Publications by Type: Journal Article

2014
Alex Dymshits, Amit Rotem, and Etgar Lioz. 10/2014. “High voltage in hole conductor free organo metalhalide perovskite solar cells.” J. Mater. Chem. A, 2014, 2, Pp. 20776. Abstract

Organo metal halide perovskite has attracted considerable attention recently due to its distinctive properties that make it especially useful in photovoltaic solar cells. In this work we demonstrate high open circuit voltage of 1.35 V using Al2O3/CH3NH3PbBr3 perovskite solar cells without a hole conductor. The contact potential difference under light measured by surface photovoltage spectroscopy of CH3NH3PbBr3 was more than twice that of CH3NH3PbI3, which results in smaller surface potential for the Al2O3/CH3NH3PbBr3 cells. Incident modulated photovoltage spectroscopy shows a longer recombination lifetime for the Al2O3/CH3NH3PbBr3 cells than for the TiO2/CH3NH3PbI3 cells or for the TiO2/CH3NH3PbBr3 cells, further supporting the high open circuit voltage. The possibility to gain high open circuit voltage even without a hole transport material in perovskite solar cells shows that the perovskite/metal oxide interface has a major effect on the open circuit voltage in perovskite based solar cells.

high_voltage_in_hole_conductor_free_organo_metal_halide_perovskite_solar_cells.pdf
Etgar Lioz, Peng Gao, Peng Qin, Michael Graetzel, and Mohammad Khaja Nazeeruddin. 6/2014. “A hybrid lead iodide perovskite and lead sulfide QD heterojunction solar cell to obtain a panchromatic response.” J. Mater. Chem. A, 2014, 2, Pp. 11586–11590. Abstract

We report for the first time on co-sensitization between CH3NH3PbI3 perovskite and PbS quantum dots (QDs) in a heterojunction solar cell to obtain a panchromatic response from the visible to near IR regions. Following the deposition of the sensitizers on a TiO2 film, an Au thin layer is evaporated on top as a back contact. Importantly, the CH3NH3PbI3 nanoparticles and the PbS QDs used here simultaneously play both the role of a light harvester and a hole conductor, rendering superfluous the use of an additional hole transporting material. The mesoscopic CH3NH3PbI3 (perovskite)–PbS (QD)/TiO2 heterojunction solar cell shows an impressive short circuit photocurrent (Jsc) of 24.63mA cm2, much higher than those of the individual CH3NH3PbI3 perovskite and the PbS QD solar cells. The advent of such co-sensitization mesoscopic heterojunction solar cells paves the way to extend the absorbance region of the promising low cost, high-efficiency perovskite based solar cells.

a_hybrid_lead_iodide_perovskite_and_lead_sulfide_qd_heterojunction_solar_cell_to_obtain_a_panchromatic_response.pdf
Shany Gamliel and Etgar Lioz. 6/2014. “Organo-metal perovskite based solar cells:sensitized versus planar architecture.” RSC Adv., 2014, 4, Pp. 29012-29021. Abstract

Organo-metal halide perovskites are composed of an ABX3 structure in which A represents a cation, B a divalent metal cation and X a halide. The organo-metal perovskite shows very good potential to be used as a light harvester in solar cells due to its direct band gap, large absorption coefficient, high carrier mobility and good stability. However, there is an important question in the photovoltaic field regarding the most advantageous architecture for perovskite based solar cells. Several studies showed sensitized perovskite solar cells achieving high performance, while high efficiency was also observed with the planar architecture. Consequently, it is still an open question regarding which operation mechanism and which architecture offers better results. This review describes both architectures, based on studies in the field. In the case of the sensitized structure, there are more difficulties in pore filling, naturally more recombination, and the possibility to use thicker metal oxide films. In the planar structure, thin metal oxide films are used, less recombination was observed and there are no infiltration problems. Both architectures exhibit long-range diffusion length and meet the demand for excellent coverage of the perovskite film.

