Model for a-Si: H/c-Si interface recombination based on the amphoteric nature of silicon dangling bonds

The performance of many silicon devices is limited by electronic recombination losses at the crystalline silicon c-Si surface. A proper surface passivation scheme is needed to allow minimizing these losses. The surface passivation properties of amorphous hydrogenated silicon a-Si:H on monocrystalline Si wafers are investigated here. We introduce a simple model for the description of the surface recombination mechanism based on recombination through amphoteric defects, i.e. dangling bonds, already established for bulk a-Si:H. In this model, the injection-dependent recombination at the a-Si:H/c-Si interface is governed by the density and the average state of charge of the amphoteric recombination centers. We show that with our surface recombination model, we can discriminate between the respective contribution of the two main mechanisms leading to improved surface passivation, which is achieved by a the minimization of the density of recombination centers and b the strong reduction of the density of one carrier type near the interface by field effect. We can thereafter reproduce the behaviors experimentally observed for the dependence of the surface recombination on the injection level on different wafers, i.e., of both p and n doping type as well as intrinsic. Finally, we are able to exploit the good surface passivation properties of our a-Si:H layers by fabricating flat heterojunction solar cells with open-circuit voltages exceeding 700 mV.

[1]  A. Cuevas,et al.  Very low bulk and surface recombination in oxidized silicon wafers , 2002 .

[2]  Ch. Hof,et al.  MOBILITY LIFETIME PRODUCT : A TOOL FOR CORRELATING A-SI:H FILM PROPERTIES AND SOLAR CELL PERFORMANCES , 1996 .

[3]  Arvind Shah,et al.  Study of surface/interface and bulk defect density in a-Si:H by means of photothermal deflection spectroscopy and photoconductivity☆ , 1987 .

[4]  M. Stutzmann,et al.  Native defects at the Si/SiO2 interface-amorphous silicon revisited , 1985 .

[5]  Modeling of reverse bias dark currents in pin structures using amorphous and polymorphous silicon , 2004 .

[6]  Vaillant,et al.  Recombination at dangling bonds and steady-state photoconductivity in a-Si:H. , 1986, Physical review. B, Condensed matter.

[7]  Wilhelm Warta,et al.  Impact of illumination level and oxide parameters on Shockley–Read–Hall recombination at the Si‐SiO2 interface , 1992 .

[8]  Stefan W. Glunz,et al.  Investigation of various surface passivation schemes for silicon solar cells , 2006 .

[9]  R. Street Localized states in doped amorphous silicon , 1985 .

[10]  R. Hall Electron-Hole Recombination in Germanium , 1952 .

[11]  J. Simmons,et al.  Nonequilibrium Steady-State Statistics and Associated Effects for Insulators and Semiconductors Containing an Arbitrary Distribution of Traps , 1971 .

[12]  W. Read,et al.  Statistics of the Recombinations of Holes and Electrons , 1952 .

[13]  A. Goetzberger,et al.  Crystalline Silicon Solar Cells , 1998 .

[14]  H. Fujiwara,et al.  Real-time monitoring and process control in amorphous∕crystalline silicon heterojunction solar cells by spectroscopic ellipsometry and infrared spectroscopy , 2005 .

[15]  A. Aberle,et al.  Carrier recombination at silicon–silicon nitride interfaces fabricated by plasma-enhanced chemical vapor deposition , 1999 .

[16]  Krick,et al.  Nature of the dominant deep trap in amorphous silicon nitride. , 1988, Physical review. B, Condensed matter.

[17]  F. D. King,et al.  Minority carrier MIS tunnel diodes and their application to electron- and photo-voltaic energy conversion—I. Theory☆ , 1974 .

[18]  L. Korte,et al.  Electronic states in a-Si:H/c-Si heterostructures , 2006 .

[19]  S. Sze Semiconductor Devices: Physics and Technology , 1985 .

[20]  G. Beaucarne,et al.  Surface passivation properties of boron-doped plasma-enhanced chemical vapor deposited hydrogenated amorphous silicon films on p-type crystalline Si substrates , 2006 .

[21]  J. Pankove,et al.  Amorphous silicon as a passivant for crystalline silicon , 1979 .

[22]  Evangelisti,et al.  Low-energy yield spectroscopy as a novel technique for determining band offsets: Application to the c-Si(100)/a-Si:H-heterostructure. , 1995, Physical review letters.

[23]  R. Street,et al.  Hydrogenated amorphous silicon: Index , 1991 .

[24]  R. Hezel,et al.  Plasma Si nitride: A promising dielectric to achieve high-quality silicon MIS/IL solar cells , 1981 .

[25]  Yanfa Yan,et al.  Atomic structure and electronic properties of c-Si∕a-Si:H heterointerfaces , 2006 .

[26]  Li-Jen Cheng,et al.  Analysis of the interaction of a laser pulse with a silicon wafer - Determination of bulk lifetime and surface recombination velocity , 1987 .

[27]  R. Sinton,et al.  Contactless determination of current–voltage characteristics and minority‐carrier lifetimes in semiconductors from quasi‐steady‐state photoconductance data , 1996 .

[28]  Marc Burgelman,et al.  Modeling polycrystalline semiconductor solar cells , 2000 .

[29]  Liao Ke-jun,et al.  STUDIES OF SOME PROPERTIES OF MECHANICAL-STRESS IN A-SI-H, A-SINX-H AND A-SI-H/A-SINX-H HETEROJUNCTION FILMS , 1988 .

[30]  R. Street,et al.  Effects of doping on transport and deep trapping in hydrogenated amorphous silicon , 1983 .

[31]  A. Shah,et al.  Effects of dangling bonds on the recombination function in amorphous semiconductors , 1992 .

[32]  M. Meaudre,et al.  Method for the determination of the capture cross sections of electrons from space-charge-limited conduction in the dark and under illumination in amorphous semiconductors , 2004 .

[33]  R. Alcubilla,et al.  Characterization of a-Si:H∕c-Si interfaces by effective-lifetime measurements , 2005 .

[34]  Marc Burgelman,et al.  Modeling thin‐film PV devices , 2004 .

[35]  Arvind Shah,et al.  Consistency between Experimental Data for Ambipolar Diffusion Length and for Photoconductivity when Incorporated into the Standard Defect Model for a-Si:H , 1995 .