{"id":{"repo_id":"vt","oai_identifier":"oai:vtechworks.lib.vt.edu:10919/32266"},"canonical_url":"https://search.dev.ndltd.org/etd/vt/oai:vtechworks.lib.vt.edu:10919/32266","repository":{"repo_id":"vt","name":"Virginia Tech","base_url":"https://vtechworks.lib.vt.edu/oai/request"},"display":{"title":"Silica Fiber with Large and Thermodynamically Stable Second Order Optical Nonlinearity","abstract":"In this thesis, we demonstrate, theoretically, that, by depositing a regular fused-silica fiber with optical nonlinear molecules, strong and thermodynamically stable SHG can be obtained. Our experiments also provide strong evidence for the theory. Start from the basic Maxwell equation, we derive the SHG efficiency that the excited power translates into the SHG signal. According to the SHG efficiency equation, a small radius and a long length will help to result in a high SHG efficiency, which also increases with the excited power. We fabricate silica fiber tapers with radius less than 5 μm through either wet etching or heating while stretching. Through improving the stretching setup, and adroitly manipulating both the stretching rate and the heating temperature, we are able to control the taper loss less than 1 dB. Then we dip taper part into cationic solution and anionic solution alternatively to have ISAM/CHISAM film on it. By improving the surface quality of film around a silica fiber taper, we are able to control film loss of PAH/PR film to less than 2 dB for 5 bilayers. We set up a SHG measurement stage for a nonlinear fiber, and develop a measurement method during the experiments. We have shown that by depositing (PAH/PB)10 films around a fiber taper with a diameter around 5 µm, we can obtain high SHG signal. The ratio of the obtained SHG signal to the excitation power for such a nonlinear fiber is more than 10 times of that of a 125 µm single mode fiber with the same length. Our experiment result provides strong evidence that centrosymmetric material can be used as SHG material.","abstract_html":"In this thesis, we demonstrate, theoretically, that, by depositing a regular fused-silica fiber with optical nonlinear molecules, strong and thermodynamically stable SHG can be obtained. Our experiments also provide strong evidence for the theory. Start from the basic Maxwell equation, we derive the SHG efficiency that the excited power translates into the SHG signal. According to the SHG efficiency equation, a small radius and a long length will help to result in a high SHG efficiency, which also increases with the excited power. We fabricate silica fiber tapers with radius less than 5 μm through either wet etching or heating while stretching. Through improving the stretching setup, and adroitly manipulating both the stretching rate and the heating temperature, we are able to control the taper loss less than 1 dB. Then we dip taper part into cationic solution and anionic solution alternatively to have ISAM/CHISAM film on it. By improving the surface quality of film around a silica fiber taper, we are able to control film loss of PAH/PR film to less than 2 dB for 5 bilayers. We set up a SHG measurement stage for a nonlinear fiber, and develop a measurement method during the experiments. We have shown that by depositing (PAH/PB)10 films around a fiber taper with a diameter around 5 µm, we can obtain high SHG signal. The ratio of the obtained SHG signal to the excitation power for such a nonlinear fiber is more than 10 times of that of a 125 µm single mode fiber with the same length. Our experiment result provides strong evidence that centrosymmetric material can be used as SHG material.","abstract_has_math":false,"creators":["Yin, Yan"],"institution":"Virginia Tech","degree_name":"Master of Science","degree_level":"masters","degree_discipline":"Electrical and Computer Engineering","degree_department":"Electrical and Computer Engineering","school":null,"contributors":[],"advisors":[],"committee_chairs":["Xu, Yong"],"committee_members":["Wang, Anbo","Heflin, James R."],"year":2008,"date_issued":"2008-04-24","date_published":"2008-04-24","updated_at":"2026-07-22T22:20:08Z","subjects":["SHG measurement","ISAM CHISAM film","fiber tapering","SHG efficiency","film surface improvement"],"languages":[],"rights":["In Copyright"],"rights_urls":["http://rightsstatements.org/vocab/InC/1.0/"],"identifier_entries":[{"key":"dc:identifier.other","label":"Dc Identifier Other","values":["etd-05062008-160353"],"render_values":[{"text":"etd-05062008-160353","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/10919/32266","outbound_label":"Handle","outbound_source":"dc:identifier.uri"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor.committeechair","label":"Committee Chair","values":["Xu, Yong"]},{"key":"dc:contributor.committeemember","label":"Committee Member","values":["Wang, Anbo","Heflin, James R."]