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Improved Gettering Efficiency of Ni from Nickel-Mediated Crystallization Silicon Using Phosphorus-Doped Amorphous Silicon

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Improved Gettering Efficiency of Ni from Nickel-Mediated

Crystallization Silicon Using Phosphorus-Doped

Amorphous Silicon

BAU-MING WANG1 and YEWCHUNG SERMON WU1,2

1.—Department of Materials Science and Engineering, National Chiao Tung University, 1001 Ta-Hsueh Road, Hsinchu 300, Taiwan, ROC.2.—e-mail: [email protected]

Ni-metal-induced lateral crystallization (NILC) has been utilized to fabricate polycrystalline silicon thin-film transistors. However, the NILC process often leads to Ni and NiSi2 precipitates being trapped. In this study, two kinds of films were used as gettering layers: (1) amorphous Si and (2) phosphorus-doped amorphous Si. After annealing at 550°C for 12 h, it was found that phosphorous dopant did improve the gettering efficiency of amorphous Si. Key words: Ni gettering, phosphorus dopant, chemical oxide (chem-SiO2)

INTRODUCTION

Low-temperature polycrystalline silicon (LTPS) thin-film transistors (TFTs) have attracted consid-erable interest for their use in active-matrix liquid-crystal displays (AMLCDs) because they exhibit good electrical properties and can be integrated in peripheral circuits on inexpensive glass substrates.1 Since polycrystalline silicon (poly-Si) TFTs require glass substrates, intensive studies have been car-ried out to lower the crystallization temperature of amorphous silicon (a-Si) films. Ni-metal-induced lateral crystallization (NILC) is one of these efforts. In NILC, Ni islands on the top of a-Si films are allowed to crystallize at a temperature below 600°C. The poly-Si formed under the Ni islands is called Ni-metal-induced crystallization (NIC), whereas the poly-Si formed outside the metal layer is called NILC. Unfortunately, the NILC poly-Si grain boundaries trap Ni and NiSi2 precipitates, which increase the leakage current and shift the threshold voltage.2–6 Therefore, Ni contamination inside the NILC poly-Si film should be reduced. Several metal gettering methods have been employed to reduce the amount of undesired metallic impurities in Si.7–11These gettering methods are complicated and require high process temperatures.

In previous studies, we have proposed several methods for reducing Ni concentration inside the NILC film. They involve using a-Si/silicon-nitride films, a-Si-coated Si wafer, and contact holes covered with a-Si film.12–14During the gettering process, Ni atoms were diffused from the NILC film to the a-Si layer due to the concentration gradient. However, when the system reached equilibrium, no more Ni diffused into the gettering layer. At this point, the Ni concentration in the a-Si layer was the same as that in NILC. In this study, phosphorus-doped a-Si (P-a-Si) film and chemical SiO2(chem-SiO2) layer were used as gettering layers. The effect of phosphorus dopant on the Ni-gettering efficiency was investigated.

EXPERIMENTAL

Three kinds of poly-Si films were investigated in this study. One was a poly-Si film fabricated by traditional NILC method without the gettering process (referred to as NoGET), and the others were poly-Si films fabricated by the same NILC method with different Ni-gettering layers (referred to as ASiGET and PSiGET). The NILC fabrication pro-cess began with capping 4-inch Si (100) wafers with 500-nm-thick wet thermal oxide. Then, silane-based 100-nm-thick a-Si films were deposited using low-pressure chemical vapor deposition (LPCVD) at 550°C in N2ambient. The photoresist was patterned to form desired Ni lines, and a 5-nm-thick Ni film was deposited on the a-Si.

(Received October 27, 2008; accepted March 2, 2009; published online March 28, 2009)

Journal of ELECTRONIC MATERIALS, Vol. 38, No. 6, 2009 Regular Issue Paper

DOI: 10.1007/s11664-009-0750-2 Ó2009 TMS

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To form NoGET poly-Si films, samples were annealed at 540°C for 24 h in N2, as shown in Fig.1a. The unreacted Ni was then removed by a mixed solution of H2SO4 and H2O2 for 20 min. Finally, poly-Si films were dipped into 1% diluted hydrogen fluoride (DHF) solution to remove the annealing surface oxide, as illustrated in Fig. 1b.

