Ion-beam lithography is the practice of scanning a focused beam of ions in a patterned fashion across a surface in order to create very small structures such as integrated circuits or other nanostructures.[1]
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Lecture 61 (CHE 323) E-Beam Lithography, part 1
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Lecture - 23 Lithography - I
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Focused Ion-Beam Milling and Lifting of Sample for Transmission Electron Microscopy
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Ion-beam lithography has been found to be useful for transferring high-fidelity patterns on three-dimensional surfaces.[2]
Ion-beam lithography offers higher resolution patterning than UV, X-ray, or electron beam lithography because these heavier particles have more momentum. This gives the ion beam a smaller wavelength than even an e-beam and therefore almost no diffraction. The momentum also reduces scattering in the target and in any residual gas. There is also a reduced potential radiation effect to sensitive underlying structures compared to x-ray and e-beam lithography.[3]
Ion-beam lithography, or ion-projection lithography, is similar to Electron beam lithography, but uses much heavier charged particles, ions. In addition to diffraction being negligible, ions move in straighter paths than electrons do both through vacuum and through matter, so there seems be a potential for very high resolution. Secondary particles (electrons and atoms) have very short range, because of the lower speed of the ions. On the other hand, intense sources are more difficult to make and higher acceleration voltages are needed for a given range. Due to the higher energy loss rate, higher particle energy for a given range and the absence of significant space charge effects, shot noise will tend to be greater.
Fast-moving ions interact differently with matter than electrons do, and, owing to their higher momentum, their optical properties are different. They have much shorter range in matter and move straighter through it. At low energies, at the end of the range, they lose more of their energy to the atomic nuclei, rather than to the atoms, so that atoms are dislocated rather than ionized. If the ions don't defuse out of the resist, they dope it. The energy loss in matter follows a Bragg curve and has a smaller statistical spread. They are "stiffer" optically, they require larger fields or distances to focus or bend. The higher momentum resists space charge effects.
Collider particle accelerators have shown that it is possible to focus and steer high momentum charged particles with very great precision.
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References
- ^ F. Watt∗, A. A. Bettiol, J. A. Van Kan, E. J. Teo and M. B. H. Breese http://www.ciba.nus.edu.sg/publications/files/pbw/pbw2005_1.pdf Archived 2011-07-21 at the Wayback Machine "Ion Beam Lithography and Nanofabrication: a Review"], The Guardian, London, 17 December 2004. Retrieved on 2011-03-03.
- ^ Dhara Parikh, Barry Craver, Hatem N. Nounu, Fu-On Fong, and John C. Wolfe, "Nanoscale Pattern Definition on Nonplanar Surfaces Using Ion Beam Proximity Lithography and Conformal Plasma-Deposited Resist", Journal of Microelectromechanical Systems, vol. 17, no. 3, June 2008
- ^ Madou, Mark (2012). Fundamentals of Microfabrication and Nanotechnology volume 2. Boca Raton, Fl: CRC Press. p. 655. ISBN 978-1-4200-5519-1.
This page was last edited on 28 May 2024, at 09:17