New chemically amplified positive resist for electron beam lithography

Author(s):  
Kazuhiko Hashimoto
2002 ◽  
Author(s):  
Andrew R. Eckert ◽  
Richard J. Bojko ◽  
Harold Gentile ◽  
Robert Harris ◽  
Jay Jayashankar ◽  
...  

1996 ◽  
Vol 35 (Part 1, No. 12B) ◽  
pp. 6506-6510 ◽  
Author(s):  
Tetsuro Nakasugi ◽  
Hitoshi Tamura ◽  
Hiromi Niiyama ◽  
Satoshi Saito ◽  
Naoko Kihara ◽  
...  

Author(s):  
L. D. Jackel

Most production electron beam lithography systems can pattern minimum features a few tenths of a micron across. Linewidth in these systems is usually limited by the quality of the exposing beam and by electron scattering in the resist and substrate. By using a smaller spot along with exposure techniques that minimize scattering and its effects, laboratory e-beam lithography systems can now make features hundredths of a micron wide on standard substrate material. This talk will outline sane of these high- resolution e-beam lithography techniques.We first consider parameters of the exposure process that limit resolution in organic resists. For concreteness suppose that we have a “positive” resist in which exposing electrons break bonds in the resist molecules thus increasing the exposed resist's solubility in a developer. Ihe attainable resolution is obviously limited by the overall width of the exposing beam, but the spatial distribution of the beam intensity, the beam “profile” , also contributes to the resolution. Depending on the local electron dose, more or less resist bonds are broken resulting in slower or faster dissolution in the developer.


1997 ◽  
Author(s):  
Zheng Cui ◽  
R. A. Moody ◽  
Ian M. Loader ◽  
John G. Watson ◽  
Philip D. Prewett

2011 ◽  
Vol 497 ◽  
pp. 127-132 ◽  
Author(s):  
Hui Zhang ◽  
Takuro Tamura ◽  
You Yin ◽  
Sumio Hosaka

We have studied on theoretical electron energy deposition in thin resist layer on Si substrate for electron beam lithography. We made Monte Carlo simulation to calculate the energy distribution and to consider formation of nanometer sized pattern regarding electron energy, resist thickness and resist type. The energy distribution in 100 nm-thick resist on Si substrate were calculated for small pattern. The calculations show that 4 nm-wide pattern will be formed when resist thickness is less than 30 nm. Furthermore, a negative resist is more suitable than positive resist by the estimation of a shape of the energy distribution.


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