• 沒有找到結果。

-0.5 0.0 0.5

0.2 0.4

Defocus [痠]

0.5 0.4 0.3 0.2 0.1 0.0

Cross Section: X Parallel, Y = 0.000

(b)

Fig 4-16 aerial image for (a) Atten-NPS =25% (b) equal binary mask (dark line=67nm, pitch=140nm)

SOLID-C ®

Average Sidewall Angle (CS) [財 85.000-92.000 Thickness Loss (CS) [%]

inf.-10.000

0.8087 7.00%

best Defocus [痠]: -0.196, best Dose [mJ/cm^2]: 56.668

(a)

Average Sidewall Angle (CS) [財 85.000-92.000 Thickness Loss (CS) [%]

inf.-10.000

0.8698 7.00%

best Defocus [痠]: -0.165, best Dose [mJ/cm^2]: 51.616

(b)

Fig 4-17 process window for (a) Atten-NPS =25% (b) equal binary mask (dark line=67nm, pitch=140nm

Chapter 5

Conclusion

5-1 Conclusion

It is found that the dark line between a bright lines pair can decrease the iso-focal intensity so to gain a better line pattern. But because in the pair bright lines mask undesirable dark line is formed between adjacent pairs, so it needs double exposure to erase the undesirable dark line.

In order to decrease the time of exposure step, so we change the dark lines between the pair of bright lines with non-phase shifting mask to increase the aerial image intensity of the place. So the original aerial image intensity which is low and can not be resolved will become high enough and can resolve.

Finally, we change the non-phase-shifting mask to a set of line patterns. The line patterns have small width that is below the resolution limit so will not be resolved and the patterns have the similar transmission behavior as non-phase-shifting mask so can be the replaced mask of non-phase-shifting mask.

The schemes of the three methods are shown in figure 5-1. And the simulated results are shown in figure 5-2. From the simulation results can improve our conclusion of above.

Fig 5-1 scheme of the three methods

SOLID-C ®

Cross Section: X Parallel, Y = 0.000

SOLID-C ® Average Sidewall Angle (CS) [財 85.000-92.000

Cross Section: X Parallel, Y = 0.000

SOLID-C ® Average Sidewall Angle (CS) [財 85.000-92.000 Thickness Loss (CS) [%]

inf.-10.000

0.8087 7.00%

best Defocus [痠]: -0.196, best Dose [mJ/cm^2]: 56.668

image=90nm

Cross Section: X Parallel, Y = 0.000

SOLID-C ® Average Sidewall Angle (CS) [財 85.000-92.000

(c) binary line equal to Att-NPS

Fig 5-2 process window and aerial image for three methods

Reference

[1] Semiconductor Industry Association, International Technology Roadmap for Semiconductors: 1999. Austin, TX: SEMATECH, 1999.

[2] Tsuneo Terasawa, “Subwavelength Lithography (PSM,OPC)”, IEEE, pp.295-300, 2000

[3] H. Fukuda, A. Imai, T. Terasawa, and S. Okazaki, “New Approach to Resolution Limit and advanced Image Formation Techniques in Optical Lithograpy”,IEEE. Truns.

Electron Devices, Vol. ED-38, No. 1, pp.67-15, 1991.

[4] R. Bunaw and H. Fukuda, “Printing Isolated Feature with kl=0.2 Using Multiole-Pupil Exposure”, Jpn. J. Appl. Phys., Vol. 35, No. 12B, pp. 6400-6403, 1996.

[5] J. Finders, A.M. Mulders, J. Krist, D. Flagello, P. Luehrmann, et al.,”Sub-0.25 micron lithography applying illumination pupil filtering (quadrupole) on a DUV step

& repeat system.”

[6] H. Fukuda, A. Imai, and S. Okazaki, “Phase-Shifting mask and FLEX method for Advanced Photolithography”, Proc. SPIE, Vol. 1264, pp. 14-25, 1990.

[7] HIROSHI FUKUDA, NOR1O HASEGAWA, et, “A New Method for Enhancing Focus Latitude in Optical Lithography: FLEX”, IEEE ELECTRON DEVICE

LETTERS, VOL. EDL-8, NO. 4, APRIL 1987

[8] Hiroshi Fukuda, Tsuneo Terasawa, and Shinji Okazaki, “Spatial filtering for depth of focus and resolution enhancement in optical lithography”, American Vacuum Socissty, pp. 3113-3116, 1991

[9] M. Noguchi, M. Muraki, Y. Iwasaki, and A. Suzuki, “Subhalf Micron Lithography System with Phase Shifting Effect”, Proc. SPIE symp. Microlithogruphy, Vol. 1674, pp. 92-104, Mar. 1992.

[10] K. Kamon, T. Miyamoto, Y. Myoi, H. Nagata, M. Tanaka, and K. Horie,

“Pholithography system using annular illumination,” Jpn. J. Appl. Phys., pt. 1, vol. 30, p. 3012, 1991.

[11] B.J. Lin, Linnovation, Inc.Off-axis illumination -- Working principles and comparison

with alternating phase-shifting masks SPIE Vol. 1927 Optical/Laser Microlithography VI (1993) / 89

[12] Jan van Schoot, Jo Finders, Koen van Ingen Schenau, Michel Klaassen and

Corine Buijk “THE MASK ERROR FACTOR: CAUSES AND IMPLICATIONS FOR PROCESS LATITUDE”SPIE Vol. 3679 p250

[13] B.J. Lin, Linnovation, “Off-axis illumination -- Working principles and comparison

with alternating phase-shifting masks”, SPIE, Vol. 1927, pp.89-100, 1993

[14] M. D. Levenson, N. S. Viswanathan, and R. A. Sympson, “Improving Resolution in photolithography with a Phase-Shifting Mask”, IEEE, Truns. Electron Devices, Vol.

