin Coating/ Ink Jet Printing
DUV
Solvent
Wash
24. Key Advantage : Continuity for e and h conduction paths is guaranteed.
Contiguous Interpenetrating Structure for PVs
25. Using Photocrosslinking for PVs
A factor of 4.5 improvement is
achieved
internal recombination bottleneck
overcome
26. Photocrosslinking possible without
significant loss of device properties
4.5% external photons per injected
electron
Similar life time
Similar results for other types of PPV
Can we make heterostructures?
PLEDs using PHOTOCROSSLINKING
27. ITO
TFB the hole-transporting and
electron-blocking interlayer
F8BT the electron-transport
and light-emitting layer
Can we make
heterostructures?
28. For solution-processed polymer OSCs,
however, this is a considerable challenge
because of redissolution, and the difficulty of
fixing a p-i-n profile -> photocrosslinking!!!
For molecular organic semiconductors
(OSCs), doping is readily achieved by
coevaporation of the dopant with the
transport layer (eg. by CVD)
Observation of p-doping with sodium
naphthalenide (Na+Np−) from transmission spectra:
the band at 2.7 eV bleaches while a sub-gap
polaron transition emerges at 1.8 eV
Observation of n-doping with nitronium
hexafluoroantimonate (NO2
+SbF6
−)from transmission
spectra: the band bleaches while a different subgap
polaron transition emerges at 2.1 eV
DOPING
Sivaramakrishnan et al, APL 2009
29. Efficient bipolar injection
Greatly improved external electroluminescence
efficiency compared to control devices without the p-i-
n structure
photocrosslinking of the first layer
bulk p-doping by diffusion of solution-state dopant,
deposition of an intrinsic polymer layer
solid-state surface n-doping to limit the doping depth in
this layer
Methodology
30. Organic PV Road Ahead…
Presented at Large Area, Organic & Printed Electronics Convention, 2010
32. Challenges
Material Level
• OPV: Low bandgap polymers with absorption edge at 1eV, large absorption
coefficients, higher charge mobilities
• OLED: Low work function cathodes with higher stability
• Minimise Energy Loss at junctions
Process Level
• To be able to create nanostructures with appropriate domain size and dimensions
Device Level
• Increase power conversion efficiency
• Increase stability
• Reduce costs
• Develop a technology for large scale production and reproducibility
• Ruggedness FlexibilityTransparent
33. Summary
• Organic Electronics has tremendous potential of
replacing the present rigid electronics.
• However, there are issues of cost-efficiency tradeoff
which need to be dealt with.
• Competitive research among the companies is
empowering the progress of organics.
• Dynamic and highly interdisciplinary field:
physicists, chemist, material scientists, electrical
engineers … truly Nano!