Moisés Garín , Mansur Gamel , Marko Yli-Koski , Ville Vähänissi , Gerard Rivera , Hele Savin , Isidro Martín
{"title":"Carrier mobility in crystalline germanium at high injection: experimental characterization of carrier-carrier scattering","authors":"Moisés Garín , Mansur Gamel , Marko Yli-Koski , Ville Vähänissi , Gerard Rivera , Hele Savin , Isidro Martín","doi":"10.1016/j.solmat.2025.114011","DOIUrl":null,"url":null,"abstract":"<div><div>The decay of the sum of electron and hole mobilities, <em>μ</em><sub>s</sub> = <em>μ</em><sub>n</sub>+<em>μ</em><sub>p</sub>, due to carrier-carrier scattering was experimentally investigated in crystalline germanium (Ge) at high-injection conditions. Contactless measurements of the mobility sum as a function of the excess carrier density (Δ<em>n</em>) in Ge were obtained using photoconductance decay methods. First, the measurement method was revised and improvements were introduced to ensure that <em>μ</em><sub>s</sub>(Δ<em>n</em>) could be obtained for independent samples with improved accuracy. This method is successfully validated with crystalline silicon and, then, applied to Ge samples of different doping types and resistivity. The analysis of the data suggests that the mobility decay at high injection levels cannot be properly explained with the usual assumption of equal cross section for carrier-carrier and carrier-ion scattering events. Instead, we find the mobility sum due to carrier-carrier scattering to be inversely proportional to Δ<em>n</em> according to the expression 8 × 10<sup>20</sup>·Δ<em>n</em><sup>−1</sup> cm<sup>2</sup>V<sup>−1</sup>s<sup>−1</sup>. The limitations and potential error sources of the measurement method are discussed and, finally, the mobility model is used to improve lifetime analysis at high injection, allowing to estimate the ambipolar Auger recombination coefficient at <em>C</em><sub>amb</sub> = 7 × 10<sup>−31</sup> cm<sup>6</sup>s<sup>−1</sup>.</div></div>","PeriodicalId":429,"journal":{"name":"Solar Energy Materials and Solar Cells","volume":"295 ","pages":"Article 114011"},"PeriodicalIF":6.3000,"publicationDate":"2025-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Solar Energy Materials and Solar Cells","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0927024825006129","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
引用次数: 0
Abstract
The decay of the sum of electron and hole mobilities, μs = μn+μp, due to carrier-carrier scattering was experimentally investigated in crystalline germanium (Ge) at high-injection conditions. Contactless measurements of the mobility sum as a function of the excess carrier density (Δn) in Ge were obtained using photoconductance decay methods. First, the measurement method was revised and improvements were introduced to ensure that μs(Δn) could be obtained for independent samples with improved accuracy. This method is successfully validated with crystalline silicon and, then, applied to Ge samples of different doping types and resistivity. The analysis of the data suggests that the mobility decay at high injection levels cannot be properly explained with the usual assumption of equal cross section for carrier-carrier and carrier-ion scattering events. Instead, we find the mobility sum due to carrier-carrier scattering to be inversely proportional to Δn according to the expression 8 × 1020·Δn−1 cm2V−1s−1. The limitations and potential error sources of the measurement method are discussed and, finally, the mobility model is used to improve lifetime analysis at high injection, allowing to estimate the ambipolar Auger recombination coefficient at Camb = 7 × 10−31 cm6s−1.
期刊介绍:
Solar Energy Materials & Solar Cells is intended as a vehicle for the dissemination of research results on materials science and technology related to photovoltaic, photothermal and photoelectrochemical solar energy conversion. Materials science is taken in the broadest possible sense and encompasses physics, chemistry, optics, materials fabrication and analysis for all types of materials.