Abstract:
During the last decade, different structures of photovoltaic (PV) cells fabricated from
organic semiconductors have drawn tremendous economic and scientific interest due to
their high optical absorption efficiency, low fabrication cost, lightweight, high
mechanical flexibility and continuous growth of their power conversion efficiencies.
Bulk heterojunction organic solar cells can be fabricated by simple processing
techniques, such as, screen printing, spin casting, etc., and, therefore, are potential
candidates for the mass production of flexible and cost-effective devices. In this
dissertation, based on the soluble macrocyclic organic semiconductors 5,10,15,20-
tetraphenyl-21H,23H-porphine zinc (ZnTPP) and copper (II) tetrakis (4-cumylphenoxy)
phthalocyanine
(Tc-CuPc)
bulk
heterjunction
structures
of
ITO/PEDOT:PSS/ZnTPP:PCBM/Al and ITO/PEDOT:PSS/Tc-CuPc:PCBM/Al were
fabricated employing spin casting and vacuum thermal evaporation techniques. The
effect of donor to acceptor (D:A) mass ratio was investigated on photovoltaic properties
of the ZnTPP:PCBM BHJ solar cell and the optimum D:A ratio was identified. Effect of
the thickness and surface morphology of the active layer on the photovoltaic properties of
this porphyrin-fullerne BHJ was also studied and the optimum active layer thickness was
identified. Bulk and hybrid-bilayer heterojunctions of copper (II) tetrakis (4-
cumylphenoxy)
phthalocyanine
(Tc-CuPc)
and
vanadyl
2,9,16,23-tetraphenoxy-
29H,31H-phthalocyanine (VOPcPhO) heterojunctions were also fabricated. Temperature
dependent electrical properties of these devices and optical performance of the Tc-
CuPc:PCBM bulk heterojunction was also investigated.
Macrocyclic semiconductors e.g. metallo-phthalocyanines (MPcs) and metallo-
porphyrins (MPPs), are restricted to dry processing techniques due to their insolubility in
common organic solvents. Thus MPcs and MPPs are used in typical thermally evaporated
donor-acceptor bi-layered solar cells. The performance of bi-layer solar cells is low due
to small exciton diffusion length; only the excitons generated within 10 nm from the D/A
interface are expected to contribute to photocurrent. This issue is resolved in BHJ
architecture, in which the D-A interfacial area is distributed throughout the volume (bulk)
viiiof the active layer. In other words the D-A interface is brought near to the exciton
generation site. Soluble versions of MPcs and MPPs can be helpful to study their opto-
electronic characteristics in BHJ solar cell architecture. In BHJ architecture there is a lot
of flexibility and ease for rapid research e.g. changing solvent, varying concentration,
using different D to A mass ratios, changing active layer thicknesses by spin coating at
different speeds, incorporating different exciton-blocking layers etc. A lot of variations
can be studied in a very short time and with less cost. However, as more and more
research groups start studying soluble macrocyclic organic semiconductors in BHJ solar
cells, further efficiency improvements and availability of new soluble macrocyclic
materials are worthwhile.
Since the microstructure of bulk heterojunction layer is strongly dependent on the donor
to acceptor (D:A) mass ratio, an optimum D:A ratio improves device performance by
improving the charge separation, transport and collection process. As one aspect of this
research
work,
porphyrin-fullerne
BHJ
solar
cells
with
ITO/PEDOT:PSS/ZnTPP:PCBM/Al structure were fabricated with different D:A mass
ratios and their optical parameters were measured both under simulated solar spectrum
AM 1.5G and monochromatic illuminations. The active layer thicknesses were extracted
from their respective optical reflection and transmission measurements using average
absorption coefficient. Scanning electron microscope (SEM) image of the device cross
section was studied to verify layer thicknesses and examine the quality of layers. Effect
of thermal annealing on performance of some devices was also studied. Incident photon-
to-current conversion efficiency (IPCE) spectra at different D:A ratios was determined.
On basis of the measured optical parameters such as fill factor FF, open circuit voltage
V OC , short circuit current density J SC , and power conversion efficiency η , the optimum
D:A ratio was identified. Maximum IPCE value of 21% was obtained for D:A ratio of 1:9
which lead to PCE of 0.21% which was 36 times better than a previously reported value
in which C 60 was used as acceptor. Also incorporating PCBM as the acceptor instead of
C 60 improved the open circuit voltage (V OC ) for all the D:A ratios. The reason for high
V OC is greater difference between the ZnTPP HOMO and PCBM LUMO . Furthermore the 1:9
devices showed consistency in optical parameters when reproduced.