000809862 001__ 809862
000809862 005__ 20210129223153.0
000809862 0247_ $$2doi$$a10.1063/1.4942656
000809862 0247_ $$2ISSN$$a0021-8979
000809862 0247_ $$2ISSN$$a0148-6349
000809862 0247_ $$2ISSN$$a1089-7550
000809862 0247_ $$2WOS$$aWOS:000372351900055
000809862 0247_ $$2Handle$$a2128/17098
000809862 037__ $$aFZJ-2016-02788
000809862 082__ $$a530
000809862 1001_ $$0P:(DE-HGF)0$$aSertsu, M. G.$$b0$$eCorresponding author
000809862 245__ $$aDeposition and characterization of B$_{4}$C/CeO$_{2}$ multilayers at 6.x nm extreme ultraviolet wavelengths
000809862 260__ $$aMelville, NY$$bAmerican Inst. of Physics$$c2016
000809862 3367_ $$2DRIVER$$aarticle
000809862 3367_ $$2DataCite$$aOutput Types/Journal article
000809862 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1467706196_2695
000809862 3367_ $$2BibTeX$$aARTICLE
000809862 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000809862 3367_ $$00$$2EndNote$$aJournal Article
000809862 520__ $$aNew multilayers of boron carbide/cerium dioxide (B4C/CeO2) combination on silicon (Si) substrate are manufactured to represent reflective-optics candidates for future lithography at 6.x nm wavelength. This is one of only a few attempts to make multilayers of this kind. Combination of several innovative experiments enables detailed study of optical properties, structural properties, and interface profiles of the multilayers in order to open up a room for further optimization of the manufacturing process. The interface profile is visualized by high-angle annular dark-field imaging which provides highly sensitive contrast to atomic number. Synchrotron based at-wavelength extreme ultraviolet(EUV) reflectance measurements near the boron (B) absorption edge allow derivation of optical parameters with high sensitivity to local atom interactions. X-ray reflectivity measurements at Cu-Kalpha(8 keV) determine the period of multilayers with high in-depth resolution. By combining these measurements and choosing robust nonlinear curve fitting algorithms, accuracy of the results has been significantly improved. It also enables a comprehensive characterization of multilayers.Interface diffusion is determined to be a major cause for the low reflectivity performance. Optical constants of B4C and CeO2 layers are derived in EUV wavelengths. Besides, optical properties and asymmetric thicknesses of inter-diffusion layers (interlayers) in EUV wavelengths near the boron edge are determined. Finally, ideal reflectivity of the B4C/CeO2 combination is calculated by using optical constants derived from the proposed measurements in order to evaluate the potentiality of the design.
000809862 536__ $$0G:(DE-HGF)POF3-899$$a899 - ohne Topic (POF3-899)$$cPOF3-899$$fPOF III$$x0
000809862 588__ $$aDataset connected to CrossRef
000809862 7001_ $$0P:(DE-HGF)0$$aGiglia, A.$$b1
000809862 7001_ $$0P:(DE-HGF)0$$aBrose, S.$$b2
000809862 7001_ $$0P:(DE-HGF)0$$aPark, D.$$b3
000809862 7001_ $$0P:(DE-HGF)0$$aWang, Z. S.$$b4
000809862 7001_ $$0P:(DE-HGF)0$$aMayer, Joachim$$b5
000809862 7001_ $$0P:(DE-Juel1)157957$$aJuschkin, Larissa$$b6
000809862 7001_ $$0P:(DE-HGF)0$$aNicolosi, P.$$b7
000809862 773__ $$0PERI:(DE-600)1476463-5$$a10.1063/1.4942656$$gVol. 119, no. 9, p. 095301 -$$n9$$p095301 -$$tJournal of applied physics$$v119$$x1089-7550$$y2016
000809862 8564_ $$uhttps://juser.fz-juelich.de/record/809862/files/1.4942656.pdf$$yOpenAccess
000809862 8564_ $$uhttps://juser.fz-juelich.de/record/809862/files/1.4942656.gif?subformat=icon$$xicon$$yOpenAccess
000809862 8564_ $$uhttps://juser.fz-juelich.de/record/809862/files/1.4942656.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000809862 8564_ $$uhttps://juser.fz-juelich.de/record/809862/files/1.4942656.jpg?subformat=icon-700$$xicon-700$$yOpenAccess
000809862 8564_ $$uhttps://juser.fz-juelich.de/record/809862/files/1.4942656.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000809862 909CO $$ooai:juser.fz-juelich.de:809862$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000809862 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000809862 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bJ APPL PHYS : 2014
000809862 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000809862 915__ $$0StatID:(DE-HGF)0110$$2StatID$$aWoS$$bScience Citation Index
000809862 915__ $$0StatID:(DE-HGF)0111$$2StatID$$aWoS$$bScience Citation Index Expanded
000809862 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5
000809862 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000809862 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz
000809862 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences
000809862 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000809862 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bThomson Reuters Master Journal List
000809862 9141_ $$y2016
000809862 9101_ $$0I:(DE-588b)36225-6$$60000-0001-6277-1976$$aRWTH Aachen$$b0$$kRWTH
000809862 9101_ $$0I:(DE-588b)36225-6$$6P:(DE-HGF)0$$aRWTH Aachen$$b2$$kRWTH
000809862 9101_ $$0I:(DE-588b)36225-6$$6P:(DE-HGF)0$$aRWTH Aachen$$b3$$kRWTH
000809862 9101_ $$0I:(DE-588b)36225-6$$6P:(DE-Juel1)130824$$aRWTH Aachen$$b5$$kRWTH
000809862 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)157957$$aForschungszentrum Jülich$$b6$$kFZJ
000809862 9101_ $$0I:(DE-588b)36225-6$$6P:(DE-Juel1)157957$$aRWTH Aachen$$b6$$kRWTH
000809862 9131_ $$0G:(DE-HGF)POF3-899$$1G:(DE-HGF)POF3-890$$2G:(DE-HGF)POF3-800$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bProgrammungebundene Forschung$$lohne Programm$$vohne Topic$$x0
000809862 920__ $$lyes
000809862 9201_ $$0I:(DE-Juel1)PGI-9-20110106$$kPGI-9$$lHalbleiter-Nanoelektronik$$x0
000809862 9201_ $$0I:(DE-82)080009_20140620$$kJARA-FIT$$lJARA-FIT$$x1
000809862 980__ $$ajournal
000809862 980__ $$aVDB
000809862 980__ $$aUNRESTRICTED
000809862 980__ $$aI:(DE-Juel1)PGI-9-20110106
000809862 980__ $$aI:(DE-82)080009_20140620
000809862 9801_ $$aFullTexts