5 research outputs found
The Transitional Heterojunction Behavior of PbS/ZnO Colloidal Quantum Dot Solar Cells
The nature of charge separation at the heterojunction
interface
of solution processed lead sulphide-zinc oxide colloidal quantum dot
solar cells is investigated using impedance spectroscopy and external
quantum efficiency measurements to examine the effect of varying the
zinc oxide doping density. Without doping, the device behaves excitonically
with no depletion region in the PbS layer such that only charge carriers
generated within a diffusion length of the PbS/ZnO interface have
a good probability of being harvested. After the ZnO is photodoped
such that the doping density is near or greater than that of the PbS,
a significant portion of the depletion region is found to lie within
the PbS layer increasing charge extraction (pān operation)
Transfer Printed Silver Nanowire Transparent Conductors for PbSāZnO Heterojunction Quantum Dot Solar Cells
Transfer-printed
silver nanowire transparent conducting electrodes are demonstrated
in lead sulfideāzinc oxide quantum dot solar cells. Advantages
of using this transparent conductor technology are increased junction
surface energy, solution processing, and the potential cost reduction
of low temperature processing. Joule heating, device aging, and film
thickness effects are investigated to understand shunt pathways created
by nanowires protruding perpendicular to the film. A <i>V</i><sub>oc</sub> of 0.39 Ā± 0.07 V, <i>J</i><sub>sc</sub> of 16.2 Ā± 0.2 mA/cm<sup>2</sup>, and power conversion efficiencies
of 2.8 Ā± 0.4% are presented
Narrow Band Gap Lead Sulfide Hole Transport Layers for Quantum Dot Photovoltaics
The band structure
of colloidal quantum dot (CQD) bilayer heterojunction solar cells
is optimized using a combination of ligand modification and QD band
gap control. Solar cells with power conversion efficiencies of up
to 9.33 Ā± 0.50% are demonstrated by aligning the absorber and
hole transport layers (HTL). Key to achieving high efficiencies is
optimizing the relative position of both the valence band and Fermi
energy at the CQD bilayer interface. By comparing different band gap
CQDs with different ligands, we find that a smaller band gap CQD HTL
in combination with a more p-type-inducing CQD ligand is found to
enhance hole extraction and hence device performance. We postulate
that the efficiency improvements observed are largely due to the synergistic
effects of narrower band gap QDs, causing an upshift of valence band
position due to 1,2-ethaneĀdithiol (EDT) ligands and a lowering
of the Fermi level due to oxidation
Poly(3-hexylthiophene-2,5-diyl) as a Hole Transport Layer for Colloidal Quantum Dot Solar Cells
Lead sulfide colloidal quantum dot
(CQD) solar cells demonstrate extremely high short-circuit currents
(<i>J</i><sub>sc</sub>) and are making decent progress in
power conversion efficiencies. However, the low fill factors (FF)
and open-circuit voltages have to be addressed with urgency to prevent
the stalling of efficiency improvements. This paper highlights the
importance of improving hole extraction, which received much less
attention as compared to the electron-accepting component of the device
architecture (e.g., TiO<sub>2</sub> or ZnO). Here, we show the use
of semiconducting polymer polyĀ(3-hexylthiophene-2,5-diyl) to create
efficient CQD devices by improving hole transport, removing interfacial
barriers, and minimizing shunt pathways, thus resulting in an overall
improvement in device performance stemming from better <i>J</i><sub>sc</sub> and FF
Influence of Shell Thickness and Surface Passivation on PbS/CdS Core/Shell Colloidal Quantum Dot Solar Cells
Cation-exchange
has been used to synthesize PbS/CdS core/shell
colloidal quantum dots from PbS starting cores. These were then incorporated
as the active material in solar cell test devices using a solution-based,
air-ambient, layer-by-layer spin coating process. We show that core/shell
colloidal quantum dots can replace their unshelled counterparts with
a similar band gap as the active layer in a solar cell device, leading
to an improvement in open circuit voltage from 0.42 to 0.66 V. This
improvement is attributed to a reduction in recombination as a result
of the passivating shell. However, this increase comes at the expense
of short circuit current by creating a barrier for transport. To overcome
this, we first optimize the shell thickness by varying the conditions
for cation-exchange to form the thinnest shell layer possible that
provides sufficient surface passivation. Next, ligand exchange with
a combination of halide and bifunctional organic molecules is used
in conjunction with the core/shell strategy. Power conversion efficiencies
of 5.6 Ā± 0.4% have been achieved with a simple heterojunction
device architecture