MRS Meetings and Events

 

EN02.08.04 2023 MRS Spring Meeting

Opto-Electrical Characterization of Back Bandgap-Graded Cu2Zn(Sn1-x,Gex)Se4 Kesterite Thin-Film Solar Cells

When and Where

Apr 12, 2023
4:45pm - 5:00pm

Moscone West, Level 2, Room 2002

Presenter

Co-Author(s)

Romain Scaffidi1,2,3,Guy Brammertz3,1,Jessica de Wild3,1,Denis Flandre2,Bart Vermang3,1

Hasselt University1,UCLouvain2,imec3

Abstract

Romain Scaffidi1,2,3,Guy Brammertz3,1,Jessica de Wild3,1,Denis Flandre2,Bart Vermang3,1

Hasselt University1,UCLouvain2,imec3
CZTSSe kesterite materials constitute a promising candidate for thin-film photovoltaics, based on abundant and non-toxic elements. Despite their high absorption coefficient and tunable bandgap for either single or tandem junctions, they suffer from significant V<sub>oc</sub> losses impeding their efficiency to level with competing technologies such as CIGS, CdTe and Perovskites. Two main culprits for this large V<sub>oc</sub> deficit are electrostatic fluctuations and high density of bulk defects, highly dependent on the absorber composition typically considered as ideal within well-established Cu-poor and Zn-rich ranges. An increasingly popular solution to tackle these two loss mechanisms and boost V<sub>oc</sub> is the alloying of Ge to substitute Sn, leading here to Cu<sub>2</sub>Zn(Sn<sub>1-x</sub>,Ge<sub>x</sub>)Se<sub>4</sub> (CZTGSe) compounds, the bandgap of which is tunable through conduction band level following the x=Ge/Ge+Sn ratio. This work focuses precisely on the opto-electrical characterization of Sn-Ge bandgap-graded CZTGSe solar cells at both the absorber and complete device levels.<br/><br/>A sequential process is implemented and optimized, involving first the physical evaporation of a CZTG metallic precursor stack, then pre-annealed in N<sub>2</sub> and finally selenized. We obtain CZTGSe absorbers with low surface roughness and acceptable grain size within a Cu-poor and Zn-rich composition range. They exhibit an average x ratio around 45%, with a clear Sn-Ge segregation appearing naturally during the annealing step that leads to x=70% at the back surface and x=20% at the front surface. This corresponds to a back bandgap gradient which should simultaneously improve carrier collection and limit interface recombination, similarly to state-of-the-art CIGS. Yet, the low carrier lifetime is likely limited by poor top surface quality with observed surface defects and ZnSe secondary phases.<br/><br/>Advanced electrical characterization is performed on complete CZTGSe solar cell samples to gauge the impact of this Sn-Ge back bandgap grading approach and detect potential loss mechanisms. An efficiency of 7.2% is attained, along with values of 484 mV, 34.5 mA/cm<sup>2</sup> and 43.3 % for V<sub>oc</sub>, J<sub>sc</sub> and FF, respectively. Even though the performance is lower than record kesterite devices, the J<sub>sc</sub> value is close to the Shockley-Queisser (SQ) limit for a confirmed minimum bandgap of 1.18eV, probably due to the largely enhanced carrier collection by our back bandgap gradient design. However, our devices are affected by important V<sub>oc</sub> and FF deficits, i.e. about 50% of their SQ limits, for which the analysis of dark and light IV curves suggest are mainly the consequence of high-density deep defects as well as dominant electrical parasitics. This is investigated more deeply via temperature-dependent admittance spectroscopy, enabling the identification of a relatively deep defect level at the CZTGSe/CdS interface with activation energy of 260 meV and capture cross section of the order of 10<sup>-16</sup> cm<sup>-2</sup>. Minority carrier recombination via this defect state is likely the explanation for the poor V<sub>oc</sub> and FF values observed. SCAPS-1D simulations are well in agreement with these experimental findings and allow to highlight this interface loss mechanism as the main limiting factor in our samples.<br/><br/>Eventually, Ge inclusion into kesterites effectively permits bandgap gradient to boost carrier collection and approach SQ limits in terms of J<sub>sc</sub>. However, our study reveals that performance is still largely restrained by V<sub>oc</sub> and FF losses at the CZTGSe/CdS interface which should be here the first area of improvement. This is preliminarily attempted via front surface sulfurization, but further investigations are required whether it concerns the Sn-Ge bandgap gradient design or the top interface quality using chemical treatments or alternative buffer materials.<br/><br/>This work has received funding from the European Union's Horizon 2020 research and innovation program under grant agreement 952982 (CUSTOM-ART project).

Keywords

defects

Symposium Organizers

Eric Colegrove, National Renewable Energy Laboratory
Jessica de Wild, imec
Byungha Shin, Korea Advanced Institute of Science and Technology
Colin Wolden, Colorado School of Mines

Publishing Alliance

MRS publishes with Springer Nature