},{"key":"dc:contributor.department","label":"Department","values":["Electrical and Computer Engineering"]},{"key":"dc:creator","label":"Author","values":["Yin, Yan"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date.accessioned","label":"Dc Date Accessioned","values":["2014-03-14T20:35:20Z"]},{"key":"dc:date.available","label":"Dc Date Available","values":["2014-03-14T20:35:20Z","2008-05-28"]},{"key":"dc:date.issued","label":"Date","values":["2008-04-24"]},{"key":"dc:publisher","label":"Institution","values":["Virginia Tech"]},{"key":"dc:type","label":"Dc Type","values":["Thesis"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Electrical and Computer Engineering"]},{"key":"thesis:degree_level","label":"Degree Level","values":["masters"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Master of Science"]},{"key":"thesis:institution_name","label":"Thesis Institution Name","values":["Virginia Polytechnic Institute and State University"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["SHG measurement","ISAM CHISAM film","fiber tapering","SHG efficiency","film surface improvement"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:rights","label":"Dc Rights","values":["In Copyright"]},{"key":"dc:rights.uri","label":"Rights URI","values":["http://rightsstatements.org/vocab/InC/1.0/"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier.other","label":"Dc Identifier Other","values":["etd-05062008-160353"]},{"key":"dc:identifier.uri","label":"Identifier URI","values":["http://hdl.handle.net/10919/32266"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description.abstract","label":"Abstract","values":["In this thesis, we demonstrate, theoretically, that, by depositing a regular fused-silica fiber with optical nonlinear molecules, strong and thermodynamically stable SHG can be obtained. Our experiments also provide strong evidence for the theory. Start from the basic Maxwell equation, we derive the SHG efficiency that the excited power translates into the SHG signal. According to the SHG efficiency equation, a small radius and a long length will help to result in a high SHG efficiency, which also increases with the excited power. We fabricate silica fiber tapers with radius less than 5 μm through either wet etching or heating while stretching. Through improving the stretching setup, and adroitly manipulating both the stretching rate and the heating temperature, we are able to control the taper loss less than 1 dB. Then we dip taper part into cationic solution and anionic solution alternatively to have ISAM/CHISAM film on it. By improving the surface quality of film around a silica fiber taper, we are able to control film loss of PAH/PR film to less than 2 dB for 5 bilayers. We set up a SHG measurement stage for a nonlinear fiber, and develop a measurement method during the experiments. We have shown that by depositing (PAH/PB)10 films around a fiber taper with a diameter around 5 µm, we can obtain high SHG signal. The ratio of the obtained SHG signal to the excitation power for such a nonlinear fiber is more than 10 times of that of a 125 µm single mode fiber with the same length. Our experiment result provides strong evidence that centrosymmetric material can be used as SHG material."]},{"key":"dc:description.degree","label":"Dc Description Degree","values":["Master of Science"]},{"key":"dc:title","label":"Title","values":["Silica Fiber with Large and Thermodynamically Stable Second Order Optical Nonlinearity"]}]}],"canonical_facts":{"dc:contributor.committeechair":["Xu, Yong"],"dc:contributor.committeemember":["Wang, Anbo","Heflin, James R."],"dc:contributor.department":["Electrical and Computer Engineering"],"dc:creator":["Yin, Yan"],"dc:date.accessioned":["2014-03-14T20:35:20Z"],"dc:date.available":["2014-03-14T20:35:20Z","2008-05-28"],"dc:date.issued":["2008-04-24"],"dc:description.abstract":["In this thesis, we demonstrate, theoretically, that, by depositing a regular fused-silica fiber with optical nonlinear molecules, strong and thermodynamically stable SHG can be obtained. Our experiments also provide strong evidence for the theory. Start from the basic Maxwell equation, we derive the SHG efficiency that the excited power translates into the SHG signal. According to the SHG efficiency equation, a small radius and a long length will help to result in a high SHG efficiency, which also increases with the excited power. We fabricate silica fiber tapers with radius less than 5 μm through either wet etching or heating while stretching. Through improving the stretching setup, and adroitly manipulating both the stretching rate and the heating temperature, we are able to control the taper loss less than 1 dB. Then we dip taper part into cationic solution and anionic solution alternatively to have ISAM/CHISAM film on it. By improving the surface quality of film around a silica fiber taper, we are able to control film loss of PAH/PR film to less than 2 dB for 5 bilayers. We set up a SHG measurement stage for a nonlinear fiber, and develop a measurement method during the experiments. We have shown that by depositing (PAH/PB)10 films around a fiber taper with a diameter around 5 µm, we can obtain high SHG signal. The ratio of the obtained SHG signal to the excitation power for such a nonlinear fiber is more than 10 times of that of a 125 µm single mode fiber with the same length. Our experiment result provides strong evidence that centrosymmetric material can be used as SHG material."],"dc:description.degree":["Master of Science"],"dc:identifier.other":["etd-05062008-160353"],"dc:identifier.uri":["http://hdl.handle.net/10919/32266"],"dc:publisher":["Virginia Tech"],"dc:rights":["In Copyright"],"dc:rights.uri":["http://rightsstatements.org/vocab/InC/1.0/"],"dc:subject":["SHG measurement","ISAM CHISAM film","fiber tapering","SHG efficiency","film surface improvement"],"dc:title":["Silica Fiber with Large and Thermodynamically Stable Second Order Optical Nonlinearity"],"dc:type":["Thesis"],"thesis:degree_discipline":["Electrical and Computer Engineering"],"thesis:degree_level":["masters"],"thesis:degree_name":["Master of Science"],"thesis:institution_name":["Virginia Polytechnic Institute and State University"]},"updated_at":"2026-07-22T22:20:08Z"}