Characterization and control of laser plasma flux parameters for soft-x-ray projection lithography.

Laser plasmas are intrinsically an attractive soft-x-ray source for projection lithography. Compact, flexible, and small enough to be dedicated to a single installation, they offer an alternative to costly multi-installation synchrotron sources. For laser plasmas to provide ideal sources of soft x rays for projection lithography, their properties must be tuned to optimize several critical parameters. High x-ray conversion in the spectral band relevant to projection lithography is obviously required and has already received the attention of several studies. However, other features, such as the spectral content and direction of the x-ray emission, the plasma and particulate emission, the technology of the target, and efficient laser design, must also be optimized. No systematic study of all these features specifically for projection lithography has yet been made. It is our purpose to optimize these parameters in a coordinated approach, which leads to the design of a source that satisfies all the demanding requirements of an operating lithographic installation. We make an initial investigation of the plasma and particle emission of plasmas that have previously been shown to be good x-ray converters to the 13-nm band. The importance of the results reported may well force new approaches to the design of laser plasma soft-x-ray sources for projection lithography.

[1]  Stephen P. Vernon,et al.  High-performance multilayer mirrors for soft x-ray projection lithography , 1992, Optics & Photonics.

[2]  A. Hawryluk,et al.  Soft x‐ray projection lithography using an x‐ray reduction camera , 1988 .

[3]  D. Phillion,et al.  X-Ray Production Efficiency at 130 A from Laser-Produced Plasmas, , 1992 .

[4]  Henri Pepin,et al.  Laser plasma x‐ray sources for microlithography , 1988 .

[5]  R. Byer,et al.  Monolithic, unidirectional single-mode Nd:YAG ring laser. , 1985, Optics letters.

[6]  Martin Richardson,et al.  High-Resolution XUV Spectroscopy Using The OMEGA Laser , 1988, Optics & Photonics.

[7]  Brown,et al.  Laser-produced spectra and QED effects for Fe, Co, Cu, and Zn ions of Au, Pb, Bi, Th, and U. , 1986, Physical review letters.

[8]  John F. Evans,et al.  Summary Abstract: Characterization of AlN films produced by chemical vapor deposition using a novel metal azide precursor , 1988 .

[9]  James B. Murphy Electron storage rings as x-ray lithography sources: an overview , 1990, Advanced Lithography.

[10]  A. Rosenbluth,et al.  Reflecting Properties of X-Ray Multilayer Devices. , 1983 .

[11]  R. Fabbro,et al.  X‐ray sources for microlithography created by laser radiation at λ=0.26 μm , 1987 .

[12]  W. T. Silfvast,et al.  Tenth micron lithography with a 10 Hz 37.2 nm sodium laser , 1988 .

[13]  N. M. Ceglio,et al.  Soft-X-Ray Projection Lithography System Design, , 1992 .

[14]  Hideo Yoshihara,et al.  A plasma x‐ray source for x‐ray lithography , 1986 .

[15]  T. Tomimasu Industrial Applications of Synchrotron Radiation J, Matsui, Chairman Review of Japanese compact electron storage rings and their applications (invited) , 1989 .

[16]  F. Irons,et al.  The ion and velocity structure in a laser produced plasma , 1972 .

[17]  Natale M. Ceglio,et al.  Soft x-ray projection lithography system design and cost analysis , 1992, Optics & Photonics.

[18]  Brian E. Newnam,et al.  Extreme ultraviolet free-electron laser-based projection lithography systems , 1991 .

[19]  D. Kalantar,et al.  X-pinch soft x-ray source for microlithography , 1990, 1992 9th International Conference on High-Power Particle Beams.

[20]  J. M. Zeigler,et al.  Extreme ultraviolet resist and mirror characterization: Studies with a laser plasma source , 1990 .