Abstract

Laser doping, though able to improve cell characteristics, enables the formation of a selective emitter without the need for additional processing. Its parameters should be investigated to minimize laser defects, such as the heat-affected zone (HAZ), and to obtain a low contact resistance. Herein, the laser fluence and speed were changed to optimize process conditions. Under a laser fluence of 1.77 J/cm2 or more, the surface deteriorated due to the formation of the HAZ during the formation of the laser doping selective emitter (LDSE). The HAZ prevented the formation of the LDSE and impaired cell characteristics. Therefore, the laser speeds were changed from 10 to 70 mm/s. The lowest contact resistivity of 1.8 mΩ·cm2 was obtained under a laser fluence and speed of 1.29 J/cm2 and 10 mm/s, respectively. However, the surface had an irregular structure due to the melting phenomenon, and many by-products were formed. This may have degraded the efficiency due to the increased contact reflectivity. Thus, we obtained the lowest contact resistivity of 3.42 mΩ·cm2, and the damage was minimized under the laser fluence and speed of 1.29 J/cm2 and 40 mm/s, respectively.

Highlights

  • The solar industry has been attracting attention as a future energy source, and the demand and supply market for crystalline silicon (c-Si) solar cells has been gradually expanding

  • The results showed that as the laser fluence increased, the doping level increased and sheet fluence increased, the doping level increased and sheet resistance decreased

  • The lightly and heavily doped emitters were formed using a diffusion furnace and a laser, and the characterization was conducted based on their sheet resistance, SEM, and transmission line method (TLM) measurements

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Summary

Introduction

The solar industry has been attracting attention as a future energy source, and the demand and supply market for crystalline silicon (c-Si) solar cells has been gradually expanding. New methods of increasing efficiency involve cell design modifications using selective emitters [4]. In contrast to a conventional single emitter, a selective emitter is a heavily doped region with a large depth of impurity diffusion in the electrode region. A lightly doped region with a small depth of impurity diffusion is formed in the non-electrode region. A heavily doped region can reduce the contact resistance between the front electrode and the emitter, and it can increase the open-circuit voltage (Voc ). A lightly doped region reduces the recombination at the surface and offers excellent quantum efficiency characteristics in the short wavelength region. Selective emitter solar cells can increase efficiency by utilizing low-concentration and high-concentration emitters

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