5 research outputs found
Ultralow Absorption Coefficient and Temperature Dependence of Radiative Recombination of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Perovskite from Photoluminescence
Spectrally resolved photoluminescence
is used to measure the band-to-band
absorption coefficient α<sub>BB</sub>(ℏω) of organic–inorganic
hybrid perovskite methylammonium lead iodide (CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>) films from 675 to 1400 nm. Unlike other methods
used to extract the absorption coefficient, photoluminescence is only
affected by band-to-band absorption and is capable of detecting absorption
events at very low energy levels. Absorption coefficients as low as
10<sup>–14</sup> cm<sup>–1</sup> are detected at room
temperature for long wavelengths, which is 14 orders of magnitude
lower than reported values at shorter wavelengths. The temperature
dependence of α<sub>BB</sub>(ℏω) is calculated
from the photoluminescence spectra of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> in the temperature range 80–360 K. Based on
the temperature-dependent α<sub>BB</sub>(ℏω), the
product of the radiative recombination coefficient and square of the
intrinsic carrier density, <i>B</i>(<i>T</i>)
Ă— <i>n</i><sub><i>i</i></sub><sup>2</sup>, is also obtained
Inverted Hysteresis in CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Solar Cells: Role of Stoichiometry and Band Alignment
J–V
hysteresis in perovskite solar cells is known to be
strongly dependent on many factors ranging from the cell structure
to the preparation methods. Here we uncover one likely reason for
such sensitivity by linking the stoichiometry in pure CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> (MAPbI<sub>3</sub>) perovskite cells
with the character of their hysteresis behavior through the influence
of internal band offsets. We present evidence indicating that in some
cells the ion accumulation occurring at large forward biases causes
a temporary and localized increase in recombination at the MAPbI<sub>3</sub>/TiO<sub>2</sub> interface, leading to inverted hysteresis
at fast scan rates. Numerical semiconductor models including ion accumulation
are used to propose and analyze two possible origins for these localized
recombination losses: one based on band bending and the other on an
accumulation of ionic charge in the perovskite bulk
Supplement 1: Total absorption of visible light in ultrathin weakly absorbing semiconductor gratings
Supplemental document Originally published in Optica on 20 June 2016 (optica-3-6-556
Light and Electrically Induced Phase Segregation and Its Impact on the Stability of Quadruple Cation High Bandgap Perovskite Solar Cells
Perovskite
material with a bandgap of 1.7–1.8 eV is highly desirable for
the top cell in a tandem configuration with a lower bandgap bottom
cell, such as a silicon cell. This can be achieved by alloying iodide
and bromide anions, but light-induced phase-segregation phenomena
are often observed in perovskite films of this kind, with implications
for solar cell efficiency. Here, we investigate light-induced phase
segregation inside quadruple-cation perovskite material in a complete
cell structure and find that the magnitude of this phenomenon is dependent
on the operating condition of the solar cell. Under short-circuit
and even maximum power point conditions, phase segregation is found
to be negligible compared to the magnitude of segregation under open-circuit
conditions. In accordance with the finding, perovskite cells based
on quadruple-cation perovskite with 1.73 eV bandgap retain 94% of
the original efficiency after 12 h operation at the maximum power
point, while the cell only retains 82% of the original efficiency
after 12 h operation at the open-circuit condition. This result highlights
the need to have standard methods including light/dark and bias condition
for testing the stability of perovskite solar cells. Additionally,
phase segregation is observed when the cell was forward biased at
1.2 V in the dark, which indicates that photoexcitation is not required
to induce phase segregation