<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Publishing DTD v1.3 20210610//EN" "JATS-journalpublishing1-3.dtd">
<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="en"><front><journal-meta><journal-id journal-id-type="publisher-id">najo</journal-id><journal-title-group><journal-title xml:lang="en">Nanosystems: Physics, Chemistry, Mathematics</journal-title><trans-title-group xml:lang="ru"><trans-title>Наносистемы: физика, химия, математика</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">2220-8054</issn><issn pub-type="epub">2305-7971</issn><publisher><publisher-name>Университет ИТМО</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.17586/2220-8054-2024-15-2-184-191</article-id><article-id custom-type="elpub" pub-id-type="custom">najo-33</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>PHYSICS</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>ФИЗИКА</subject></subj-group></article-categories><title-group><article-title>Q-switched and mode-locked pulse generations with Ti3AlC2 absorber</article-title><trans-title-group xml:lang="ru"><trans-title>Генерация импульсов с модуляцией добротности и синхронизацией мод с помощью поглотителя Ti3AlC2</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0009-0003-9890-6926</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Альджунид</surname><given-names>С. З.З.</given-names></name><name name-style="western" xml:lang="en"><surname>Aljunid</surname><given-names>S. Z.Z.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Альджунид Сайед Зиад З. </p></bio><bio xml:lang="en"><p>Syed Ziad Z. Aljunid.</p><p>Kuala Lumpur 50603</p></bio><email xlink:type="simple">22064743@siswa.um.edu.my</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0003-4557-5695</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Гафар</surname><given-names>Н. А.М.А.</given-names></name><name name-style="western" xml:lang="en"><surname>Ghafar</surname><given-names>N. A.M. A.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Гафар Нурул Атира М.А.</p></bio><bio xml:lang="en"><p>Nurul Athirah M. A. Ghafar.</p><p>Kuala Lumpur 50603</p></bio><email xlink:type="simple">athirahghafar97@gmail.com</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Ахмад</surname><given-names>Б. А.</given-names></name><name name-style="western" xml:lang="en"><surname>Ahmad</surname><given-names>B. A.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Ахмад Билал А.</p></bio><bio xml:lang="en"><p>Bilal A. Ahmad.</p><p>Al-Washash, 700921 Baghdad</p></bio><email xlink:type="simple">belalanwer@yahoo.com</email><xref ref-type="aff" rid="aff-2"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0002-3597-5938</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Апсари</surname><given-names>Р.</given-names></name><name name-style="western" xml:lang="en"><surname>Apsari</surname><given-names>R.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Апсари Ретна.</p></bio><bio xml:lang="en"><p>Retna Apsari.</p><p>Surabaya (60115)</p></bio><email xlink:type="simple">retna-a@fst.unair.ac.id</email><xref ref-type="aff" rid="aff-3"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0003-4879-5853</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Харун</surname><given-names>С. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Harun</surname><given-names>S. W.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Харун Сулейман В. </p></bio><bio xml:lang="en"><p>Sulaiman W. Harun.