I. Introduction
Silicon heterojunction (SHJ) solar cells are increasingly attracting attention, thanks to their potential for stable high conversion efficiencies at competitive production costs [1]. Record efficiencies of 24.7% [2] and 25.6% [3] were recently reported by Panasonic, Japan, for standard two-side-contacted and interdigitated back-contacted device structures, respectively. These results refer to devices certified under standard testing conditions (STC, 1000 W·m−2, 25 °C, AM1.5 g spectrum). Independently from these outstanding results, the values taken in STC and used for certification could be questioned, as encapsulated devices deployed in the field can reach operating-temperatures (T) as high as 90 °C [4]. In fact, photovoltaic devices typically show significant performance losses with increasing T. Hence, the temperature coefficient of the conversion efficiency () represents an important figure-of-merit for the energy yield of a given photovoltaic technology.
1If not stated differently, we refer to TC as the relative temperature coefficient, i.e., for a solar cell parameter X (open-circuit voltage, etc.), TC = 1/X0 X/T (X0: value at the reference temperature, typically 25 °C) [5]. The absolute TC refers to the absolute value of X/T.
In this respect, compared to conventional crystalline silicon homojunction technologies ( for standard homojunction and −0.35%/°C for homojunctions with passivating contacts [6]), SHJ solar cells are less sensitive to increasing operation temperatures ( [7] to −0.1%/°C [8]2This is comparable with thin-film solar cells, which exhibit high Vocs as well [9].
). To underline the importance of a favorable , starting from a 20%-efficient cell (at 25 °C), a difference in of 0.12 or 0.35%/°C results in ∼5.4 or 15.8% relative difference in efficiency at an operating-temperature of 70 °C.