Experimental results of the stochastic Coulomb interaction in ion projection lithography

Citation
Pwh. De Jager et al., Experimental results of the stochastic Coulomb interaction in ion projection lithography, J VAC SCI B, 17(6), 1999, pp. 3098-3106
Citations number
11
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B
ISSN journal
10711023 → ACNP
Volume
17
Issue
6
Year of publication
1999
Pages
3098 - 3106
Database
ISI
SICI code
1071-1023(199911/12)17:6<3098:EROTSC>2.0.ZU;2-L
Abstract
Throughput and resolution are connected in ion and electron projection lith ography (IPL and EPL) because of the space charge and Coulomb interaction b etween the particles in the beam. Due to the lack of experimental data it w as not possible Co estimate this effect accurately. Therefore an experiment setup has been developed which has the most significant parameters close t o planned IPL exposure tools. These parameters are the linear particle dens ity and the crossover shape and size. The stochastic Coulomb interaction bl ur, depending on the total beam current, has been measured in about 100 set tings of the beam current, beam energy, and crossover shape. The results sh ow that the stochastic Coulomb interaction blur scales to the power of 0.58 7+/-0.101 (1 sigma) of the Linear particle density in a system with a unifo rm crossover of 400 mu m. To decrease the current density in crossover IPL systems can have an aberrated crossover. In case of this type of crossover of 670 mu m the current dependency is 0.820+/-0.072 (1 sigma). With an aber rated crossover the stochastic Coulomb interaction is not uniform over the exposure held; it decreases towards the edges of the exposure field and pla teaus near its center. This reflects the shape of the crossover. The experi mental results can be used to make predictions of the allowable current in planned IPL exposure tools. The process development tool can have 1.00+/-0. 25 (1 sigma) mu A He+ ion current at 100 nm resolution. The allowable H+ io n current in the beta tool at 100 nm resolution is 9.09+/-2.14 (1 sigma) mu A and 3.69+/-0.81 (1 sigma) mu A at 50 nm. This corresponds to a throughpu t of 40.1+/-0.4 (1 sigma) wafers per hour (300 mm) at 100 nm and 26.1+/-2.0 (1 sigma) wafers per hour (300 nm) at 50 nm. (C) 1999 American Vacuum Soci ety. [S0734-211X(98)17606-6].