Electrical performance of Ti/Pt thin films on glass-ceramic substrates after high temperature loading |
| |
Authors: | U. Schmid and M. Grosser |
| |
Affiliation: | (1) Vienna University of Technology, Department for Microsystems Technology, Institute of Sensor and Actuator Systems, Floragasse 7, 1040 Vienna, Austria;(2) Chair of Micromechanics, Microfluidics/Microactuators, Faculty of Natural Sciences and Technology II, Saarland University, 66123 Saarbruecken, Germany |
| |
Abstract: | In this study, the influence of post-deposition annealings (PDA) up to temperatures of T PDA=700°C on the room-temperature resistivity of e-beam evaporated titanium/platinum (Ti/Pt) bi-layers on low temperature co-fired (LTCC) substrates covered with a glass encapsulate is investigated. The thickness of the platinum top layer is varied between 24 and 95 nm (titanium film thickness: 5 nm) and between 23 and 90 nm (titanium film thickness: 15 nm), respectively. In the “as-deposited” state and up to post-deposition annealing temperatures of T PDA=450°C, the film resistivity is linearly correlated with the reciprocal value of the platinum film thickness according to the size effect. When applying, however, solely the Fuchs-Sondheimer model for evaluation, the effective mean free path for electrons is substantially above the value reported for crystalline platinum at room temperature. Compared to similar investigations on smooth Si/SiO2 substrates yielding interpretable results within this theoretical approach, this is due to the increase of the thickness-dependent fraction in film resistivity which is strongly affected by the enhanced LTCC/glass surface roughness. At T PDA>600°C, diffusion of titanium into the platinum top layer and the roughening of the LTCC/glass substrate dominate the electrical behavior, both causing an increase in film resistivity above average. In contrast to Si/SiO2 substrates, thermal induced grooving effects in the Pt top layer play a minor role as the temperature coefficients of expansion of metallization and glass-ceramic substrate match better and the effective temperature difference for stress generation is lower due a glass softening temperature of about 450°C. |
| |
Keywords: | KeywordHeading" >PACS 68.60.Dv 72.10.Fk 73.50.Bk 73.61.-r |
本文献已被 SpringerLink 等数据库收录! |
|