Ion‐Charged Dielectric Nanolayers for Enhanced Surface Passivation in High Efficiency Photovoltaic Devices

The power conversion efficiency of solar cells is strongly impacted by an unwanted loss of charge carriers occurring at semiconductor surfaces and interfaces. Here the use of ion‐charged oxide nanolayers to enhance the passivation of silicon surfaces via the field effect mechanism is reported. The first report of enhanced passivation from rubidium and cesium ion‐charged oxide nanolayers is provided. The charge state and formation energy of ion‐charged silicon dioxide are calculated from first principles. Ion embedding is demonstrated and exploited to control the interface population of carriers and minimize electron‐hole pair recombination. The passivation quality directly improves with charge concentration, yet excess ions can produce detrimental interface states. An optimal ionic charge concentration of ≈1.5 × 1012 q cm−2 is deduced, and a recombination velocity and current density as low as 2.8 cm s−1 and 7.8 fA cm−2 are achieved at the Si‐SiO2 interface. Maximized charge is shown to provide efficiency improvements as high as 0.7% absolute. This work provides a unique route to enhance passivation without compromising the film synthesis, thus retaining the antireflection and hydrogenation film properties. As such, ion‐charged dielectrics provide complementary paths for surface and interface optimization in future single‐junction and tandem solar cells.

[1]  R. S. Bonilla Modelling of Kelvin probe surface voltage and photovoltage in dielectric-semiconductor interfaces , 2022, Materials Research Express.

[2]  B. Rech,et al.  Field Effect Passivation in Perovskite Solar Cells by a LiF Interlayer , 2022, Advanced Energy Materials.

[3]  Katherine A. Collett,et al.  Electrostatic Tuning of Ionic Charge in SiO2 Dielectric Thin Films , 2022, ECS Journal of Solid State Science and Technology.

[4]  M. Schubert,et al.  Reassessment of the intrinsic bulk recombination in crystalline silicon , 2022, Solar Energy Materials and Solar Cells.

[5]  A. Masuda,et al.  Potential‐induced degradation in high‐efficiency n‐type crystalline‐silicon photovoltaic modules: A literature review , 2021, Solar RRL.

[6]  Mingzhe Yu,et al.  Extracting band-tail interface state densities from measurements and modelling of space charge layer resistance , 2021 .

[7]  Stylianos P. Syrigos,et al.  Behavioral Analysis of Potential Induced Degradation on Photovoltaic Cells, Regeneration and Artificial Creation , 2021, Energies.

[8]  Mingzhe Yu,et al.  Assessing the Potential of Inversion Layer Solar Cells Based on Highly Charged Dielectric Nanolayers , 2021, physica status solidi (RRL) – Rapid Research Letters.

[9]  S. Glunz,et al.  Design rules for high-efficiency both-sides-contacted silicon solar cells with balanced charge carrier transport and recombination losses , 2021, Nature Energy.

[10]  Hee‐eun Song,et al.  Analysis of the negative charges injected into a SiO2/SiNx stack using plasma charging technology for field‐effect passivation on a boron‐doped silicon surface , 2020, Progress in Photovoltaics: Research and Applications.

[11]  Mingzhe Yu,et al.  Charge fluctuations at the Si–SiO2 interface and its effect on surface recombination in solar cells , 2020, Solar Energy Materials and Solar Cells.

[12]  A. Masuda,et al.  Effect of a silicon nitride film on the potential-induced degradation of n-type front-emitter crystalline silicon photovoltaic modules , 2020, Japanese Journal of Applied Physics.

[13]  Zu-Po Yang,et al.  Hydrogenation behaviors in passivated emitter and rear silicon solar cells with variously hydrogenated SiNx films , 2020 .

[14]  W. D. Ceuninck,et al.  Physics of potential-induced degradation in bifacial p-PERC solar cells , 2019, Solar Energy Materials and Solar Cells.

[15]  R. Brendel,et al.  Surface passivation of crystalline silicon solar cells: Present and future , 2018, Solar Energy Materials and Solar Cells.