ED-29, No. 12, pp. 1828- 1836, 1982.

[15] T. Terasawa, N. Hasegawa, T. Tanaka, S. Katagiri, and T. Kurosaki, “Improved resolution of an i-line stepper using a phase-shifting mask”, J. Vuc. Sci. Techno!., Vol.

B8, No.6, pp. 1300-1308, Nov/Dec. 1990.

[16] A. Nitayama, T. Sato, K. Hashimoto, E Shigematsu, and M Nakase, “New Phase Shifting Mask with Self-aligned Phase Shifter for Quarter Micron Photolithography”, Technicul Dig., pp.57-60, Dec. 1989.

[17] T. Terasawa, N. Hasegawa, H. Fukuda, and S. Katagiri, “Imaging characteristics of Multi-Phase-Shifting and Halftone phase Shifting Masks”, Jpn.J. Appl. Phys., Vol.

30, No. 11, pp. 2991-2997, 1991.

[18] H.-Y. Liu, L. Karklin, Y.-T. Wang, and Y.C. Pati, “The application of

phase-shifting masks to 140 nm gate patterning (II): Mask tolerances,” Proc. SPIE, vol. 3334, p. 2, 1998.

[19] H.-Y. Liu, L. Karklin, Y.-T. Wang, and Y. C. Pati, “The application of alternating phase-shifting masks to 140 nm gate patterning: Line width control improvements and design optimization,” in Proc. SPIE, vol. 3236.,1997

[20] B. J. Lin, “The attenuated phase-shifting mask,” Solid State Technol., vol. 35, pp.

43–47, January 1992.

[21] B.J. Lin, “Phase-Shift ing Masks Gain an Edge”, Circuits & Devices, pp.28-35, 1993

[22] K. Toh, G. Dao, R. Singh, and H. Gaw, “Chromeless phase-shifted masks: A new approach to phase-shifting masks,” in Proc. SPIE, vol. 1496, pp. 27–53, 1990

[23] J. F. Chen, J. Petersen, R Socha, T Laidig, K. Wampler, K. Nakagawa, G.

Hughes, S. MacDonald, and W. Ng, “Binary halftone chromeless PSM technology for λ/4 optical lithography”, Proc. SPIE 4346, pp.515-533 , 2001.

[24] C. Hsu, R. Chu, J. F. Chen, D. J. Van Den Broeke, X. Shi, S. D. Hsu, and T.

Wang, “Patterning half-wavelength DRAM cell using Chromeless Phase Lithography

(CPL)”, Proc. SPIE 4691, pp.76-88, 2002

[25] Jan van Schoot, Jo Finders, Koen van Ingen Schenau, Michel Klaassen and Corine Buijk, “THE MASK ERROR FACTOR: CAUSES AND IMPLICATIONS FOR PROCESS LATITUDE”, SPIE , Vol. 3679, pp.250-260, 1999

[26] Richard Rogoff, Guy Davies, Jan Mulkens, Jos de Kierk, Peter van Oorschot,

“PHOTOLITHOGRAPHY USING THE AERIALTM ILLUMINATOR IN A VARIABLE NA WAFER STEPPER”, SPIE, Vol. 2726, pp.54-70,

[27] Nakao, K. Narimatsu, T. Miyagi, S. Ogawa, N. Tamada, A. Nakae, A. Tokui, K.

Tsujita, I. Arimoto, W. Wakamiya, "Innovative Imaging ofUltra-fine Line without Using Any Strong RET", Proc. SPIE, 4346, 503 (2001).

[28] M. Born and E. Wolf, Principles of Optics, 6th ed.

[29] J. A. Torres, “Contrast analysis and optimization for resolution enhancement technique” 2003 Society of Photo-Optical Instrumentation Engineers

[30] M. Sanchez, W. Hinsberg, F. Houle, J. Hoffnagle, H. Ito, and C. Nguyen, “Aerial image contrast using interferometric lithography: Effect on line-edge roughness,” in Proc. SPIE, W. Conley, Ed., 1999, vol. 3678, pp. 160–171.

[31] J. Shin, G. Han, Y. Ma, K. Moloni, F. Cerrina, "Resist Lie Edge Roughness and Aerial Image Contrast", J. Vac. Sci. Technol. B, 19(6), 2890 (2001).

[32] B. G. Kim, S. W. Choi, W. S. Han, and J. M. Sohn, “Beneath the MEEF,” Solid State Technol., vol. 43, no. 8, p. 107, 2000.

[33] Chun-Kung Chen, Tsai-Sheng Gau, Jaw-Jung Shin, Ru-Gun Liu, Shinn-Sheng Yu, Anthony Yen and Burn J. Lin, “Mask Error Tensor can Causality of Mask Error Enhancement for Low-k1 Imaging: Theory and Experiments”, TSMC corporation [34] J. van Schoot, J. Finders, and C. Bujik, “The mask error factor: Causes and implications for process latitude,” Proc. SPIE, vol. 3679, pp. 250–260.

[35] Chris A.Mack, “Resolution and Depth of Focus in Optical Lithography”, SPIE, Vol.3183, pp.14-27

[36] D.Fuard, P.Schiavone and M.Besacier “ Validity of the diffused aerial image model: an assessment based on multiple test cases”, Proc of SPIE, vol.5040 p.1536, (2003)

[37] J.Van Wingerden et al. “ Lithographic process optimisation using process capability analysis”, Proc of SPIE, vol.5040 p.882-893, (2003)

[38] T. Terasawa, N. Hasegawa, "Theoretical Calculation of Mask Error Enhancement Factor for Periodic Pattern Imaging", Jpn. J. Appl. Phys., 39, 6786 (2000).

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