Please use this identifier to cite or link to this item: https://doi.org/10.1016/j.mee.2003.10.003
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dc.titleModified Rayleigh criterion for 90 nm lithography technologies and below
dc.contributor.authorChua, G.S.
dc.contributor.authorTay, C.J.
dc.contributor.authorQuan, C.
dc.contributor.authorLin, Q.
dc.date.accessioned2014-10-07T09:07:55Z
dc.date.available2014-10-07T09:07:55Z
dc.date.issued2004-02
dc.identifier.citationChua, G.S., Tay, C.J., Quan, C., Lin, Q. (2004-02). Modified Rayleigh criterion for 90 nm lithography technologies and below. Microelectronic Engineering 71 (2) : 139-149. ScholarBank@NUS Repository. https://doi.org/10.1016/j.mee.2003.10.003
dc.identifier.issn01679317
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/85430
dc.description.abstractIn this paper, we have systematically investigated the dependencies of k1 on illumination conditions such as coherence setting and opening angle in off-axis illumination scheme. As result, conventional Rayleigh's equations are not sufficient to address the effect of NA and coherence on DOF. Therefore, a new metric called coherency factor (σc) is proposed as a complementary new metric of the low k1 lithography. Coherency factor (σc) is defined as the ratio of areas of captured first-order and zero-order light. The theory is based on simple geometrical analysis of the diffraction orders in the pupil plane. Areas of different diffraction orders captured by the pupil are evaluated as a function of wavelength, numerical aperture and pitch. As corresponding to experimental results, higher σc value concurs to larger depth of focus. Extracting from Fraunhofer diffraction equation for a single slit and incorporating coherency factor σc, we have modified and extend the use of Rayleigh's equations for 90 nm processes and below. Results show that the extension of Rayleigh's equations is capable to optimize the depth of focus and map out the forbidden pitch locations for any design rules and illumination conditions. More importantly, it can complement the concept of objective lens pupil filling to provide the theoretical ground for illumination design in order to suppress the forbidden pitch phenomenon. © 2003 Elsevier B.V. All rights reserved.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1016/j.mee.2003.10.003
dc.sourceScopus
dc.subjectDepth of focus
dc.subjectDiffraction orders
dc.subjectDipole illumination
dc.subjectForbidden pitch
dc.subjectFraunhofer diffraction
dc.subjectLow k1 imaging
dc.subjectOff-axis illumination
dc.subjectRayleigh's equations
dc.typeArticle
dc.contributor.departmentMECHANICAL ENGINEERING
dc.description.doi10.1016/j.mee.2003.10.003
dc.description.sourcetitleMicroelectronic Engineering
dc.description.volume71
dc.description.issue2
dc.description.page139-149
dc.description.codenMIENE
dc.identifier.isiut000188297000004
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