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Laser-Doped Selective Emitters (LDSE) with a Green CW Laser

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Laser-Doped Selective Emitters (LDSE) with a Green CW Laser Industrial Laser Application Focus Applications Lab No. 9 Laser-Doped Selective Emitters (LDSE) LasWeri-tDho ap eGdr eSeenl eCcWtiv eLaser CrCysrytasltlainllein-Se-ilSiciloicno (nc -(Sc-i)S si)o slaorl acre cllesl lcso cnotinntuineu teo tboe b ae lae aledaedr earm aomnognsgt stth ethe various competing solar cell vatreiocuhsn ocloomgipeest.i nRge assoolanrs c feolrl theicsh innocllougdie ss.t aRbelaes osunps pfloyr otfh issi lincoclnu,d we esltla-dbeleveloped Emsiumptpalnyt uoffa ecstiluicriornng, spwroecl le-dse(seveLs,l oapnDedd, omfa cSnouufrasceEt,u trhine)g h p igrohwc aenssde gsri, oawtnidn,hg o cf ocno vuera srsei,on the fhfiicgihe nacnide sg trhoawt incagn c obnev aecrhsioenve edf.f iHcieernec, iwese t rheapto crat no nb eL aascehri eDvoepde. dH Sereele, cwtie ve repEomrtit toenr sL a(LsDeSr ED)o –p ead r eSlealteivcetilvye s Etrmaigtthetrfso r(LwDaSrdE,) l–a sae r-eblatsievde lymanufacturing process Grestrtaehiagth htnfaosr wb eaerdnC, dlaesmeWro-nbsatsreadte m d atLhnautf aiatc tcuarnisn ign cperreoacseers sc ethlla et fhfiacsie bnecey nb ys huopw tno t1o –2% gepnoeirnattse oavbesro cluotnev ecnetlli oenfafilc cieenllcsy. gains of 1–2% over conventional cells. A conventional p-type wafer c-Si solar cell has a thin but heavily-doped n++ region of silicon on the front surface. This region, generated via high- A conventional p-type wafer c-Si solar cell has a thin but heavily-doped n ++ region temperature phosphorus gas furnace diffusion, forms a p-n junction, of silicon on the front surface. This region, generated via high-temperature directing current flow into a grid pattern of thin conducting strips on the cell phosphorus gas furnace diffusion, forms a p-n junction, directing current flow into surface. These are referred to as finger lines, and consist of a metallic paste a grid pattern of thin conducting strips on the cell surface. These are referred to as material that is screen printed onto the cell surface and subsequently finger lines , and consist of a metallic paste material that is screen printed onto the Gcaeulls siuarnf amcaec hainidng (top) and flattop machining (bottom) microscope “baked-in” at high-temperature, creating electrical contacts to the image and 3D depth profile trace heavily-doped n ++ emitter region of the cell. In partnership with the ARC Photovoltaic Centre of Excellence at the University of New South Wales in Sydney, Australia, we have used LDSE processing combined with a light-induced plating (LIP) metallization technique to improve cell efficiency. Using Spectra-Physics’ Millennia ® Prime™ 15 W, 532 nm CW laser, the result has been the fabrication of high-efficiency solar cells with minimal impact to the overall cell processing line and with fewer high-temperature steps. By scanning the focused laser beam over the areas to be metalized, localized heavy doping regions in silicon are formed. Then, during the light-induced plating step, metal atoms in solution plate only on the doped regions, in what amounts to a self-aligning metallization process. The localized doping results in less “dead” area on the cell; and the shorter, narrower finger lines reduce losses due to shadowing of the Basic differences between conventional screen-printed and LDSE/electroplated solar cell architecture incoming light. Several aspects of this conventional design place limits on cell performance: the screen printed finger lines are somewhat wide and tall, resulting in shadowing of incoming light; also, the n++ emitter region covering the entire cell front surface means reduced photovoltaic action for blue light that is absorbed closer to the wafer’s surface; and finally, there are several high-temperature process steps which can increase damage to the crystal structure. Laser-Doped Selective Emitters (LDSE) With a Green CW Laser 1.0E+21 Various studies 1,2 have been conducted aimed at characterizing the 4 m/s 1.0E+20 performance of solar cells after LDSE processing with the Millennia laser. 6 m/s ) 3 Data tabulated below show cell performance when processed at various - 10 m/s m c ( 1.0E+19 . beam scanning speeds: c n o c t n 1.0E+18 a p V J o Scan Speed oc sc FF n D 1.0E+17 0.5 m/sec 635 mV 37.4 mA/cm 2 78% 18.5% 2 m/sec 634 mV 37.4 mA/cm 2 78% 18.5% 1.0E+16 0 123 4 6 m/sec 631 mV 37.6 mA/cm 2 77% 18.1% Depth (µm) SIMS data plot illustrating dopant concentration below the wafer surface for While the best-performing cells are achieved at scan speeds of 2 m/sec and various LDSE scan speeds below, even the 6 m/sec scan speed resulted in good performance. For a With slower scan speeds, there is increased dopant diffusion deeper into 125 mm solar cell, 2 m/sec scan speed results in 10–12 seconds per wafer the silicon wafer; whereas faster scan speeds result in shallower doping processing time; whereas the time for a 6 m/sec scan speed is in the depths. Controlling the laser power can also control the strength and 3–5 second range. depth of the doping. Hence, depending on other aspects of the solar cell design, the dopant profile (and therefore junction depth) can be easily fine- tuned for optimal cell performance, which is a powerful tool to have both in the laboratory and on the production floor. While there are various competing laser technologies for the LDSE process, Millennia Prime 532 nm CW lasers has established a proven track record of generating high-efficiency solar cells. And considering the high reliability of the laser, it is the perfect tool for the manufacture of next generation high-efficiency crystalline silicon solar cells. 1 A. Sugianto et. al., Proc. 35th IEEE PVSC (2010) 2 B. Tjahjono et. al., Proc. 25th EU PVSEC, (2010) SEM image showing cross-sectional perspective of nickel-copper plated LDSE finger line . Image courtesy of UNSW. Product: Millenia Prime The Spectra-Physics Millennia ® Prime™ laser is an excellent tool for LDSE processing. It offers high CW output power (15 W) at the 532 nm wavelength with excellent beam quality, which is important for maximizing the intensity at the workpiece. Furthermore, the stable, reliable, and robust performance of the laser are well suited for exceeding the demands of today’s high-volume, high- yield, and high-uptime manufacturing environments. Spectra-Physics ® Lasers Sales 1-800-775-5273 [email protected] www.newport.com/spectra-physics © 2011 Newport Corporation. All rights reserved. Millennia, Spectra-Physics, the Spectra-Physics logo and the Newport logo are registered trademarks of Newport Corporation. Prime is a trademark of Newport Corporation. q09 DS-041103.
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