organo-metal_perovskite_based_solar_cells.pdf
Sigalit Aharon, Bat El Cohen, and Etgar Lioz. 4/17/2014. “Hybrid Lead Halide Iodide and Lead Halide Bromide in Efficient HoleConductor Free Perovskite Solar Cell.” J. Phys. Chem. C, 2014, 118, Pp. 17160−17165. Abstract

In this work we used CH3NH3PbInBr3−n (where 0 ≤ n ≤ 3) as hole conductor and light harvester in the solar cell. Various concentrations of methylammonium iodide and methylammonium bromide were studied which reveal that any composition of the hybrid CH3NH3PbInBr3−n can conduct holes. The hybrid perovskite was deposited in two steps, separating it to two precursors to allow better control of the perovskite composition and efficient tuning of its band gap. The X-ray diffraction reveals the change in the lattice parameter due to the introducing of the Br− ions. The hybrid iodide/bromide perovskite hole conductor free solar cells show very good stability, their power conversion efficiency achieved 8.54% under 1 sun illumination with current density of 16.2 mA/cm2. The results of this work open the possibility for graded structure of perovskite solar cells without the need for hole conductor.

hybrid_lead_halide_iodide_and_lead_halide_bromide_in_efficient_hole_conductor_free_perovskite_solar_cell.pdf
Sigalit Aharon, Shany Gamliel, Bat El Cohen, and Etgar Lioz. 4/2014. “Depletion region effect of highly efficient holeconductor free CH3NH3PbI3 perovskite solar cells.” Phys.Chem.Chem.Phys., 2014, 16, Pp. 10512-10518. Abstract

The inorganic–organic perovskite is currently attracting a lot of attention due to its use as a light harvester in solar cells. The large absorption coefficients, high carrier mobility and good stability of organo-lead halide perovskites present good potential for their use as light harvesters in mesoscopic heterojunction solar cells. This work concentrated on a unique property of the lead halide perovskite, its function simultaneously as a light harvester and a hole conductor in the solar cell. A two-step deposition technique was used to optimize the perovskite deposition and to enhance the solar cell efficiency. It was revealed that the photovoltaic performance of the hole conductor free perovskite solar cell is strongly dependent on the depletion layer width which was created at the TiO2–CH3NH3PbI3 junction. X-ray diffraction measurements indicate that there were no changes in the crystallographic structure of the CH3NH3PbI3 perovskite over time, which supports the high stability of these hole conductor free perovskite solar cells. Furthermore, the power conversion efficiency of the best cells reached 10.85% with a fill factor of 68%, a Voc of 0.84 V, and a Jsc of 19 mA cm2, the highest efficiency to date of a hole conductor free perovskite solar cell.

depletion_region_effect_of_highly_efficient_hole_conductor_free_ch3nh3pbi3_perovskite_solar_cells.pdf
2013
Waleed Abu Laban and Etgar Lioz. 9/2013. “Depleted hole conductor-free lead halide iodideheterojunction solar cells.” Energy Environ. Sci., 2013, 6, Pp. 3249–3253. Abstract

Lead halide perovskite is an excellent candidate for use as a light harvester in solar cells. Our work presents a depleted hole conductor free CH3NH3PbI3/TiO2 heterojunction solar cell using a thick CH3NH3PbI3 film. The CH3NH3PbI3 formed large crystals which function
simultaneously as light harvesters and as hole transportmaterials. We performed capacitance voltage measurements, which show a depletion regionwhich extends to both n and p sides. The built-in field of the depletion region assists in the charge separation and suppresses the back reaction of electrons from the TiO2 film to the CH3NH3PbI3 film. This depleted hole conductor free CH3NH3PbI3/TiO2 heterojunction solar cell provides a power conversion efficiency of 8% with a current density of 18.8 mA cm2, the highest efficiency achieved to date for perovskite based solar cells without a hole conductor.

