Abstract

Laser doping of silicon with the help of precursors is well established in photovoltaics. Upon illumination with the constant or pulsed laser beam, the silicon melts and doping atoms from the doping precursor diffuse into the melted silicon. With the proper laser parameters, after resolidification, the silicon is doped without any lattice defects. Depending on laser energy and on the kind of precursor, the precursor either melts or evaporates during the laser process. For high enough laser energies, even parts of the silicon’s surface evaporate. Here, we present a unified model and simulation program, which considers all these cases. We exemplify our model with experiments and simulations of laser doping from a boron oxide precursor layer. In contrast to previous models, we are able to predict not only the width and depth of the patterns on the deformed silicon surface but also the doping profiles over a wide range of laser energies. In addition, we also show that the diffusion of the boron atoms in the molten Si is boosted by a thermally induced convection in the silicon melt: the Gaussian intensity distribution of the laser beam increases the temperature-gradient-induced surface tension gradient, causing the molten Si to circulate by Marangoni convection. Laser pulse energy densities above H > 2.8 J/cm2 lead not only to evaporation of the precursor, but also to a partial evaporation of the molten silicon. Without considering the evaporation of Si, it is not possible to correctly predict the doping profiles for high laser energies. About 50% of the evaporated materials recondense and resolidify on the wafer surface. The recondensed material from each laser pulse forms a dopant source for the subsequent laser pulses.

Highlights

  • IntroductionPublisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations

  • This section validates the present model via a comparison with the experimental data

  • Previous models were either limited to precursor layers with a high melting and evaporation temperature [13], or they did not work when silicon evaporates due to high laser pulse energy densities [13,14,30]

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Summary

Introduction

Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. They used a boron precursor, a pulsed laser of 532 nm wavelength and a 42 ns pulse duration (at full width at half maximum (FWHM) and medium laser pulse energy densities For these experimental conditions, their model [13] explained the measured doping profiles well. (ii) Gas/Melt-Doping: Doping of the Si melt from the gas phase; in this case, the precursor evaporates and doping of the Si melt takes place from the gas phase This process resembles classic doping using a doping furnace and a gaseous doping source. The present work presents a unified model, which is able to cover all three possibilities (solid/melt, gas/melt, gas/gas-melt) of laser doping, including the high energy regime in which the doping precursor as well as parts of the silicon’s surface evaporate. It allow us to predict the diffusion profiles over a wide range of laser pulse energy densities H

Pulse Energy Density Regimes
Laser Beam
Principles of Laser Doping
Experimental Results
Surface Profiles
Melting and Resolidification
Doping Profiles
Numerical Simulation
Numerical Discretization
Laser Absorption
Heat Transfer
Diffusion
Recondensation
Discussion and Conclusions
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