Elsevier

Materials Science and Engineering: A

Volume 744, 28 January 2019, Pages 746-753
Materials Science and Engineering: A

Cohesive and adhesive properties of nanocrystalline Ti thin films on polyimide substrates

https://doi.org/10.1016/j.msea.2018.12.089Get rights and content

Abstract

In this work, cohesive and adhesive properties of Ti thin films on polyimide substrates were studied systematically as a function of grain size by in situ optical microscopy, resistance measurements and synchrotron X-ray diffraction under uniaxial tensile testing. The characteristic of cohesive and adhesive behavior can be well reflected in the stress-strain curves determined by synchrotron X-ray diffraction. Generally, the yield strength decreases while the cracking strain increases with increasing grain size, due to the constraint effect of grain size on dislocation activity. Different from the yield strength, the fracture strength is almost unchanged with grain size. The fracture toughness is found to increase as the grain size increases, which is attributed to the enhanced plasticity during fracture process. Additionally, the interfacial adhesion energy is determined to be 3.8 J m−2. The buckling strain increases with increasing grain size as a result of enhanced plastic dissipation. The formation of patches, instead of buckles, in Ti film with smaller grain size is ascribed to the low deformation capability of the film.

Introduction

Titanium (Ti) thin films have arose much more attention for their extensive applications in microelectromechanical systems (MEMS), medical implants, and intelligent materials due to high mechanical strength, excellent thermal stability, good corrosion resistance in extreme conditions and intrinsic biocompatibility [1], [2], [3], [4]. Many works have been focused on the investigation of chemical and structural characteristics [1], [5], [6], phase transformation [7], [8], and hardness/strength [9] of Ti thin films, and also their dependence on film thickness [10], temperature [9], and deposition conditions [6]. Generally, pure Ti and most its alloys form an hexagonal close-packed (hcp) structure (α-Ti) under the low temperature condition, and it is transformed into a body-centered cubic (bcc) structure (β-Ti) under the high temperature condition [11]. Additionally, a phase transformation from face-centered cubic (fcc) to hcp structure with increasing film thickness (h) has been observed in polycrystalline Ti thin films [7].

Recently, with the emergence and rapid development of flexible electronics, composing of metallic thin films on flexible substrates, complex service environment brings forth the increasingly stringent requirements for materials. The capabilities to be bent, folded, stretched, compressed, twisted and even deformed to arbitrary shapes without failure are needed for the effective utilization of metallic film/compliant substrate systems. Consequently, much effort has been devoted to cohesive and adhesive failure/properties and their film thickness dependence [12], [13], [14], [15], [16], [17], [18]. Lu et al. [14] and Niu et al. [19] performed uniaxial tensile tests on polyimide-supported Cu films and reported an monotonically enhanced cracking strain (εC) with increasing film thicknesses. Frank et al. [20], [21] investigated the cohesive and adhesive failure of thin tantalum films by an uniaxial tensile testing combined with in situ optical microscopy and synchrotron X-ray diffraction and developed a two dimensional shear lag model to describe the biaxial stress field within a film fragment. The cracking strain was found to decrease as the film thickness increases [21]. Similar results were also reported in polyethylene terephthalate (PET) substrates-supported Cr films [22]. Schlich et al. [12], [23] revealed two different film thickness dependence of the buckling strain (εB) and proposed two delamination mechanisms to describe them. For fracture toughness measurements on thin films, several methods such as indentation-based techniques [24], [25], bulge tests [26], [27] and tensile tests [20], [28] have been used. However, only the tensile tests will be suitable to determine the fracture toughness (KIC) for films adherent to flexible substrates. Based on tensile tests, some energy-based models [20], [29], [30] have been developed.

Actually, the aforementioned works mainly focused on the Ti films adherent to the rigid substrates, such as Si wafer. Yet, to date, the cohesive and adhesive properties of Ti films on compliant substrates were less studied, although such systems are also widely employed as adhesion layers [16], [31] in flexible electronics, as bolometers in infrared sensors [32], and as electrical connectors in thermal insulating structures [33]. Therefore, systematic investigation of the mechanical properties of Ti films on compliant substrates needs to be developed urgently. Additionally, it is well known that the grain size usually increases with film thickness for metallic films [14], [34], [35]. Thus, the film thickness dependence of the cohesive and adhesive properties in previous works is usually a result of the superposition influence of film thickness and grain size. The individual effect of grain size on the cohesive and adhesive properties is still unclear and the underlying mechanism is also poorly understood. In this work, we overcome this gap by investigating the cohesive and adhesive properties of Ti thin films with the same thickness but different grain sizes (d) ranging from 20 nm to 80 nm. Uniaxial tensile testing combined with synchrotron X-ray diffraction, optical microscopy, and resistance measurements are performed to determine the cracking strain, yield strength, fracture strength, fracture toughness, buckling strain, and adhesion energy. Also, these properties will be discussed elaborately in light of the grain size-dependent deformation.

Section snippets

Sample preparation

Ti thin films with the same film thickness h (h= 600 nm) but different average grain sizes d were deposited on the 125 μm-thick polyimide substrates by using a magnetron sputtering system with a base pressure lower than 5 × 10−5 Pa. Prior to deposition, the polyimide substrates were cleaned for 10 min by ultrasonic treatment in actone and isopropyl alcohol sequentially. Ti films were sputtered through a mask, matching the size of the gage section of the sample. The grain sizes were controlled

Microstructure and residual stress

XRD patterns (not shown here) of Ti thin films reveal a single-phase hexagonal close-packed (hcp) Ti structure with (10-10), (0002) and (10-11) peaks. Typical planar-view bright-field and dark-field TEM micrographs are shown in Fig. 1a-e, exhibiting the approximately equiaxed grain in Ti films. The selected area diffraction patterns inserted show random in-plane orientations. The statistical distributions of grain sizes are shown in Fig. 1f, where the average grain sizes were determined to be ~

Residual stress

Many studies [42], [43], [44] have concentrated on the residual stress of sputtered films. The tensile residual stress was found in present Ti films, which mainly originated from an island coalescence mechanism [44], [45], where neighboring grains in the growing film are presumed to spontaneously join together under the action of interatomic forces. The decreasing σr with increasing deposition rate can be attributed to the enhanced atomic peening effect during deposition [44].

Length scale dependent cohesive properties

Strengthening with

Conclusions

In conclusion, the grain size effect on cohesive and adhesive properties of Ti films was determined by in situ optical microscopy, resistance measurements and synchrotron X-ray diffraction under uniaxial tensile testing. Both of the cracking strain and buckling strain increase with increasing grain size, which suggests an alternative way to improve simultaneously the cracking and buckling resistance. The yield strength is found to increase as the grain size decreases, while the fracture

Acknowledgements

This work was supported by the National Natural Science Foundation of China (Grant Nos. 51621063, 51571157, 51625103, 51790482, 51761135031, 51722104, 51790484 and 51801146), the National Key Research and Development Program of China (2017YFB0702301) and the 111 Project of China (B06025). This work is also supported by the International Joint Laboratory for Micro/Nano Manufacturing and Measurement Technologies. JYZ is grateful for the For Ying-Tong Education Foundation (161096), China

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