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IMPROVEMENT OF POLYSILICON OXIDE CHARACTERISTICS BY FLUORINE INCORPORATION

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IEEE ELECTRON DEVICE LEITERS, VOL. 15, NO. 5, MAY 1994 181

Improvement

of

Poly silicon Oxide

Characteristics by

Fluorine Incorporation

Horng Nan Chern, Chung

Abstract-The effect of fluorine on the polysilicon oxide (poly- oxide) characteristics is investigated. It is found that the polyoxide leakage current and breakdown strength are improved as fluorine is incorporated into the oxide film. Experimental results show

that the improvement is believed to be due to the oxide stress relaxation rather than the change of the polyoxiddpolysilicon interface texture.

I. INTRODUCTION

N order to obtain good data retention characteristics for

I

non-volatile memory, the inter-plysilicon oxides with a low conductivity and a high breakdown field are pursued [l]. It had been reported that the breakdown strength of the polyoxide is mainly determined by the polysilicodpolyoxide interface roughness [2,3]. Fluorine had been investigated to be

applied to single crystal Si (c-Si) metal-oxide-semiconductor (MOS) device to increase the device hot-carrier immunity and irradiation hardness [4]. These reliability improvements were suspected to be due to the strain relaxation of the interface. Recently, it had been experimentally demonstrated that the c-Si oxide grown in NF3 ambient exhibited a smaller stress than those grown in dry 02[ 5 ] . In this letter, we report that the introduction of fluorine into polyoxide reduces its leakage current and increases its breakdown strength.

11. EXPERIMENT

A polysilicon film of 3000 \AA thickness was deposited

at625^{ \circ}C by a low-pressure chemical vapor deposition (LPCVD) system on p-type silicon substrate on which a 5000)

8,

thick thermal oxide was grown at 1050°C in wet 0 2 . The

polysilicon was implanted with 5 x 1015 arsenickm' at 120 keV and then annealed at 850" C for 60 min in an NZ gas. After defining the polysilicon island, a 270

8,

gate oxide was grown at 850" C in a dry 0 2 ambient. Then an LPCVD amorphous silicon of 800

8,

thickness was deposited at 550°C.

After defining the top-gate pattern, a 200

8,

pad oxide was grown at 85OOC in dry 0 2 on the amorphous silicon and then implanted with 2 x 1015 phosphoruskm' at 40 keV. The dopant was annealed at 850" C for 60 min in an NZ gas. Fluorine ions with doses of 1 x 1013, 1 x 1 x 1015 and 3 x 1015 cm-2 were implanted at 25 keV through the pad

Manuscript received November 3, 1993; revised February 23, 1994. This research was supported by the National Science Council of R.O.C. through the contract of NSC-82-0404-EO09- 190.

The authors are with the Department of Electronics Engineering and Institute of Electronics, National Chiao Tung University, Hsinchu, Taiwan, R.O.C.

IEEE Log Number 9401 148.

Len Lee,

and

Tan

Fu Lei

10' I I I

Top- Poly. Bottom-

polysilicon oxide Poiysilicon

0 6 0 0 1200 1800 2400

Depth

(A)

Fig. 1.

cmP2, 1 x 10l4 cm-2, 1 x lOI5 cmP2, 3 x 1015

implantation. The post-implantation annealing temperature is 850' C. The SIMS profiles of fluorine for the devices implanted with 1 x l O I 3

and without fluorine

oxide and then annealed at 850" C for 60 min in a NZ gas. For the control samples, no fluorine was implanted, but they were also subjected to the same high temperature annealing as fluorine-implanted samples. All devices were covered with a 2000 8, plasma-enhanced chemical vapor deposition (PECVD) Si02 for passivation. Contact holes were opened, and A1 were deposited and the pattern. Finally, all devices were sintering at 350" C for 35 min in N2 gas. The I-V characteristics of the polyoxides were measured by HP 4145 semiconductor parameter analyzer.

111. RESULTS AND DISCUSSIONS

The SIMS profiles of fluorine for the devices implanted with 0 , l x 1 x 1 x and 3 x 1015 F+/cm2 followed by annealing at 850" C in an Nz ambient are shown in Fig. 1. It is seen that fluorine accumulated within the polyoxide and the higher the fluorine dose, the higher the fluorine peak value. There are also some amount of fluorine existing within the polysilicons. Fig. 2(a) and (b) shows the J-E characteristics of the polyoxides implanted with different doses of fluorine for the positive top-gate bias (electron injection from the bottom- gate) and the negative top-gate bias (electron injection from the top-gate), respectively. It is seen that all the fluorine- implanted polyoxides exhibit a smaller leakage current and a higher breakdown strength than the non-implanted polyoxide. This result is in contrast to that of previous reports on the c-Si Si0-{2}, i.e., fluorine did not affect or even degrade the oxide breakdown strength and its leakage current [6], [ 7 ] . In this experiment, it is found that the optimum dose of fluorine to improve the polyoxide J-E characteristics is 1 x 1015 cm-2. Too much fluorine seems to cause degradation to polyoxide

(2)

182 1o-’Q

5-

o.21 , ’ I 1 1 0

1 .

