Low-cost bump-bonding processes for high energy physics pixel detectors

被引:7
作者
Caselle, M. [1 ]
Blank, T. [1 ]
Colombo, F. [2 ]
Dierlamm, A. [1 ,2 ]
Husemann, U. [2 ]
Kudella, S. [2 ]
Weber, M. [1 ,2 ]
机构
[1] Karlsruhe Inst Technol, Inst Data Proc & Elect IPE, Hermann von Helmholtz Pl 1, D-76344 Eggenstein Leopoldshafen, Germany
[2] Karlsruhe Inst Technol, Inst Expt Kernphys IEKP, Wolfgang Gaede Str 1, D-76131 Karlsruhe, Germany
基金
英国科学技术设施理事会;
关键词
Large detector systems for particle and astroparticle physics; Particle tracking detectors (Solid-state detectors);
D O I
10.1088/1748-0221/11/01/C01050
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
In the next generation of collider experiments detectors will be challenged by unprecedented particle fluxes. Thus large detector arrays of highly pixelated detectors with minimal dead area will be required at reasonable costs. Bump-bonding of pixel detectors has been shown to be a major cost-driver. KIT is one of five production centers of the CMS barrel pixel detector for the Phase I Upgrade. In this contribution the SnPb bump-bonding process and the production yield is reported. In parallel to the production of the new CMS pixel detector, several alternatives to the expensive photolithography electroplating/electroless metal deposition technologies are developing. Recent progress and challenges faced in the development of bump-bonding technology based on gold-stud bonding by thin (15 mu m) gold wire is presented. This technique allows producing metal bumps with diameters down to 30 mu m without using photolithography processes, which are typically required to provide suitable under bump metallization. The short setup time for the bumping process makes gold-stud bump-bonding highly attractive (and affordable) for the flip-chipping of single prototype ICs, which is the main limitation of the current photolithography processes.
引用
收藏
页数:9
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