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Photovoltaics: new materials for better efficiency

Pere ROCA
Pere Roca i Cabarrocas
CNRS Research Director at LPICM* at École Polytechnique (IP Paris) and scientific director of Institut Photovoltaïque d'Île-de-France (IPVF)
Key takeaways
  • The global solar energy market today is 95% silicon-based – although, silicon is not actually the most ideal material for photovoltaic panels because it does not absorb light very well.
  • Researchers are looking at alternatives such as thin-film solar cell technology and perovskites.
  • Perovskites have now reached the same level of performance as silicon (with an energy conversion of more than 25%), but they are unstable, a problem that still needs to be resolved.
  • Photovoltaics in tandem (silicon and perovskites together) are promising since their efficiency can exceed 30%.

Sol­ar photo­vol­ta­ic (PV) tech­no­logy has grown almost expo­nen­tially over the past 15 years and is now cost-com­pet­it­ive with fossil fuels. Remark­ably, the under­ly­ing PV struc­ture has remained vir­tu­ally unchanged since its devel­op­ment at Bell Labor­at­or­ies in 1954. Indeed, mod­ern sol­ar cells are still based on a simple junc­tion between ‘n’ type (elec­tron-rich) sil­ic­on and ‘p’ type (hole-rich) sil­ic­on. The first sol­ar cells con­ver­ted sun­light into elec­tri­city with an effi­ciency of about 5%, a fig­ure that has soared to over 25% in recent years thanks to more soph­ist­ic­ated cell design, namely the addi­tion of highly doped sil­ic­on and anti-reflec­tion layers.

Although sil­ic­on still accounts for about 95% of the glob­al sol­ar energy mar­ket, it has one major draw­back: it does not absorb light very well. Large thick­nesses of mater­i­al – to the order of hun­dreds of microns – are there­fore required. Since this is a long dis­tance for elec­trons to travel, PV-grade sil­ic­on must be highly crys­tal­line and very pure for the charge car­ri­ers to effi­ciently pass through. Fab­ric­at­ing such mater­i­al is com­plex, how­ever, and there­fore expensive.

Changing our approach to silicon

To reduce pro­duc­tion costs and the amount of mater­i­al needed, research­ers have long been look­ing into altern­at­ive mater­i­als. My team is focus­ing on thin-film sol­ar cell tech­no­logy, so-called because the films only need to be a few microns thick for suf­fi­cient optic­al absorp­tion. Lower qual­ity, lower pur­ity mater­i­als are also accept­able and they can be fab­ric­ated using rap­id depos­ition meth­ods: evap­or­a­tion, dir­ect-to-glass sput­ter­ing or plasma enhanced chem­ic­al vapour depos­ition (PECVD). These mater­i­als, which include hydro­gen­ated amorph­ous sil­ic­on, cad­mi­um tel­lur­ide (CdTe) and cop­per indi­um gal­li­um sel­en­ide (CuIn1-xGax­Se2, or CIGS for short), make for very effi­cient cells and can be grown on any type of substrate.

The effi­ciency of sol­ar cells that con­vert sun­light into elec­tri­city has increased from 5% to 25% in recent years.

Today, crys­tal­line sil­ic­on wafers are con­ven­tion­ally fab­ric­ated by draw­ing ingots and then cut­ting them into wafers about 180 µm thick. We are try­ing to break new ground in the way crys­tal­line sil­ic­on is made by using new growth tech­niques that rely on low-tem­per­at­ure PECVD pro­cesses – that is, between 150 and 300 degrees Celsi­us. We are also using this tech­nique to make ‘III‑V’ mater­i­als which, although widely used in opto­elec­tron­ics, are about 100 times more expens­ive than crys­tal­line sil­ic­on. In the world of photo­vol­ta­ics, costs must be reduced to com­pete with crys­tal­line silicon.

The stand­ard meth­ods for cre­at­ing III‑V mater­i­als are molecu­lar beam epi­taxy (MBE) and met­al organ­ic chem­ic­al vapour decom­pos­i­tion (MOCVD). These epi­taxi­al growth meth­ods require ultra-high vacu­um envir­on­ments for MBE and high tem­per­at­ures (700‑1000°C) for MOCVD, mak­ing them expens­ive. The plasma depos­ition pro­cesses that we are devel­op­ing at LPICMt in col­lab­or­a­tion with the Insti­tut Photo­voltaïque d’Ile de France (IPVF) aim to reduce this cost. This is one of the last vari­ables we have any con­trol over as III‑V com­pounds are already at the max­im­um of their effi­ciency when it comes to con­vert­ing sol­ar radi­ation into electricity.