depleted_hole_conductor-free_lead_halide_iodide_heterojunction_solar_cells.pdf
Etgar Lioz, Guillaume Schuchardt, Daniele Costenaro, Fabio Carniato, Chiara Bisio, Shaik M. Zakeeruddin, Mohammad K. Nazeeruddin, Leonardo Marchese, and Michael Graetzel. 6/2013. “Enhancing the open circuit voltage of dye sensitizedsolar cells by surface engineering of silica particles in agel electrolyte.” J. Mater. Chem. A, 2013, 1, Pp. 10142–10147. Abstract

We prepared a quasi-solid electrolyte for dye-sensitized solar cells (DSSCs) that consist of ionic liquid and modified silica particles. Commercial bare silica F5 particles and modified silica F5 by NH2 and NH3groups were prepared, and fully characterized. The best photovoltaic performance was observed using the NH2 modified silica particles giving an open circuit voltage (Voc) of 815 mV, a short-circuit current (Jsc) of 11.23 mA cm-2, and a fill factor (FF) of 0.75 corresponding to an overall power conversion efficiency of 7.04% at 100 mW cm-2 AM 1.5. The modification of the silica particles by NH2 groups increases the Voc of DSSCs by around 60 mV compared to pure ionic liquid electrolyte based DSSCs.

enhancing_the_open_circuit_voltage_of_dye_sensitized_solar_cells_by_surface_engineering_of_silica_particles_in_a_gel_electrolyte.pdf
Etgar Lioz. 2/2013. “Semiconductor Nanocrystals as Light Harvesters in Solar Cells.” Materials, 2013, 6, Pp. 445-459. Abstract

Photovoltaic cells use semiconductors to convert sunlight into electrical current
and are regarded as a key technology for a sustainable energy supply. Quantum dot-based
solar cells have shown great potential as next generation, high performance, low-cost
photovoltaics due to the outstanding optoelectronic properties of quantum dots and their
multiple exciton generation (MEG) capability. This review focuses on QDs as light
harvesters in solar cells, including different structures of QD-based solar cells, such as QD
heterojunction solar cells, QD-Schottky solar cells, QD-sensitized solar cells and the recent
development in organic-inorganic perovskite heterojunction solar cells. Mechanisms,
procedures, advantages, disadvantages and the latest results obtained in the field are
described. To summarize, a future perspective is offered.