As for the ASiGET poly-Si film, a NoGET poly-Si film was dipped into a mixed solution of H2SO4and H2O2 for 10 min to form a chem-SiO2 layer on the top of NILC poly-Si. A 100-nm-thick a-Si film was then deposited on the chem-SiO2 layer using LPCVD at 550°C for 1 h in N2ambient, as shown in Fig.1c. The top a-Si film served as the Ni-gettering layer. To examine the quality of chem-SiO2, after the chem-SiO2 layer was formed, platinum was deposited on top of the chem-SiO2for image contrast in transmission electron microscopy (TEM) sample preparation. As shown in Fig.2, the oxide layer was only about 5 nm thick. This chemical oxide layer was used as an etching stop layer in the 5% tetra-methylammonium hydroxide (TMAH) etching solu-tion. Moreover, this thin oxide layer also served as a diffusion interlayer during the Ni-gettering process. Ni atoms needed to diffuse from the NILC-Si through the thin chem-SiO2 into the Ni-gettering layer.

As for the PSiGET poly-Si film, phosphorous ions were implanted into a-Si to form a P-a-Si film, as shown in Fig.1c. The projection range of ions was set at the middle of the a-Si film. The dosage of phosphorous ions and the ion-accelerating energy were 1 9 1016cm 2and 35 keV, respectively.

Samples undergoing Ni-gettering were then an-nealed at 550°C for 12 h in N2ambient with the goal of removing the unwanted Ni metal inside the NILC-Si. Following the annealing process, the top Ni-gettering films were removed using 5% TMAH for 2 min at 55°C, and the chem-SiO2 layers were

removed using 1% DHF solution, as shown in Fig.1d. To study the effect of gettering on the sur-face roughness of NILC poly-Si, the NILC sursur-faces were measured using atomic force microscopy (AFM). It was found that the metal gettering did not change the surface roughness greatly: the root-mean-square (rms) roughness of ASiGET (0.65 nm) and PSiGET (0.69 nm) were almost the same as that of NoGET (0.64 nm).

For the purpose of comparison, the NoGET poly-Si film was also subjected to an extended heat treatment at 550°C for 12 h in N2ambient.

RESULTS AND DISCUSSION

The NoGET film was composed of NILC poly-Si grains.12 After the formation of gettering layers and the gettering process, the Ni-gettering layers Fig. 1. Schematic illustration of the Ni-gettering process: (a) fabrication of NILC poly-Si, (b) removal of unreacted Ni, (c) capped with a chem-SiO2layer and a gettering layer (a-Si or P-a-Si), and (d) removal of the gettering layer and chem-SiO2layer.

Fig. 2. TEM image of the cross-section of the NoGET film caped with5-nm-thick chem-SiO2layer. Platinum film deposited on the

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(a-Si and P-a-Si) were examined by optical micro-scopy (OM) to investigate the gettering efficiency. The results are shown in Fig.3. In the figure, the pink region was a-Si and the green region was needle-like NILC poly-Si, which has been verified using scanning electron microscopy (SEM) and TEM.12The pale-green region in Fig. 3b was NILC poly-Si on NoGET film underneath the chem-SiO2 layer. This means that, during the gettering pro-cess, Ni atoms diffused from the NoGET film through chem-SiO2into the Ni-gettering layer due to the concentration gradient. When Ni atoms reached the gettering film, enough Ni metal would be accumulated to form NiSi2 precipitates, and a-Si would then be transformed into needle-like poly-Si grains by the NILC mechanism. NILC poly-poly-Si grains first appeared right above the top of the NIC area, and then extended to the surrounding areas. This is because the Ni concentration above the NIC area was higher than that in other areas of the gettering film. Therefore, we can still see the NIC strip patterns.

Figure3 also shows that the length of the NILC poly-Si growth on the P-a-Si gettering layer was 13 lm, which was much shorter than that (60 lm) on the a-Si gettering layer. Since the NILC grains were induced by indiffusion of Ni atoms, it seemed that phosphorous dopant did not improve the get-tering efficiency of a-Si.

