Infrared and Laser Engineering, Volume. 54, Issue 1, 20240315(2025)

A study of the effect of evaporation factors on indium bumps in high density infrared focal plane

Pengfei BAO1,2,3, Xianliang ZHU1,2、*, Chunlei YU1,2, Bo YANG1,2, Xiumei SHAO1,2, Xue LI1,2, and Dafu LIU1,2
Author Affiliations
  • 1State Key Laboratory of Transducer Technology, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
  • 2Key Laboratory of Infrared Imaging Materials and Detectors, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    Objective The preparation of a high consistency, high aspect ratio indium bump arrays represent a pivotal technology for fabricating high density focal plane array (FPA). Indium is one of the most commonly utilized materials for interconnecting bumps in FPAs, particularly cooled FPAs, due to its exceptional ductility, electrical conductivity, thermal conductivity, and other properties. The current research on indium bump growth is primarily concerned with the macroscopic effects of process parameters on the growth of indium bump. However, there is a paucity of in-depth reports on the growth mechanism of indium bump. When considered in conjunction with the theory of thin-film nucleation growth, the impact of pivotal process parameters, such as substrate temperature and deposition rate, on the growth of indium bumps can be elucidated from a microscopic perspective. This offers a theoretical and technical foundation for developing and preparing indium bump arrays with smaller pixel pitch.Methods According to the indium bump growth model (Fig.1), indium bump arrays with an image element spacing of 10 μm and a photolithography pattern diameter of 6 μm (abbreviated as P10-Φ6) were studied, and indium bump arrays were obtained by thermal evaporation method under different growth parameters. The morphological differences (Fig.2(a)-(f)), high uniformity (Fig.3(a)-(b)), top diameter uniformity (Fig.4(a)-(b)), and indium bump growth rate differences (Fig.5(a)-(b)) of the indium bump arrays were comparatively analyzed with the theory of thin film micro growth for the indium bump arrays with three different substrate temperatures (T0 K, T0-30 K, and T0-45 K). Comparative analysis of indium bump arrays at three different deposition rates (VV0+2 Å/s, VV0+15 Å/s, and VV0+23 Å/s) in terms of morphology difference (Fig.6(a)-(f)), height uniformity (Fig.7(a)-(b)) and top diameter uniformity (Fig.8(a)-(b)), indium bump growth rate differences (Fig.9(a)-(b)).Results and Discussions The standard deviation of the height distribution of indium bumps decreased from 0.22 to 0.14 and 0.09(Fig.3(a)-(b)), the height nonuniformity from 15.4% to 11.8% and 6.6%(Fig.3(a)-(b)), and the standard deviation of the top diameters from 0.64 to 0.43 and 0.37(Fig.4(a)-(b)), respectively, when the substrate temperature was decreased from T0 K to T0-30 K and T0-45 K. This resulted in an improvement in the homogeneity of the indium bump arrays. Nevertheless, a reduction in the substrate temperature from T0-30 K to T0-45 K has been observed to increase the lateral growth rate of the indium layer from 3.4 Å/s to 4.1 Å/s(Fig.5(a)-(b)). This is an unfavorable phenomenon for the growth of indium bumps with high aspect ratio. The increase in deposition rate from VV0+2 Å/s to VV0+15 Å/s and VV0+23 Å/s resulted in a reduction in the standard deviation of the indium bump height distribution from 0.14 to 0.09(Fig.7(a)-(b)), the height nonuniformity from 11.8% to 8.1%(Fig.7(a)-(b)), and the standard deviation of the top diameter of the indium bumps from 0.49 to 0.31(Fig.8(a)-(b)). The standard deviation of the top diameter of the indium bumps decreased from 0.49 to 0.31 and 0.34(Fig.8(a)-(b)), respectively. The increase in deposition rate resulted in enhanced indium bump uniformity. Nevertheless, when the deposition rate is elevated from VV0+15 Å/s to VV0+23 Å/s, the indium film roughness undergoes a mere 0.001 μm alteration(Fig.9(a)-(b)). Additionally, the lateral growth rate of the indium layer demonstrates a linear correlation with the deposition rate, thereby limiting the potential for further enhancement of indium bumps through the continued pursuit of elevated deposition rates.Conclusions On the one hand, high deposition rates and low substrate temperatures result in the refinement of indium film grains and facilitate the deposition of highly uniform indium bump arrays. Following a decrease in substrate temperature of 45K, the nonuniformity of the indium bump height was observed to decrease from 15.4% to 6.6%. In contrast, the indium bumps' top diameter range difference decreased by 0.9 μm. Following an increase in deposition rate of 21 Å/s, the indium bump height nonuniformity decreased from 11.8% to 6.6%, and the top diameter range difference of indium bumps decreased by 0.4 μm. Conversely, the impact of kinematic roughening in the high deposition rate specific gravity increases, while indium film roughness moderates with the deposition rate. Concurrently, the capacity of indium diffusion from the photolithography pattern edge to the surrounding area is diminished at a high deposition rate and low substrate temperature.Furthermore, the lateral growth rate of the indium layer increases from 3.4 Å/s to 4.1 Å/s following sustained temperature reduction. However, accelerated closure of the photolithography pattern is not conducive to the growth and preparation of high density, high aspect ratio and high uniformity indium bumps. The effects of the deposition rate and substrate temperature on indium bump growth are twofold. In order to obtain indium bump arrays with flat tops, high uniformity, and full morphology, it is necessary to select a suitable combination of substrate temperature and deposition rate parameters for small pitch focal planes.

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    Pengfei BAO, Xianliang ZHU, Chunlei YU, Bo YANG, Xiumei SHAO, Xue LI, Dafu LIU. A study of the effect of evaporation factors on indium bumps in high density infrared focal plane[J]. Infrared and Laser Engineering, 2025, 54(1): 20240315

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    Paper Information

    Category: 红外技术及应用

    Received: Jul. 11, 2024

    Accepted: --

    Published Online: Feb. 12, 2025

    The Author Email:

    DOI:10.3788/IRLA20240315

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