Perovskites: a new material

Per­ovskites are anoth­er class of mater­i­als we are work­ing on. These are crys­tal­line mater­i­als with the struc­ture ABX3, where A is cae­si­um, methyl­am­moni­um (MA) or form­amidini­um (FA), B is lead or tin and X is chlor­ine, brom­ine or iod­ine. They are prom­ising can­did­ates for thin-film sol­ar cells because they can absorb light over a wide range of wavelengths of the sol­ar spec­trum thanks to their tune­able elec­tron­ic band gaps 1. Charge car­ri­ers (elec­trons and holes) can also dif­fuse quickly and over long dis­tances. These prop­er­ties mean that per­ovskite sol­ar cells now boast an energy con­ver­sion effi­ciency of over 25%, put­ting their per­form­ance on a par with estab­lished sol­ar cell mater­i­als such as sil­ic­on, gal­li­um arsen­ide and cad­mi­um telluride.

While we know how to make them cheaply and effi­ciently, the prob­lem is that per­ovskites con­tain nat­ur­al sur­face defects and suf­fer from struc­tur­al changes known as ion migra­tion. Both of these factors tend to make per­ovskite films unstable and these instabil­it­ies become even more pro­nounced in the pres­ence of mois­ture and high­er tem­per­at­ures. To improve their sta­bil­ity, we need to under­stand these mater­i­als and the inter­faces between the dif­fer­ent com­pon­ents that make up the sol­ar cell.

This will be a chal­lenge, but it is worth it, because per­ovskites are very ver­sat­ile: their opto­elec­tron­ic prop­er­ties can be manip­u­lated quite eas­ily by simple chem­ic­al modi­fic­a­tions. Thanks to their incred­ible light absorp­tion capa­city, they can be used not only in sol­ar cells, but also in light-emit­ting diodes and oth­er elec­tron­ic applic­a­tions. Research on per­ovskites is boom­ing and thou­sands of stud­ies are pub­lished every year.

Tandem cells 

The next ques­tion is: how do we go bey­ond cur­rent effi­cien­cies? While optim­ising mater­i­als and inter­faces is cru­cial, per­ovskites can also be added to estab­lished sol­ar cell tech­no­lo­gies (such as sil­ic­on) to build so-called tan­dem sol­ar cells. This is the sub­ject of research at the IPVF and it is an extremely inter­est­ing way to increase the over­all effi­ciency of devices. Sil­ic­on-only- and per­ovskite-only cells can both achieve effi­cien­cies of 26%, but if you put them togeth­er you can push the effi­ciency to a high­er value (to bey­ond 30%). High­er effi­cien­cies mean, for example, that you can cov­er a smal­ler area with your PV pan­el to get the same energy out­put – in oth­er words, it costs less.

Cells made solely of sil­ic­on or per­ovskite can achieve effi­cien­cies of 26%, but togeth­er this value can exceed 30%.

So, what are the best mater­i­als? If we are able to solve the sta­bil­ity of per­ovskites, they seem the most prom­ising. III-Vs are also inter­est­ing, but we need to reduce their cost. To address cli­mate change, our chal­lenge is to devel­op ter­awatts of photo­vol­ta­ic pan­els, which means man­u­fac­tur­ing large quant­it­ies of photo­vol­ta­ic pan­els that require large install­a­tion areas. Increas­ing their effi­ciency while decreas­ing the thick­ness of the cells is the best way to reduce the amount of mater­i­al used.

There are also oth­er prob­lems to be solved, such as recyc­ling the photo­vol­ta­ic mater­i­als and keep­ing them free of dust so that they can con­tin­ue to absorb sol­ar radi­ation effi­ciently. We are work­ing on the eco-design of sol­ar cells that can be recycled to recov­er the con­stitu­ent mater­i­als. Photo­vol­ta­ic plants are in fact pre­cious met­al ‘mines’. Per­ovskites also con­tain lead, which is tox­ic and could leach out of a cell in the event of flood­ing or fire. This aspect of PV tech­no­logy is a research top­ic in itself and could be the sub­ject of a future article.

Interview by Isabelle Dumé 
1The energy ranges between the valence band and the con­duc­tion band where elec­tron­ic states are for­bid­den.

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