5 research outputs found
Revealing the Role of Potassium Treatment in CZTSSe Thin Film Solar Cells
Potassium
(K) post-treatment on CIGSSe has been shown to yield
the highest efficiency reported to date. However, very little is known
on the effect of K doping in CZTSSe and the mechanism behind the efficiency
improvement. Here we reveal the mechanism by which K enhances the
charge separation in CZTSSe. We show that K accumulates at the CdS/CZTSSe,
passivating the recombination at the front interface and improving
carrier collection. K is also found to accumulate at the CZTSSe/Mo
interface and facilitates the diffusion of Cd into the absorber which
affects the morphology and grain growth of CZTSSe. As revealed by
the <i>C</i>–<i>V</i>, external quantum
efficiency, and color <i>J</i>–<i>V</i> test, K doping significantly increases the carrier density, improves
carrier collection, and passivates the front interface and grain boundaries,
leading to the enhancement of <i>V</i><sub>oc</sub> and <i>J</i><sub>sc</sub>. The average power conversion efficiency
has been promoted from 5% to above 7%, and the best 7.78% efficiency
has been achieved for the 1.5 mol % K-doped CZTSSe device. This work
offers some new insights into the K doping effects on CZTSSe via solution-based
approach and demonstrates the potential of facile control of K doping
for further improvement of CZTSSe thin film solar cells
Solution-Processed Trigonal Cu<sub>2</sub>BaSnS<sub>4</sub> Thin-Film Solar Cells
Recently,
Cu<sub>2</sub>BaSnS<sub>4</sub> (CBTS) thin film has emerged as a
promising candidate for single- or multiple-junction photovoltaics
(PVs) due to its excellent optical and electrical properties, and
earth-abundant, nontoxic constituents. In this study, a molecular
solution-based nonvacuum process has been employed to prepare CBTS
thin films for solar cells. The obtained CBTS films show trigonal
structure with band gap of 2.01 eV and p-type conductivity. The solar
cell device with configuration of Mo-coated glass/CBTS/CdS/i-ZnO/ITO
has achieved a power conversion efficiency (PCE) of 1.72% for CBTS
with a Ba/Sn atomic ratio of 1.30. An abrupt band gap cutoff in external
quantum efficiency (EQE) data coupled with the very small offset (only
10 meV) in band gap between EQE and photoluminescence (PL) measurements
reveals that band tailing is not the limiting factor in CBTS
Kesterite Cu<sub>2</sub>ZnSn(S,Se)<sub>4</sub> Solar Cells with beyond 8% Efficiency by a Sol–Gel and Selenization Process
A facile
sol–gel and selenization process has been demonstrated
to fabricate high-quality single-phase earth abundant kesterite Cu<sub>2</sub>ZnSnÂ(S,Se)<sub>4</sub> (CZTSSe) photovoltaic absorbers. The
structure and band gap of the fabricated CZTSSe can be readily tuned
by varying the [S]/([S] + [Se]) ratios via selenization condition
control. The effects of [S]/([S] + [Se]) ratio on device performance
have been presented. The best device shows 8.25% total area efficiency
without antireflection coating. Low fill factor is the main limitation
for the current device efficiency compared to record efficiency device
due to high series resistance and interface recombination. By improving
film uniformity, eliminating voids, and reducing the MoÂ(S,Se)<sub>2</sub> interfacial layer, a further boost of the device efficiency
is expected, enabling the proposed process for fabricating one of
the most promising candidates for kesterite solar cells
Enhancement of Open-Circuit Voltage of Solution-Processed Cu<sub>2</sub>ZnSnS<sub>4</sub> Solar Cells with 7.2% Efficiency by Incorporation of Silver
Recently,
considerable attention in the development of Cu<sub>2</sub>ZnSnS<sub>4</sub> (CZTS)-based thin-film solar cells has been given
to the reduction of antisite defects via cation substitution. In this
Letter, we report the substitution of copper atoms by silver, incorporated
into the crystal lattice through a solution processable method. We
observe an increase in open-circuit voltage (<i>V</i><sub>OC</sub>) by 50 mV and an accompanying rise in device efficiency
from 4.9% to 7.2%. The incorporation of Ag is found to improve the
grain size, enhance the depletion width of the pn-junction, and reduce
the concentration of antisite defect states. This work demonstrates
the promising role of Ag in
reducing the <i>V</i><sub>OC</sub> deficit of Cu-kesterite
thin-film solar cells
Origin of Photocarrier Losses in Iron Pyrite (FeS<sub>2</sub>) Nanocubes
Iron pyrite has received significant
attention due to its high
optical absorption. However, the loss of open circuit voltage (<i>V</i><sub>oc</sub>) prevents its further application in photovoltaics.
Herein, we have studied the photophysics of pyrite by ultrafast laser
spectroscopy to understand fundamental limitation of low <i>V</i><sub>oc</sub> by quantifying photocarrier losses in high quality,
stoichiometric, and phase pure {100} faceted pyrite nanocubes. We
found that fast carrier localization of photoexcited carriers to indirect
band edge and shallow trap states is responsible for major carrier
loss. Slow relaxation component reflects high density of defects within
the band gap which is consistent with the observed Mott-variable range
hopping (VRH) conduction from transport measurements. Magnetic measurements
strikingly show the magnetic ordering associated with phase inhomogeneity,
such as FeS<sub>2−δ</sub> (0 ≤ δ ≤
1). This implies that improvement of iron pyrite solar cell performance
lies in mitigating the intrinsic defects (such as sulfur vacancies)
by blocking the fast carrier localization process. Photocarrier generation
and relaxation model is presented by comprehensive analysis. Our results
provide insight into possible defects that induce midgap states and
facilitate rapid carrier relaxation before collection