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Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering
A. Chiasera,
C. Meroni,
F. Scotognella,
Y.G. Boucher,
G. Galzerano,
A. Lukowiak,
D. Ristic,
G. Speranza,
S. Valligatla,
S. Varas,
L. Zur,
M. Ivanda,
G.C. Righini,
S. Taccheo,
R. Ramponi,
M. Ferrari,
Stefano Taccheo
Optical Materials
Swansea University Author: Stefano Taccheo
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DOI (Published version): 10.1016/j.optmat.2018.04.057
Abstract
All Er3+ doped dielectric 1-D microcavity was fabricated by rf sputtering technique. The microcavity was constituted by half wave Er3+ doped SiO2 active layer inserted between two Bragg reflectors consists of ten pairs of SiO2/TiO2 layers also doped with Er3+ ions. The scanning electron microscopy w...
Published in: | Optical Materials |
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ISSN: | 09253467 |
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2018
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URI: | https://cronfa.swan.ac.uk/Record/cronfa40264 |
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<?xml version="1.0"?><rfc1807><datestamp>2018-08-06T15:19:35.7616063</datestamp><bib-version>v2</bib-version><id>40264</id><entry>2018-05-18</entry><title>Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering</title><swanseaauthors><author><sid>ab5f951bdf448ec045d42a35d95dc0bf</sid><ORCID>0000-0003-0578-0563</ORCID><firstname>Stefano</firstname><surname>Taccheo</surname><name>Stefano Taccheo</name><active>true</active><ethesisStudent>false</ethesisStudent></author></swanseaauthors><date>2018-05-18</date><deptcode>MECH</deptcode><abstract>All Er3+ doped dielectric 1-D microcavity was fabricated by rf sputtering technique. The microcavity was constituted by half wave Er3+ doped SiO2 active layer inserted between two Bragg reflectors consists of ten pairs of SiO2/TiO2 layers also doped with Er3+ ions. The scanning electron microscopy was used to check the morphology of the structure. Transmission measurements confirm the third and first order cavity resonance at 530 nm and 1560 nm, respectively. The photoluminescence measurements were obtained by optically exciting at the third order cavity resonance using 514.5 nm Ar+ laser with an excitation angle of 30°. The Full Width at Half Maximum of the emission peak at 1560 nm decrease with the pump power until the spectral resolution of the detection system of ∼1.0 nm. Moreover, the emission intensity presents a non-linear behavior with the pump power and a threshold at about 24 mW was observed with saturation of the signal at above 185 mW of pump power.</abstract><type>Journal Article</type><journal>Optical Materials</journal><publisher/><issnPrint>09253467</issnPrint><keywords>rf-sputtering, 1-D dielectric microcavity, Silica, Titania, Erbium, Coherent emission</keywords><publishedDay>31</publishedDay><publishedMonth>12</publishedMonth><publishedYear>2018</publishedYear><publishedDate>2018-12-31</publishedDate><doi>10.1016/j.optmat.2018.04.057</doi><url/><notes/><college>COLLEGE NANME</college><department>Mechanical Engineering</department><CollegeCode>COLLEGE CODE</CollegeCode><DepartmentCode>MECH</DepartmentCode><institution>Swansea University</institution><apcterm/><lastEdited>2018-08-06T15:19:35.7616063</lastEdited><Created>2018-05-18T08:52:36.6268151</Created><path><level id="1">Faculty of Science and Engineering</level><level id="2">School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering</level></path><authors><author><firstname>A.</firstname><surname>Chiasera</surname><order>1</order></author><author><firstname>C.</firstname><surname>Meroni</surname><order>2</order></author><author><firstname>F.</firstname><surname>Scotognella</surname><order>3</order></author><author><firstname>Y.G.</firstname><surname>Boucher</surname><order>4</order></author><author><firstname>G.</firstname><surname>Galzerano</surname><order>5</order></author><author><firstname>A.</firstname><surname>Lukowiak</surname><order>6</order></author><author><firstname>D.</firstname><surname>Ristic</surname><order>7</order></author><author><firstname>G.</firstname><surname>Speranza</surname><order>8</order></author><author><firstname>S.</firstname><surname>Valligatla</surname><order>9</order></author><author><firstname>S.</firstname><surname>Varas</surname><order>10</order></author><author><firstname>L.</firstname><surname>Zur</surname><order>11</order></author><author><firstname>M.</firstname><surname>Ivanda</surname><order>12</order></author><author><firstname>G.C.</firstname><surname>Righini</surname><order>13</order></author><author><firstname>S.</firstname><surname>Taccheo</surname><order>14</order></author><author><firstname>R.</firstname><surname>Ramponi</surname><order>15</order></author><author><firstname>M.</firstname><surname>Ferrari</surname><order>16</order></author><author><firstname>Stefano</firstname><surname>Taccheo</surname><orcid>0000-0003-0578-0563</orcid><order>17</order></author></authors><documents><document><filename>0040264-18052018085553.pdf</filename><originalFilename>chiasera2018.pdf</originalFilename><uploaded>2018-05-18T08:55:53.8130000</uploaded><type>Output</type><contentLength>618446</contentLength><contentType>application/pdf</contentType><version>Accepted Manuscript</version><cronfaStatus>true</cronfaStatus><embargoDate>2019-05-10T00:00:00.0000000</embargoDate><copyrightCorrect>false</copyrightCorrect><language>eng</language></document></documents><OutputDurs/></rfc1807> |