In addition to the gettering layer, the gettering efficiencies of ASiGET and PSiGET poly-Si films were also investigated. After the gettering layer and chem-SiO2were removed, the samples were dipped into a silicide-etching solution (HNO3:NH4F:H2O = 4:1:50). As shown in Fig.4a and b, numerous holes were observed at the boundaries where two NILC poly-Si fronts intersected (NILC/NILC boundaries). These holes were residues of the Ni silicide that had been etched away by the silicide-etching solution. These silicide-etching holes seen in Fig.4b were quite sensitive to the reduction of Ni residue in the NILC poly-Si, and were therefore ideal for eluci-dating the ‘‘Ni gettering’’ phenomenon observed. After the gettering process, fewer and smaller

silicide-etching holes were found at the NILC/NILC boundaries of ASiGET, as shown in Fig.4c. Fur-thermore, there were almost no silicide-etching holes observed at the NILC/NILC boundaries of PSiGET, as shown in Fig.4d. These results indicate that phosphorous dopant did improve the gettering efficiency of a-Si, which was different from our OM observation of gettering layers (Fig.3).

Fig. 3. OM images of gettering layers after annealing at 550°C for 12 h: (a) a-Si and (b) p-a-Si.

Fig. 4. Schematic illustration of (a) silicide-etching holes at NILC/ NILC boundaries, and SEM images of etching holes of (b) NoGET, (c) ASiGET, and (d) PSiGET.

Improved Gettering Efficiency of Ni from Nickel-Mediated Crystallization Silicon Using Phosphorus-Doped Amorphous Silicon

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Secondary-ion mass spectroscopy (SIMS) was employed to clarify the Ni concentration in PSiGET and ASiGET. Unfortunately, the Ni concentration in the NILC poly-Si is hard to measure since the SIMS sputtering area (125 lm 9 125 lm2) is much larger than that in the NILC poly-Si area. There-fore, we used NIC poly-Si to demonstrate that phosphorus dopant did improve the gettering effi-ciency of a-Si. The fabrication process of NIC poly-Si is shown in Fig. 5. Silane-based 100-nm-thick a-Si films were deposited using LPCVD at 550°C in N2 ambient, as shown in Fig.5a. A 5-nm-thick Ni film was then deposited on the a-Si, and subsequently annealed at 540°C for 24 h to form NIC poly-Si. The unreacted Ni was then removed by a mixed solution of H2SO4and H2O2for 20 min, as shown in Fig.5b. The poly-Si film was dipped into a mixed solution of H2SO4and H2O2to form a chem-SiO2layer. A 100-nm-thick a-Si film was then deposited on the chem-SiO2 layer using LPCVD at 550°C for 1 h in N2 ambient to form the a-Si gettering layer, as shown in Fig. 5c. Phosphorous ions were implanted into a-Si to form the P-a-Si gettering layer. Samples were then annealed at 550°C for 12 h in N2ambient. Even though the Ni concentration in NIC poly-Si was much higher than that in NILC poly-Si, we can still have a preliminary understanding of the get-tering efficiency of a-Si films. Figure6 shows that

the Ni concentration of NIC poly-Si was reduced after the Ni-gettering process. As can be seen, the Ni concentration in NIC poly-Si with the a-Si get-tering layer was relatively higher than that with the P-a-Si gettering layer. Moreover, P-a-Si traps many more Ni atoms than does a-Si in the gettering layer. These results indicate that phosphorous dopant did improve the gettering efficiency of a-Si. Phosphorus implant and implant damage trap Ni and slow down the NILC rate on the gettering layer.15As a result, the length of the NILC poly-Si growth on P-a-Si (Fig.3) was much shorter than that on a-Si, but the silicide-etching holes (Fig.4) of PSiGET were fewer and smaller than those of ASiGET.

Figure6also shows that the middle of the P-a-Si layer had a higher Ni concentration than other parts of the layer. This concentration distribution of Ni was similar to that of phosphorous atoms since the projection range of phosphorous ions was set at the middle of the a-Si film. This result also indicates that phosphorus did trap Ni atoms.

