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Optical properties of Ti and N implanted soda lime glass
dc.contributor.authorWas, Gary S.en_US
dc.contributor.authorRotberg, V. H. (Victor H.)en_US
dc.contributor.authorPlatts, Dennisen_US
dc.contributor.authorBomback, Johnen_US
dc.date.accessioned2010-05-06T23:19:44Z
dc.date.available2010-05-06T23:19:44Z
dc.date.issued1995-01-09en_US
dc.identifier.citationWas, G. S.; Rotberg, V.; Platts, D.; Bomback, J. (1995). "Optical properties of Ti and N implanted soda lime glass." Applied Physics Letters 66(2): 142-144. <http://hdl.handle.net/2027.42/71178>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/71178
dc.description.abstractSoda lime glass was implanted sequentially with Ti+ and N+ to doses ranging from 2 to 30×1016 cm−2 in order to study the resulting optical properties. Analysis of the implant distributions was made by using Rutherford backscattering and x‐ray photoelectron spectroscopy and revealed profiles which closely followed each other as designed by the selection of implant energies. Analysis of optical properties showed that the highest dose resulted in an increase in the fraction of infrared reflected by more than a factor of 4 versus 1.7 for the visible regime. The percentage of the total solar radiation rejected exceeded 60% at the highest dose, indicating that the buried layer is highly effective in reducing solar load. © 1995 American Institute of Physics.  en_US
dc.format.extent3102 bytes
dc.format.extent57695 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleOptical properties of Ti and N implanted soda lime glassen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Nuclear Engineering, University of Michigan, Ann Arbor, Michigan 48109‐2104en_US
dc.contributor.affiliationumGlass Division, Ford Motor Company, Dearborn, Michigan 48120‐1225en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/71178/2/APPLAB-66-2-142-1.pdf
dc.identifier.doi10.1063/1.113543en_US
dc.identifier.sourceApplied Physics Lettersen_US
dc.identifier.citedreferenceA. K. Rai, R. S. Bhattacharya, and S. C. Kung, Mater. Lett. MLETDJINS13, 35 (1992).en_US
dc.identifier.citedreferenceP. Mazzoldi, F. Caccavale, E. Cattaruzza, A. Boscolo-Boscoletto, R. Bertoncello, A. Glisenti, G. Battaglin, and C. Geradi, Nucl. Instrum. Methods Phys. Res. B NIMBEUINS65, 367 (1992).en_US
dc.identifier.citedreferenceG. Battaglin, in Modification Induced by Irradiation in Glasses, edited by P. Mazzoldi (Elsevier, Amsterdam, 1992), p. 11.en_US
dc.identifier.citedreferenceR. Bertoncello, A. Glisenti, G. Granozzi, G. Battaglin, E. Cattaruzza, and P. Mazzoldi, Mater. Res. Soc. Symp. Proc. MRSPDHINS268, 325 (1992).en_US
dc.identifier.citedreferenceL. R. Dolittle, Nucl. Instrum. Methods Phys. Res. B NIMBEUINS9, 334 (1985).en_US
dc.identifier.citedreferenceProprietary code, Ford Motor Company, Glass Division, 15000 Commerce Drive North, Dearborn, MI 48120.en_US
dc.owningcollnamePhysics, Department of


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