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2018-08-06T15:19:35.7616063 v2 40264 2018-05-18 Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering ab5f951bdf448ec045d42a35d95dc0bf 0000-0003-0578-0563 Stefano Taccheo Stefano Taccheo true false 2018-05-18 MECH All Er3+ doped dielectric 1-D microcavity was fabricated by rf sputtering technique. The microcavity was constituted by half wave Er3+ doped SiO2 active layer inserted between two Bragg reflectors consists of ten pairs of SiO2/TiO2 layers also doped with Er3+ ions. The scanning electron microscopy was used to check the morphology of the structure. Transmission measurements confirm the third and first order cavity resonance at 530 nm and 1560 nm, respectively. The photoluminescence measurements were obtained by optically exciting at the third order cavity resonance using 514.5 nm Ar+ laser with an excitation angle of 30°. The Full Width at Half Maximum of the emission peak at 1560 nm decrease with the pump power until the spectral resolution of the detection system of ∼1.0 nm. Moreover, the emission intensity presents a non-linear behavior with the pump power and a threshold at about 24 mW was observed with saturation of the signal at above 185 mW of pump power. Journal Article Optical Materials 09253467 rf-sputtering, 1-D dielectric microcavity, Silica, Titania, Erbium, Coherent emission 31 12 2018 2018-12-31 10.1016/j.optmat.2018.04.057 COLLEGE NANME Mechanical Engineering COLLEGE CODE MECH Swansea University 2018-08-06T15:19:35.7616063 2018-05-18T08:52:36.6268151 Faculty of Science and Engineering School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering A. Chiasera 1 C. Meroni 2 F. Scotognella 3 Y.G. Boucher 4 G. Galzerano 5 A. Lukowiak 6 D. Ristic 7 G. Speranza 8 S. Valligatla 9 S. Varas 10 L. Zur 11 M. Ivanda 12 G.C. Righini 13 S. Taccheo 14 R. Ramponi 15 M. Ferrari 16 Stefano Taccheo 0000-0003-0578-0563 17 0040264-18052018085553.pdf chiasera2018.pdf 2018-05-18T08:55:53.8130000 Output 618446 application/pdf Accepted Manuscript true 2019-05-10T00:00:00.0000000 false eng |
title |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering |
spellingShingle |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering Stefano Taccheo |
title_short |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering |
title_full |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering |
title_fullStr |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering |
title_full_unstemmed |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering |
title_sort |
Coherent emission from fully Er 3+ doped monolithic 1-D dielectric microcavity fabricated by rf-sputtering |
author_id_str_mv |
ab5f951bdf448ec045d42a35d95dc0bf |
author_id_fullname_str_mv |
ab5f951bdf448ec045d42a35d95dc0bf_***_Stefano Taccheo |
author |
Stefano Taccheo |
author2 |
A. Chiasera C. Meroni F. Scotognella Y.G. Boucher G. Galzerano A. Lukowiak D. Ristic G. Speranza S. Valligatla S. Varas L. Zur M. Ivanda G.C. Righini S. Taccheo R. Ramponi M. Ferrari Stefano Taccheo |
format |
Journal article |
container_title |
Optical Materials |
publishDate |
2018 |
institution |
Swansea University |
issn |
09253467 |
doi_str_mv |
10.1016/j.optmat.2018.04.057 |
college_str |
Faculty of Science and Engineering |
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|
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facultyofscienceandengineering |
hierarchy_top_title |
Faculty of Science and Engineering |
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facultyofscienceandengineering |
hierarchy_parent_title |
Faculty of Science and Engineering |
department_str |
School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering |
document_store_str |
1 |
active_str |
0 |
description |
All Er3+ doped dielectric 1-D microcavity was fabricated by rf sputtering technique. The microcavity was constituted by half wave Er3+ doped SiO2 active layer inserted between two Bragg reflectors consists of ten pairs of SiO2/TiO2 layers also doped with Er3+ ions. The scanning electron microscopy was used to check the morphology of the structure. Transmission measurements confirm the third and first order cavity resonance at 530 nm and 1560 nm, respectively. The photoluminescence measurements were obtained by optically exciting at the third order cavity resonance using 514.5 nm Ar+ laser with an excitation angle of 30°. The Full Width at Half Maximum of the emission peak at 1560 nm decrease with the pump power until the spectral resolution of the detection system of ∼1.0 nm. Moreover, the emission intensity presents a non-linear behavior with the pump power and a threshold at about 24 mW was observed with saturation of the signal at above 185 mW of pump power. |
published_date |
2018-12-31T03:51:16Z |
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1763752517832802304 |
score |
11.036531 |