semiconductor_nanocrystals_as_light_harvesters_in_solar_cells.pdf
Etgar Lioz, Diana Yanover, Richard Karel Cˇapek, Roman Vaxenburg, Zhaosheng Xue, Bin Liu, Mohammad Khaja Nazeeruddin, Efrat Lifshitz, and Michael Grätzel. 1/2013. “Core/Shell PbSe/PbS QDs TiO2 Heterojunction Solar Cell.” Adv. Funct. Mater., 2013, 23, Pp. 2736–2741.
coreshell_pbsepbs_qds_tio2_heterojunction_solar_cell.pdf
Takafumi Fukumoto, Thomas Moehl, Yusuke Niwa, Md. K. Nazeeruddin, Michael Grätzel, and Etgar Lioz. 2013. “Effect of Interfacial Engineering in Solid-State Nanostructured Sb2S3 Heterojunction Solar Cells.” Adv. Energy Mater, 2013, 3, Pp. 29–33.
effect_of_interfacial_engineering_in_solid-state_nanostructured_sb2s3_heterojunction_solar_cells.pdf
2012
Etgar Lioz, Peng Gao, Zhaosheng Xue, Qin Peng, Aravind Kumar Chandiran, Bin Liu, Md. K. Nazeeruddin, and Michael Grätzel. 10/2012. “Mesoscopic CH3NH3PbI3/TiO2 Heterojunction Solar Cells.” J. Am. Chem. Soc., 2012, 134, Pp. 17396−17399.
mesoscopic_ch3nh3pbi3_tio2_heterojunction_solar_cells.pdf
Etgar Lioz, James S. Bendall, Vincent Laporte, Mark E. Welland, and Michael Graetzel. 9/2012. “Reducing recombination in ZnO photoanodes for dye sensitised solar cellsthrough simple chemical synthesis.” J. Mater. Chem., 2012, 22, Pp. 24463–24468.
reducing_recombination_in_zno_photoanodes_for_dye_sensitised_solar_cells_through_simple_chemical_synthesis.pdf
Etgar Lioz, Thomas Moehl, Stefanie Gabriel, Stephen G. Hickey, Alexander Eychmu¨ ller, and Michael Gra¨ tzel. 3/2012. “Light Energy Conversion by Mesoscopic PbS Quantum Dots/TiO2 Heterojunction Solar Cells.” ACS Nano, 2012, 4, Pp. 3092–3099.
light_energy_conversion_by_mesoscopic_pbs_quantum_dots_tio2_heterojunction_solar_cells.pdf
Etgar Lioz, Jinhyung Park, Claudia Barolo, Vladimir Lesnyak, Subhendu K. Panda, Pierluigi Quagliotto, Stephen G. Hickey, Md. K. Nazeeruddin, Alexander Eychmu¨ ller, Guido Viscardi, and Michael Gra¨ tzel. 2/2012. “Enhancing the efficiency of a dye sensitized solar cell due to the energytransfer between CdSe quantum dots and a designed squaraine dye.” RSC Adv., 2012, 2, Pp. 2748–2752.
enhancing_the_efficiency_of_a_dye_sensitized_solar_cell_due_to_the_energy_transfer_between_cdse_quantum_dots_and_a_designed_squaraine_dye.pdf
Etgar Lioz, Wei Zhang, Stefanie Gabriel, Stephen G. Hickey, Md K. Nazeeruddin, Alexander Eychmüller, Bin Liu, and Michael Grätzel. 1/2012. “High Efficiency Quantum Dot Heterojunction Solar CellUsing Anatase (001) TiO2 Nanosheets.” Adv. Mater., 2012, 24, Pp. 2202–2206.
high_efficiency_quantum_dot_heterojunction_solar_cell_using_anatase_001_tio2_nanosheets.pdf
Etgar Lioz and Michael Grätzel. 2012. “Solid state PbS Quantum dots /TiO2 Nanoparticles heterojunction solar cell.” MRS Proceedings, 2012, 1390.
2011
Etgar Lioz, Jinhyung Park, Claudia Barolo, Md. K. Nazeeruddin, Guido Viscardi, and Michael Graetzel. 8/2011. “Design and Development of Novel Linker for PbS Quantum Dots/TiO2 Mesoscopic Solar cell.” ACS Appl. Mater. Interfaces, 2011, 3, Pp. 3264–3267.
design_and_development_of_novel_linker_for_pbs_quantum_dots_tio2_mesoscopic_solar_cell.pdf
D. Aaron R. Barkhouse, Ratan Debnath, Illan J. Kramer, David Zhitomirsky, Andras G. Pattantyus-Abraham, Larissa Levina, Etgar Lioz, Michael Grätzel, and Edward H. Sargent. 5/2011. “Depleted Bulk Heterojunction Colloidal Quantum Dot Photovoltaics.” Adv. Mater., 2011, 23, Pp. 3134–3138.
depleted_bulk_heterojunction_colloidal_quantum_dot_photovoltaics.pdf
James S. Bendall, Etgar Lioz, Swee Ching Tan, Ning Cai, Peng Wang, Shaik M. Zakeeruddin, Michael Grätzel, and Mark E. Welland. 5/2011. “An efficient DSSC based on ZnO nanowire photo-anodes and a new D-p-Aorganic dye.” Energy Environ. Sci., 2011, 4, Pp. 2903–2908.
an_efficient_dssc_based_on_zno_nanowire_photo-anodes_and_a_new_d-p-a_organic_dye.pdf
Aravind Kumar Chandiran, Frederic Sauvage, Etgar Lioz, and Michael Grätzel. 4/2011. “Ga3+ and Y3+ Cationic Substitution in Mesoporous TiO2 Photoanodesfor Photovoltaic Applications.” J. Phys. Chem. C, 2011, 115, Pp. 9232–9240.
ga3_and_y3_cationic_substitution_in_mesoporous_tio2_photoanodes_for_photovoltaic_applications.pdf

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