about
Low-temperature processed electron collection layers of graphene/TiO2 nanocomposites in thin film perovskite solar cells.Effects of the Gaussian energy dispersion on the statistics of polarons and bipolarons in conducting polymers.Physical electrochemistry of nanostructured devices.Characterization of nanostructured hybrid and organic solar cells by impedance spectroscopy.Device modeling of dye-sensitized solar cells.High reduction of interfacial charge recombination in colloidal quantum dot solar cells by metal oxide surface passivation.Classification of solar cells according to mechanisms of charge separation and charge collection.Controlled carbon nitride growth on surfaces for hydrogen evolution electrodes.Nano-Enabled Photovoltaics. Progress in Materials and Methodologies.Elucidating Operating Modes of Bulk-Heterojunction Solar Cells from Impedance Spectroscopy Analysis.Effect of Organic and Inorganic Passivation in Quantum-Dot-Sensitized Solar Cells.Interpretation of Cyclic Voltammetry Measurements of Thin Semiconductor Films for Solar Fuel Applications.Factors determining the photovoltaic performance of a CdSe quantum dot sensitized solar cell: the role of the linker molecule and of the counter electrode.Bandgap modulation in efficient n-thiophene absorbers for dye solar cell sensitization.Solution-processed small molecule:fullerene bulk-heterojunction solar cells: impedance spectroscopy deduced bulk and interfacial limits to fill-factors.Impact of Capacitive Effect and Ion Migration on the Hysteretic Behavior of Perovskite Solar Cells.Mechanism of carrier accumulation in perovskite thin-absorber solar cells.Core/shell colloidal quantum dot exciplex states for the development of highly efficient quantum-dot-sensitized solar cells.The JPCL New Year's Editorial.Investigating the Consistency of Models for Water Splitting Systems by Light and Voltage Modulated Techniques.Relaxation of photogenerated carriers in P3HT:PCBM organic blends.Interfacial Degradation of Planar Lead Halide Perovskite Solar Cells.Selective contacts drive charge extraction in quantum dot solids via asymmetry in carrier transfer kinetics.Understanding the synergistic effect of WO3-BiVO4 heterostructures by impedance spectroscopy.Interpretation of electron diffusion coefficient in organic and inorganic semiconductors with broad distributions of states.Inductive Loop in the Impedance Response of Perovskite Solar Cells Explained by Surface Polarization Model.Imidazolium Iodide-Doped PEDOT Nanofibers as Conductive Catalysts for Highly Efficient Solid-State Dye-Sensitized Solar Cells Employing Polymer Electrolyte.Triumphing over Charge Transfer Limitations of PEDOT Nanofiber Reduction Catalyst by 1,2-Ethanedithiol Doping for Quantum Dot Solar Cells.Surface Recombination and Collection Efficiency in Perovskite Solar Cells from Impedance Analysis.Theory of Light-Modulated Emission Spectroscopy.Surface Polarization Model for the Dynamic Hysteresis of Perovskite Solar Cells.Cooperative Catalytic Effect of ZrO2 and α-Fe2 O3 Nanoparticles on BiVO4 Photoanodes for Enhanced Photoelectrochemical Water Splitting.High-efficiency "green" quantum dot solar cells.Triplication of the photocurrent in dye solar cells by increasing the elongation of the π-conjugation in Zn-porphyrin sensitizers.Characteristics of high efficiency dye-sensitized solar cells.Implications of the negative capacitance observed at forward bias in nanocomposite and polycrystalline solar cells.Carbon Counter-Electrode-Based Quantum-Dot-Sensitized Solar Cells with Certified Efficiency Exceeding 11.Control of I-V hysteresis in CH3NH3PbI3 perovskite solar cell.Photoinduced Giant Dielectric Constant in Lead Halide Perovskite Solar Cells.Slow Dynamic Processes in Lead Halide Perovskite Solar Cells. Characteristic Times and Hysteresis.
