On the importance of the Vg,maxVth parameter on LTPS TFT stressing behavior

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Abstract

In this work we point out the importance of the device parameter Vg,maxVth (the difference between the gate voltage at maximum transconductance and the threshold voltage obtained from linear extrapolation method) for LTPS TFTs under dc stress. The evolution of this parameter with stress time is monitored for the first time, along with the other typical device parameters (Vth, Gm,max, S) in order to further clarify the nature of the traps generated. In the first dc stress case considered, we observed very different S degradation of the two samples, but very similar Gm,max degradation, as well as similar Vg,maxVth evolution. Therefore, Gm,max evolution with stress time was found to be related more strongly to tail state generation, probed through Vg,maxVth, and not to midgap trap generation, probed through S. In the second case, no midgap state generation is observed, but only severe tail state generation. Hence, the nature of the created defects and the reason for the significant Gm,max reduction could only be probed through the observation of Vg,maxVth, a parameter not utilized until now. Finally, stressing both n- and p-channel devices, we are able to explain the much more intense Gm,max degradation observed for n-channel devices, associating it to the larger tail state generation in n-channel TFTs, also pointed by Vg,maxVth evolution with stress.

Introduction

Low temperature polycrystalline silicon thin film transistors (LTPS TFTs) are essential for large area electronics, VLSI technology and high performance flat panel display applications [1]. The primary advantage of poly-silicon TFTs over a:Si ones is their higher field-effect mobility and consequently higher drive current. With the recent poly-silicon crystallization process breakthroughs, using various excimer laser anneal (ELA) methods such as sequential lateral solidification (SLS), the TFT performance has substantially increased [2], [3], [4], [5], [6]. The several variations of the SLS technique allow the manufacturing of poly-silicon films with excellent intragrain quality and grains of different geometry. However, high TFT reliability should also be achieved for the fabrication of commercial products to be possible. Unfortunately, the degradation mechanisms of advanced LTPS TFTs have not yet been fully clarified, not allowing us to positively identify the origin and nature of the defects created through device stressing [7], [8]. Such information would be invaluable to the LTPS TFT industry, since it would provide input on the factors degrading the TFTs and therefore help optimize their performance through time and their operational lifetime.

In this work, we explore the potential of a newly introduced electrical characterization parameter, namely Vg,maxVth, proved to reflect the density of poly-silicon traps density particularly near the edge of the band gap [9], also known as tail states, as a means to distinguish the defects created by the stress. This way we suggest for the first time the importance of using the parameter Vg,maxVth for stressing experiments and propose its use along with the ones already monitored during stress (Vth, S, Gm,max) in order to specify the nature and origin of the created defects.

Section snippets

Experimental

The TFTs studied were fabricated in 50 nm thick poly-silicon films, formed by two different SLS ELA crystallization techniques: M × N [10], [11] and location control crystallization [12], with each one yielding a different grain geometry and poly-Si microstructural characteristics. For the M × N technique, in particular, two variations were examined: M × N#8 yielding larger domain sizes and “advanced” M × N (M × Nadv) yielding smaller domain sizes. The above crystallization techniques were used

Results and discussion

The first crystallization technology studied was the M × N technique, applying Vg,stress = 5 V, Vd,stress = 10 V for the M × N#8 variation and Vg,stress = 4 V, Vd,stress = 8 V for the M × Nadv variation, since these devices proved to be more sensitive. The fact that the M × Nadv sample is more sensitive to stress could be attributed to the smaller crystal domain sizes obtained from this procedure. Smaller domain sizes result in more protrusions of the poly-silicon film in the gate oxide, therefore more points of

Conclusions

Advanced SLS ELA TFT degradation behavior, under dc stress, is investigated, utilizing for the first time the evolution of the parameter Vg,maxVth in order to further clarify the nature of the traps generated. In the first dc stress case considered, the Gm,max degradation was found to be related more strongly to tail state generation, probed through Vg,maxVth, and not to midgap trap generation, probed through S. In the second case, no midgap state generation is observed, but only severe tail

Acknowledgement

The authors acknowledge financial support through the research project PENED 3ED550, administered by the Greek General Secretariat for Research and Technology.

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