</p><p>Kuala Lumpur 50603, Malaysia; Surabaya (60115) Indonesia</p></bio><email xlink:type="simple">swharun@um.edu.my</email><xref ref-type="aff" rid="aff-4"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Department of Electrical Engineering, Faculty of Engineering, University of Malaya</institution><country>Malaysia</country></aff><aff xml:lang="en" id="aff-2"><institution>Department of Communication Engineering, Al-Ma’moon University College</institution><country>Iraq</country></aff><aff xml:lang="en" id="aff-3"><institution>Department of Physics, Faculty of Science and Technology, Airlangga University</institution><country>Indonesia</country></aff><aff xml:lang="en" id="aff-4"><institution>Department of Electrical Engineering, Faculty of Engineering, University of Malaya; Department of Physics, Faculty of Science and Technology, Airlangga University</institution><country>Malaysia</country></aff><pub-date pub-type="collection"><year>2024</year></pub-date><pub-date pub-type="epub"><day>31</day><month>05</month><year>2025</year></pub-date><volume>15</volume><issue>2</issue><fpage>184</fpage><lpage>191</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Aljunid S.Z., Ghafar N.A., Ahmad B.A., Apsari R., Harun S.W., 2025</copyright-statement><copyright-year>2025</copyright-year><copyright-holder xml:lang="ru">Альджунид С.З., Гафар Н.А., Ахмад Б.А., Апсари Р., Харун С.В.</copyright-holder><copyright-holder xml:lang="en">Aljunid S.Z., Ghafar N.A., Ahmad B.A., Apsari R., Harun S.W.</copyright-holder><license xml:lang="ru" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>Данная работа распространяется под лицензией Creative Commons Attribution 4.0.</license-p></license><license xml:lang="en" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://nanojournal.ifmo.ru/jour/article/view/33">https://nanojournal.ifmo.ru/jour/article/view/33</self-uri><abstract><p>Exploring advanced saturable absorber (SA) materials that exhibit exceptional performance for achieving Q-switching and mode-locking operations remains a vibrant area of research in the field of fiber lasers. The remarkable optical nonlinearity, coupled with high thermal and chemical stability of MAX phase materials, positions them as promising candidates for high-performance SAs. In this study, we demonstrated the potential of Ti3AlC2 MAX phase as an effective material for Q-switched and mode-locked fiber laser applications. The Ti3AlC2 film was synthesized through a straightforward and cost-effective casting method employing polyvinyl alcohol (PVA) as a host material. The SA was cleverly constructed from the film, utilizing a sandwich-structured fiber-ferrule platform, and seamlessly integrated into an Erbium-doped fiber laser (EDFL) ring cavity. Initially, a stable Q-switched laser was realized at a center wavelength of 1531 nm. The repetition rate exhibited a commendable increase from 35.0 to 50.8 kHz, and the pulse width reduced from 6.58 to 3.40 µs as the pump power was adjusted within the range of 25.98 to 58.29 mW. Notably, the maximum output power of 2.49 mW and a pulse energy of 49.02 nJ were recorded at a pump power of 58.29 mW. Subsequently, an additional 200 m long single-mode fiber was added into a similar laser cavity, leading to the generation of a stable mode-locked laser at a threshold pump power of 81.37 mW, operating at a central wavelength of 1558.96 nm. The observed stable repetition rate of 969.3 kHz, coupled with a pulse duration of 300 ns, demonstrated robust performance as the pump power increased from 81.37 to 113.68 mW. These findings highlight the exceptional performance of Ti3AlC2 SA for both Q-switching and mode-locking applications. The versatility of these lasers makes them valuable for diverse applications, including micromachining of materials, frequency comb generation, and remote sensing.</p></abstract><trans-abstract xml:lang="ru"><p>Исследование современных материалов насыщающегося поглотителя (SA), которые демонстрируют исключительные характеристики для выполнения операций переключения добротности и синхронизации мод, остается динамичной областью исследований в области волоконных лазеров. Замечательная оптическая нелинейность в сочетании с высокой термической и химической стабильностью материалов фазы MAX делает их перспективными кандидатами на роль высокопроизводительных СА. В этом исследовании мы продемонстрировали потенциал фазы Ti3AlC2 MAX в качестве эффективного материала для применения в волоконных лазерах с модуляцией добротности