[16]  A. Cuevas,et al.  Carrier population control and surface passivation in solar cells , 2018, Solar Energy Materials and Solar Cells.

[17]  P. Altermatt,et al.  Effect of carrier-induced hydrogenation on the passivation of the poly-Si/SiOx/c-Si interface , 2018 .

[18]  R. S. Bonilla,et al.  Potassium ions in SiO2: electrets for silicon surface passivation , 2018 .

[19]  Katherine A. Collett,et al.  An enhanced alneal process to produce SRV < 1 cm/s in 1 Ω cm n-type Si , 2017 .

[20]  M. Hermle,et al.  Long term stability of c-Si surface passivation using corona charged SiO 2 , 2017 .

[21]  P. Hamer,et al.  Dielectric surface passivation for silicon solar cells: A review , 2017 .

[22]  R. S. Bonilla,et al.  On the c-Si/SiO2 interface recombination parameters from photo-conductance decay measurements , 2017 .

[23]  P. Hamer,et al.  A novel source of atomic hydrogen for passivation of defects in silicon , 2017 .

[24]  Katherine A. Collett,et al.  Corona Charge in SiO2: Kinetics and Surface Passivation for High Efficiency Silicon Solar Cells☆ , 2016 .

[25]  Manabu Ataka,et al.  Charging mechanism of electret film made of potassium-ion-doped SiO2 , 2016 .

[26]  Z. Hameiri,et al.  The impact of surface damage region and edge recombination on the effective lifetime of silicon wafers at low illumination conditions , 2015 .

[27]  A. D. Corso Pseudopotentials periodic table: From H to Pu , 2014 .

[28]  R. S. Bonilla,et al.  Very low surface recombination velocity in n-type c-Si using extrinsic field effect passivation , 2014 .

[29]  R. S. Bonilla,et al.  A technique for field effect surface passivation for silicon solar cells , 2014 .

[30]  Andres Cuevas,et al.  Effect of boron concentration on recombination at the p-Si–Al2O3 interface , 2014 .

[31]  G. Kovačević,et al.  Structure, defects, and strain in silicon-silicon oxide interfaces , 2014 .

[32]  G. Dingemans,et al.  Plasma-enhanced Chemical Vapor Deposition of Aluminum Oxide Using Ultrashort Precursor Injection Pulses , 2012 .

[33]  Wmm Erwin Kessels,et al.  Silicon surface passivation by ultrathin Al2O3 films synthesized by thermal and plasma atomic layer deposition , 2010 .

[34]  Ulrich Mescheder,et al.  Properties of SiO2 electret films charged by ion implantation for MEMS-based energy harvesting systems , 2009 .

[35]  Stefano de Gironcoli,et al.  QUANTUM ESPRESSO: a modular and open-source software project for quantum simulations of materials , 2009, Journal of physics. Condensed matter : an Institute of Physics journal.

[36]  Andre Stesmans,et al.  Degradation of the thermal oxide of the Si/SiO2/Al system due to vacuum ultraviolet irradiation , 1995 .

[37]  R. Hezel,et al.  Studies on evaporated cesium incorporation in MIS inversion layer solar cells , 1994 .

[38]  R. Hezel UV radiation hardness of silicon inversion layer solar cells , 1990, IEEE Conference on Photovoltaic Specialists.

[39]  J. Snel The doped Si/SiO2 interface , 1981 .

[40]  C. Sah,et al.  Determination of the MOS oxide capacitance , 1975 .

[41]  L. Terman An investigation of surface states at a silicon/silicon oxide interface employing metal-oxide-silicon diodes , 1962 .

[42]  O. Anderson,et al.  Calculation of Activation Energy of Ionic Conductivity in Silica Glasses by Classical Methods , 1954 .

[43]  S. Steingrube,et al.  Advances in the Surface Passivation of Silicon Solar Cells , 2012 .

[44]  Armin G. Aberle,et al.  Crystalline silicon solar cells : advanced surface passivation and analysis , 1999 .