manifestation_id original_title title_alternative title_transcription statement_of_responsibility manifestation_identifier creator contributor publisher date_of_publication pub_date year_of_publication publication_place manifestation_created_at manifestation_updated_at carrier_type content_type frequency language isbn issn doi jpno ncid lccn iss_itemno volume_number volume_number_string edition edition_string issue_number issue_number_string serial_number extent start_page end_page dimensions height width depth manifestation_price access_address manifestation_required_role abstract description identifier:unknown identifier:nbn identifier:isbn10 identifier:iss_itemno identifier:online_isbn identifier:print_isbn identifier:print_issn identifier:online_issn identifier:escidoc identifier:nims series_statement_id series_statement_original_title series_statement_title_subseries series_statement_title_subseries_transcription series_statement_title_transcription series_statement_creator series_statement_volume_number series_statement_series_master series_statement_root_manifestation_id series_statement_manifestation_id series_statement_position series_statement_note series_statement_created_at series_statement_updated_at subject:ndlsh subject:unknown subject:bsh classification:ndc8 classification:ndc9 classification:udc item_id item_identifier binding_item_identifier call_number library shelf item_note accepted_at acquired_at item_created_at item_updated_at 105417 "Formation of optical coupling structure between two ends of silica glass optical fibers by inserting tellurite glass melt" TODOROKI Shin-ichi//Nukui A.//Inoue S. "" "" 2002-05-01 00:00:00 +0900 2002-05-01 2002 2015-12-15 21:30:37 +0900 2023-07-31 14:41:14 +0900 online_resource text unknown English "" "" 476 478 https://hdl.handle.net/20.500.11932/28375 Guest " Several nano liters of tellurite glass melt was inserted and quenched between two ends of silica glass optical fibers to form a optical coupling structure, whose length was several hundred um. Dispite the large gap of thermal expansion coefficient between these glass materials, neither fracture nor bubbles were observed, which usually lead to a large optical propagation loss. The insertion loss was less than 10 dB, which was mainly due to the lack of an optical waveguide structure in the tellurite glass segment. Further loss decrease is expected to be possible by introducing a refractive index modulation. " "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" optical fiber//tellurite glass//thermal expansion//optical fiber//tellurite glass//thermal expansion//optical fiber//tellurite glass//thermal expansion "" "" "" "" 99798 web web 2023-07-31 14:41:14 +0900 2023-07-31 14:41:14 +0900 105407 "Combinatorial Fluorescence Lifetime Measuring System for Developing Er-Doped Transparent Glass Ceramics" TODOROKI Shin-ichi//Inoue S. "" "" 2004-02-15 00:00:00 +0900 2004-02-15 2004 2015-12-15 21:30:27 +0900 2023-07-31 14:38:51 +0900 online_resource text unknown English "" "" 39 43 https://hdl.handle.net/20.500.11932/28369 Guest "Fluorescence lifetime of Er3+ was measured for F-doped tellurite glasses with parallel heat treatment under a temperature gradient atmosphere in order to find the annealing condition to make transparent glass ceramics in which Er3+ ions are located in the precipitated crystals. The preparation and annealing of the samples were performed in a vertical temperature gradient furnace, where molten glass was sucked into a pre-heated Pyrex glass tube. The annealing temperature range is between 350 degC and 800 degC. After the annealing treatment, time-resolved fluorescence emission of Er3+ (1.55um; excitation light source is 977nm) were measured sequentially along the tube. The lifetime of the emission was about 2.6 msec for as-prepared glass. We have found that the lifetime increased to 5.2 msec when the glass was annealed at 470 degC for 5 min and 550 degC for 5 min successively, although its transparency was lost. This increase implies that the Er3+ ions are embedded in fluorine-rich phase to bring about reduced non-radiative emission. We are now continuing to find the condition to get transparent glass ceramics. " "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" tellurite glass//erbium//fluorescence lifetime "" "" "" "" 99360 web web 2023-07-31 14:38:51 +0900 2023-07-31 14:38:51 +0900 105406 "Low loss optical coupling structure between two ends of silica glass optical fibers by inserting TeO2 melt" TODOROKI Shin-ichi//Inoue S. "" "" 2003-10-15 00:00:00 +0900 2003-10-15 2003 2015-12-15 21:30:25 +0900 2023-07-31 14:40:53 +0900 online_resource text unknown English "" "" 237 240 https://hdl.handle.net/20.500.11932/28372 Guest "Less than 1.5dB of insertion loss was realized in an optical coupling structure in which two TEC (Thermal-diffusion Expanded Core) fibers are spliced via quenched TeO2 melt whose length was 0.5mm. The quenched melt seems to be free of precipitates because they would bring about larger loss if existed. The loss due to imperfect optical coupling between the fibers is estimated to be about 1 dB, which can be reduced by introducing some refractive index modulation into the present structure. " "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" optical fiber//tellurite glass "" "" "" "" 99731 web web 2023-07-31 14:40:53 +0900 2023-07-31 14:40:53 +0900 105335 Formation of optical coupling structure between silica glass waveguides and molten tellurite glass droplet Todoroki S.