и синхронизацией мод. Пленка Ti3AlC2 была синтезирована простым и экономичным методом литья с использованием поливинилового спирта (ПВС) в качестве основного материала. SA был умело сконструирован из пленки с использованием многослойной платформы с оптоволоконными наконечниками и легко интегрирован в кольцевой резонатор волоконного лазера, легированного эрбием (EDFL). Первоначально был реализован стабильный лазер с модуляцией добротности с центральной длиной волны 1531 нм. Частота повторения заметно увеличилась с 35,0 до 50,8 кГц, а длительность импульса уменьшилась с 6,58 до 3,40 мкс при регулировке мощности накачки в диапазоне от 25,98 до 58,29 мВт. Примечательно, что максимальная выходная мощность 2,49 мВт и энергия импульса 49,02 нДж были зафиксированы при мощности накачки 58,29 мВт. Впоследствии в аналогичный резонатор лазера было добавлено дополнительное одномодовое волокно длиной 200 м, что привело к генерации стабильного лазера с синхронизацией мод с пороговой мощностью накачки 81,37 мВт, работающего на центральной длине волны 1558,96 нм. Наблюдаемая стабильная частота следования 969,3 кГц в сочетании с длительностью импульса 300 нс продемонстрировала устойчивую работу при увеличении мощности накачки с 81,37 до 113,68 мВт. Эти результаты подчеркивают исключительные характеристики Ti3AlC2 SA как для приложений с модуляцией добротности, так и для синхронизации мод. Универсальность этих лазеров делает их ценными для различных применений, включая микрообработку материалов, генерацию гребенки частот и дистанционное зондирование.</p></trans-abstract><kwd-group xml:lang="en"><kwd>Ti3AlC2</kwd><kwd>max phase material</kwd><kwd>Q-switching</kwd><kwd>mode-locking</kwd><kwd>saturable absorber</kwd><kwd>erbium-doped fiber laser</kwd></kwd-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Dong L., Samson B. Fiber Lasers: Basics, Technology, and Applications. CRC press, New York, 2016.</mixed-citation><mixed-citation xml:lang="en">Dong L., Samson B. Fiber Lasers: Basics, Technology, and Applications. CRC press, New York, 2016.</mixed-citation></citation-alternatives></ref><ref id="cit2"><label>2</label><citation-alternatives><mixed-citation xml:lang="ru">Shi W., et al. Fiber lasers and their applications. Applied optics, 2014, 53 (28), P. 6554–6568.</mixed-citation><mixed-citation xml:lang="en">Shi W., et al. Fiber lasers and their applications. Applied optics, 2014, 53 (28), P. 6554–6568.</mixed-citation></citation-alternatives></ref><ref id="cit3"><label>3</label><citation-alternatives><mixed-citation xml:lang="ru">Sun S., et al. Demonstration of passively Q-switched and mode-locked operations through dispersion control in Er-doped fiber lasers with a cylindrite-based saturable absorber. J. of Luminescence, 2022, 250, 119064.</mixed-citation><mixed-citation xml:lang="en">Sun S., et al. Demonstration of passively Q-switched and mode-locked operations through dispersion control in Er-doped fiber lasers with a cylindrite-based saturable absorber. J. of Luminescence, 2022, 250, 119064.</mixed-citation></citation-alternatives></ref><ref id="cit4"><label>4</label><citation-alternatives><mixed-citation xml:lang="ru">Liu W., et al. 2D Materials for Fiber Lasers: Recent Advances of 2D Materials in Nonlinear Photonics and Fiber Lasers. Advanced Optical Materials, 2020, 8 (8), 2070031.</mixed-citation><mixed-citation xml:lang="en">Liu W., et al. 2D Materials for Fiber Lasers: Recent Advances of 2D Materials in Nonlinear Photonics and Fiber Lasers. Advanced Optical Materials, 2020, 8 (8), 2070031.</mixed-citation></citation-alternatives></ref><ref id="cit5"><label>5</label><citation-alternatives><mixed-citation xml:lang="ru">Zhang Y., et al. Study of the influence of SESAM parameters on the evolution of mode-locked pulses at different repetition rates. Applied Physics B, 2021, 127 (8), P. 1–10.</mixed-citation><mixed-citation xml:lang="en">Zhang Y., et al. Study of the influence of SESAM parameters on the evolution of mode-locked pulses at different repetition rates. Applied Physics B, 2021, 127 (8), P. 1–10.