In the gettering process, when more Ni atoms diffused into the gettering layer, more a-Si would be transformed into poly-Si by the NILC mechanism. The gettering efficiency increased with the growth of NILC poly-Si grains. However, when the system reached equilibrium, no more Ni could diffuse into the gettering layer. At this point, the Ni concen-tration in the a-Si gettering layer will be the same as that in ASiGET. However, the Ni concentration in the P-a-Si gettering layer will be higher than that in PSiGET since phosphorus implant traps Ni atoms. In other words, the gettering efficiency of a-Si is indeed improved by phosphorous dopant.

CONCLUSION

Two kinds of films were employed to investigate the effect of phosphorus dopant on the gettering efficiency of a-Si. To form the ASiGET and PSiGET, Fig. 5. Schematic illustration of the gettering process of the NIC

poly-Si: (a) fabrication of the NIC poly-Si, (b) removal of unreacted Ni, and (c) capped with a chem-SiO2layer and a gettering layer (a-Si

or P-a-Si).

Fig. 6. SIMS depth profiles of the NIC poly-Si films. RPis the

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a5-nm-thick porous chem-SiO2layer was capped on the top of the NoGET film, and then either a a-Si or a P-a-Si film was deposited on the top of the chem-SiO2 film. The chem-SiO2 layer was used as an etching stop layer, while the Si film served as a gettering layer. It was found that the Ni concen-tration in the NoGET film was greatly reduced after gettering at 550°C for 12 h. Compared with those on the NoGET film, the silicide-etching holes found at the NILC/NILC boundaries of ASiGET were fewer and smaller, while almost no holes were observed at the boundaries of PSiGET. This is because the concentration gradient acts as a driving force for transport of Ni from the NoGET poly-Si through the chem-SiO2layer to the gettering layer.

It was also found that the gettering layer was transformed into poly-Si by the NILC mechanism. The NILC fraction in the gettering layer increased with an increase in annealing time and tempera-ture, as expected from the kinetic nature of the diffusion process. Moreover, the length of NILC poly-Si growth on the P-a-Si gettering layer was much shorter than that on the a-Si gettering layer. This is because phosphorus implant and implant damage trap Ni and slow down the NILC rate on the gettering layer. In other words, the gettering effi-ciency of a-Si is indeed improved by the doping of phosphorous.

ACKNOWLEDGEMENTS

This project was funded by Sino American Silicon Products Incorporation and the National Science Council of the Republic of China under Grant No. 95-2221-E009-087-MY3. Technical support from the

National Nano Device Laboratory, Center for Nano Science and Technology, and the Nano Facility Center of the National Chiao Tung University are also acknowledged.

REFERENCES

1. M. Stewart, R.S. Howell, L. Pires, and M.K. Hatalis, IEEE Trans. Electron. Dev. 48, 845 (2001). doi:10.1109/16.918227. 2. P.J. van der Zaag, M.A. Verheijen, S.Y. Yoon, and N.D. Young, Appl. Phys. Lett. 81, 3404 (2002). doi:10.1063/1.151 7406.

3. G.A. Bhat, Z. Jin, H.S. Kwok, and M. Wong, IEEE Electron. Dev. Lett. 20, 97 (1999). doi:10.1109/55.740664.

4. Z. Jin, K. Moulding, H.S. Kowk, and M. Wong, IEEE Electron. Dev. Lett. 20, 167 (1999). doi:10.1109/55.753755. 5. G.A. Bhat, H.S. Kwok, and M. Wong, Solid-State Electron.

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Improved Gettering Efficiency of Ni from Nickel-Mediated Crystallization Silicon Using Phosphorus-Doped Amorphous Silicon

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Fig. 2. TEM image of the cross-section of the NoGET film caped with 5-nm-thick chem-SiO 2 layer
Fig. 3. OM images of gettering layers after annealing at 550°C for 12 h: (a) a-Si and (b) p-a-Si.
Fig. 6. SIMS depth profiles of the NIC poly-Si films. R P is the pro-

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