//Nukui A.//Inoue S. "" "" 2015-12-15 21:29:11 +0900 2025-07-14 15:47:27 +0900 online_resource text unknown English "" "" https://hdl.handle.net/20.500.11932/28398 Guest "Several nano liters of tellurite glass melt (xTeO2-(100-x)ZnO, x=80,90,100 in mol%) were inserted and quenched between two ends of silica glass optical fibers to form a new optical coupling structure, whose length was several hundred microns. No visible precipitates were found even in the quenched melt of 100% TeO2. On the basis of reflection and insertion loss measurements and a bending test, it is proved that there's no micro crystals in the quenched melt segment which cause light scattering and/or stress concentration. Few tens nano liters of the melt were also inserted into a silica glass capillary tube with the interior diameter of 126 $\mu$m, in order to examine their tolerance to the residual stress induced on cooling due to the large gap in thermal expansion coefficient between the two glasses. Neither fracture nor bubbles were observed in the quenched melt inside if its length is less than 2mm. This implies that tellurite melt can be introduced into voids of sub-mm in size to integrate hybrid lightwave circuits. " "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" optical fiber//tellurite glass//insertion loss//thermal expansion coefficient//optical fiber//tellurite glass//insertion loss//thermal expansion coefficient//optical fiber//tellurite glass//insertion loss//thermal expansion coefficient "" "" "" "" 104431 web web 2025-07-14 15:02:29 +0900 2025-07-14 15:47:27 +0900 103749 Formation of optical coupling structure between silica glass waveguides and molten tellurite glass droplet TODOROKI Shin-ichi//Nukui A.//Inoue S. Zhu Congshan "" 2015-05-28 18:07:12 +0900 2023-07-31 14:42:08 +0900 online_resource text unknown English "" "" https://hdl.handle.net/20.500.11932/101921 Guest "Several nano liters of tellurite glass melt (xTeO2-(100-x)ZnO, x=80,90,100 in mol%) were inserted and quenched between two ends of silica glass optical fibers to form a new optical coupling structure, whose length was several hundred microns. No visible precipitates were found even in the quenched melt of 100% TeO2. On the basis of reflection and insertion loss measurements and a bending test, it is proved that there's no micro crystals in the quenched melt segment which cause light scattering and/or stress concentration. Few tens nano liters of the melt were also inserted into a silica glass capillary tube with the interior diameter of 126 $\mu$m, in order to examine their tolerance to the residual stress induced on cooling due to the large gap in thermal expansion coefficient between the two glasses. Neither fracture nor bubbles were observed in the quenched melt inside if its length is less than 2mm. This implies that tellurite melt can be introduced into voids of sub-mm in size to integrate hybrid lightwave circuits." "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" optical fiber//tellurite glass//insertion loss//thermal expansion coefficient//optical fiber//tellurite glass//insertion loss//thermal expansion coefficient//optical fiber//tellurite glass//insertion loss//thermal expansion coefficient//optical fiber//tellurite glass//insertion loss//thermal expansion coefficient "" "" "" "" 99968 web web 2023-07-31 14:42:08 +0900 2023-07-31 14:42:08 +0900 103439 Low loss optical coupling structure between two ends of silica glass optical fibers by inserting TeO2 melt TODOROKI Shin-ichi//Inoue Satoru "" "" 2003-10-02 00:00:00 +0900 2003-10-02 2003 2015-05-28 18:04:28 +0900 2023-07-31 14:46:42 +0900 online_resource text unknown English "" "" https://hdl.handle.net/20.500.11932/94914 Guest Less than 1.5 dB of insertion loss was realized in an optical coupling structure in which two TEC (Thermal-diffusion Expanded Core) fibers are spliced via quenched TeO2 melt whose length was 0.5 mm. The quenched melt seems to be free of precipitates because they would bring about larger loss if existed. The loss due to imperfect optical coupling between the fibers is estimated to be about 1 dB, which can be reduced by introducing some refractive index modulation into the present structure. This fabrication method is useful to make a connection between silica waveguides and non-silica glasses with poor thermal stability. "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" "" optical fiber//tellurite glass//splicing//optical fiber//tellurite glass//splicing//optical fiber//tellurite glass//splicing//optical fiber//tellurite glass//splicing "" "" "" "" 100820 web web 2023-07-31 14:46:42 +0900 2023-07-31 14:46:42 +0900