P50
Q34392139-33BC9E93-ED19-4B3D-9E0A-944AB0CD824BQ35842460-9D40E845-1827-49EA-A464-2BF4EF5362A0Q37030607-873969D1-E527-4AF5-8219-8E3A5F82BB2DQ37862101-2A527790-8E55-42F8-BBC7-F49136487889Q38148487-B6DAAA11-C2AC-49E9-AB1D-B1C5244EC829Q38445114-C6B9D921-D003-475B-BAED-1A0EA5A7F27EQ39059215-F27D2AAF-FF26-4324-ACCD-956CBAE72099Q39244099-DCC05755-AEC4-4994-935F-6EB7D7A721F8Q40624107-008EF6E5-9E1D-4325-A64C-AF1AFCAE0B76Q40624261-D5651F8E-F829-41FA-B2A1-6ED67D6CD1B4Q40633831-E0A14D43-E904-4F4A-89A4-89654BA1F735Q40634145-1B648369-C75A-4C93-9A89-D371D7E1299CQ42727769-42903A44-7A56-4548-91B0-E414E4639839Q43235875-7AA58BC2-A541-4C1D-AD34-59D15024DC3AQ44803049-931BA162-427F-4E27-B672-83FD6BAF578FQ45021897-3E8AED64-2D5A-4F63-A6C1-877CCA52AE70Q45195383-F2E530A8-BFC9-48D3-9076-F22D062979D5Q45345560-94651398-BE6F-48C3-80CF-7B8159BCD04AQ45939710-9DCCB7B4-1501-45DD-A9A0-45913D14D891Q45987696-9DE74F84-8D07-4B74-90DE-A339CD4BE94AQ46060565-B8500E8B-57EF-4D9C-83E0-7E4A8435826BQ46087379-A55B304F-B944-4F44-99D9-5F196B463CCFQ46177560-959EF259-0D84-4360-A7B5-0591A56BD328Q46763673-843F898A-DE18-4C2D-9AF5-E9E7D70B3FCBQ47686185-7FD04DC9-4C9E-4CFB-8285-5CA583CB2A92Q47932447-7E40655E-9396-4692-BE70-2596F917210CQ48045370-AF496ABD-849E-4D89-9F9D-963DA4EEC230Q48051212-BF84CBF2-D2D6-46D7-BB90-A569E9DB9D2AQ48052044-4B981E80-1DAC-4351-8FC9-AC5651097C36Q48088072-70665753-721B-4447-8C02-173BFABE1F41Q48266442-21D99C80-D2AA-4FDB-AFCB-711EAE24DD34Q48374133-290D1E32-4695-4E89-A613-45D50D856575Q50455577-70A93A66-D26C-41FA-8986-980EE39AFEB8Q50543497-2A0F86E9-0001-4972-AC19-D43347B49781Q51094270-A0218880-6FE0-47D2-88F4-7B356B120FAAQ51227996-EEE88F8B-F4A8-44CD-BE77-75DE081267B1Q51233202-9CF542FF-DC87-47DD-B4C5-E78DE6B9D3D8Q51652524-E62FC9B3-C804-480C-8311-EE4F34FA214DQ51806563-A17970B1-58C6-4D95-8442-A9D40CD46B8EQ51806579-C795822E-858E-4F76-9D01-8E0EDED49EB2
P50
description
hulumtues
@sq
researcher
@en
taighdeoir
@ga
wetenschapper
@nl
հետազոտող
@hy
name
Juan Bisquert
@ast
Juan Bisquert
@en
Juan Bisquert
@es
Juan Bisquert
@nl
Juan Bisquert
@sl
type
label
Juan Bisquert
@ast
Juan Bisquert
@en
Juan Bisquert
@es
Juan Bisquert
@nl
Juan Bisquert
@sl
prefLabel
Juan Bisquert
@ast
Juan Bisquert
@en
Juan Bisquert
@es
Juan Bisquert
@nl
Juan Bisquert
@sl
P1053
O-2543-2013
P106
P19
P21
P31
P3829
P496
0000-0003-4987-4887
P569
1962-01-01T00:00:00Z