ALL:.

I I.. . I - ” ” ’ ’ ’ ” ’ ” ” ’ ’ . ’

I

1 2 3 4 5 6 7 8 Electric Field E (MV/crn) (b)

Fig. 2. The J-E characteristics of the polyoxides implanted with different doses of fluorine for (a) positive top-gate bias (electron injection from the bottom gate), and (b) negative top-gate bias (electron injection from top gate).

characteristics. In Fig. 2, the less tunneling leakage current when top-gate is positively biased is attribute that the bottom- polysilicodpolyoxide interface has a smoother morphology [2]. Fig. 3 shows the effective barrier height extracted from Fowler-Nordheim plots of these samples at positive top-gate bias. It is seen that the effective barrier heights were almost the same for these samples. Since the barrier height value is very sensitive to the interface texture structure [8], this implied that the fluorine-induced improvement of polyoxide characteristics was not caused by the change of the polysilicodpolyoxide interface texture. We would then suspected that the improve- ment of the polyoxide property is caused by the oxide stress relaxation due to the incorporation of fluorine. When fluorine was implanted into the top polysilicon and then driven in, it diffused into the polyoxide as revealed in Fig. 1. Originally, due to the high stress in the polyoxide [9], there are many strained bonds within the oxide, especially at regions nearby grain boundaries. These strained bonds are easy to be broken by high energy electrons to cause breakdown when a field is applied to the oxide. After the fluorination, the fluorine in the

IEEE ELECTRON DEVICE LETTERS, VOL. 15, NO. 5 , MAY 1994

E I I 4

1

o No F’ implantation 8 F’: 1x1013 cm-‘ 0 F+: 1x1014 cm-’ A F+: 1x1015 ~ m - ~ I I I I 2.0 2.5 1 0 . ~ 3.0 3.5 4.0 1 0 . ~ 1/E (cm/v)

Fig. 3. Fowler-Nordheim plots for the polyoxide leakage currents at positive top-gate bias. The insert shows the effective barrier heights for the polyoxide implanted with different fluorine doses.

oxide tends to break the strained bonds and releases the oxide film stress. Hence, the oxide breakdown strength is improved.

IV. SUMMARY

In summary, it is found that the incorporation of fluorine in the polyoxide reduced the oxide leakage current and increased the breakdown strength. This improvement is believed to be due to the oxide stress relaxation rather than the change of the polysilicordpolyoxide interface texture.

REFERENCES

[I] S. Mori, Y. Kaneko, N. Arai, Yoichi, H. Araki, K. Narita, E. Sakagemi, and K. Yoshikawa, “Reliability study of thin inter-poly dielectrics for non-volatile memory application,” in Proc. 28th IRPS, pp. 132-144,

1990.

[2] S. L. Wu, T. Y. Lin, C. L. Lee, and T. F. Lei, “Electrical characteristics of textured polysilicon oxide prepared by low-temperature wafer loading and Nz preannealing process,” IEEE Electron Device Lett., vol. 14, pp. 113-1 14, 1993.

[3] M. Hendriks and C. Mavero, “Phosphorus doped polysilicon for double poly structure,” J. Electrochem. Soc., vol. 138, pp. 1466-1474, 1991.

[4] T. P. Ma, “Metal-oxide-semiconductor gate oxide reliability and the role of fluorine,” J. Vac. Sci. Technol. A , vol. 10, no. 4, pp. 705-712, 1992. [5] D. Kouvatsos, J. G. Huang, and R. J. Jaccodine, “Fluorine-enhanced oxidation of silicon: effects of fluorine on oxide stress and growth kinetics,” J. Electronchem. Soc., vol. 138, pp. 1752-1755, 1991. [6] P. J. Wright, M. Wong, and K. C. Saraswat, “The effect of fluorine on

gate dielectric properties,” in IEDM Tech. Dig., 1987, pp. 574-577. [7] Y. Shioya, S. Kawamura, I. Kobayashi, M. Maeda, and K. Yanagida,

“Effect of fluorine in chemical-vapor-deposited tungsten silicide film on electrical breakdown of Si02 film,” J. Appl. Phys., vol. 61, pp. [8] K. Shinada, S. Mori, and Y. Mikata, “Reduction in polysilicon oxide leakage current by annealing prior to oxidation,” J. Electronchem. Soc., [9] A. Shintani and H. Nakashima, “Anomalous stress in thermal oxide of

polycrystalline Si,” Appl. Phys. Lett., vol. 36, pp. 983-985, 1980. 5102-5109, 1987.

數據

Fig.  3.  Fowler-Nordheim plots for the polyoxide leakage currents at positive  top-gate bias

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