</mixed-citation></citation-alternatives></ref><ref id="cit6"><label>6</label><citation-alternatives><mixed-citation xml:lang="ru">Nishizawa N., et al. Dynamics of a dispersion-managed passively mode-locked Er-doped fiber laser using single wall carbon nanotubes. Photonics, 2015, 2 (3), P. 808–824.</mixed-citation><mixed-citation xml:lang="en">Nishizawa N., et al. Dynamics of a dispersion-managed passively mode-locked Er-doped fiber laser using single wall carbon nanotubes. Photonics, 2015, 2 (3), P. 808–824.</mixed-citation></citation-alternatives></ref><ref id="cit7"><label>7</label><citation-alternatives><mixed-citation xml:lang="ru">Haris H., et al. Generation of Vector Soliton Pulses with Graphene Oxide Film in Mode-locked Erbium-doped Fiber Laser Cavity. Nonlinear Optics Quantum Optics-Concepts in Modern Optics, 2020, 52 (1–2), P. 111–118.</mixed-citation><mixed-citation xml:lang="en">Haris H., et al. Generation of Vector Soliton Pulses with Graphene Oxide Film in Mode-locked Erbium-doped Fiber Laser Cavity. Nonlinear Optics Quantum Optics-Concepts in Modern Optics, 2020, 52 (1–2), P. 111–118.</mixed-citation></citation-alternatives></ref><ref id="cit8"><label>8</label><citation-alternatives><mixed-citation xml:lang="ru">Hu J.-W., et al. Passively mode-locked Er-doped fiber laser based on a semi-metallic InBi saturable absorber. J. of Physics D: Applied Physics, 2021, 55 (10), 105104.</mixed-citation><mixed-citation xml:lang="en">Hu J.-W., et al. Passively mode-locked Er-doped fiber laser based on a semi-metallic InBi saturable absorber. J. of Physics D: Applied Physics, 2021, 55 (10), 105104.</mixed-citation></citation-alternatives></ref><ref id="cit9"><label>9</label><citation-alternatives><mixed-citation xml:lang="ru">Haris H., et al. Mode-Locked YDFL Using Topological Insulator Bismuth Selenide Nanosheets as the Saturable Absorber. Crystals, 2022, 12 (4), 489.</mixed-citation><mixed-citation xml:lang="en">Haris H., et al. Mode-Locked YDFL Using Topological Insulator Bismuth Selenide Nanosheets as the Saturable Absorber. Crystals, 2022, 12 (4), 489.</mixed-citation></citation-alternatives></ref><ref id="cit10"><label>10</label><citation-alternatives><mixed-citation xml:lang="ru">Ismail E., et al. Black phosphorus crystal as a saturable absorber for both a Q-switched and mode-locked erbium-doped fiber laser. RSC Advances, 2016, 6 (76), P. 72692–72697.</mixed-citation><mixed-citation xml:lang="en">Ismail E., et al. Black phosphorus crystal as a saturable absorber for both a Q-switched and mode-locked erbium-doped fiber laser. RSC Advances, 2016, 6 (76), P. 72692–72697.</mixed-citation></citation-alternatives></ref><ref id="cit11"><label>11</label><citation-alternatives><mixed-citation xml:lang="ru">Tiu Z., et al. Application of transition metal dichalcogenide in pulsed fiber laser system. Materials Research Express, 2019, 6 (8), 082004.</mixed-citation><mixed-citation xml:lang="en">Tiu Z., et al. Application of transition metal dichalcogenide in pulsed fiber laser system. Materials Research Express, 2019, 6 (8), 082004.</mixed-citation></citation-alternatives></ref><ref id="cit12"><label>12</label><citation-alternatives><mixed-citation xml:lang="ru">Rosol A.H.A., et al. Nanosecond pulses generation with rose gold nanoparticles saturable absorber. Indian J. of Physics, 2020, 94 (7), P. 1079–1083.</mixed-citation><mixed-citation xml:lang="en">Rosol A.H.A., et al. Nanosecond pulses generation with rose gold nanoparticles saturable absorber. Indian J. of Physics, 2020, 94 (7), P. 1079–1083.</mixed-citation></citation-alternatives></ref><ref id="cit13"><label>13</label><citation-alternatives><mixed-citation xml:lang="ru">Jafry A.A.A., et al. MXene Ti3C2Tx as a passive Q-switcher for erbium-doped fiber laser. Optical Fiber Technology, 2020, 58, 102289.</mixed-citation><mixed-citation xml:lang="en">Jafry A.A.A., et al. MXene Ti3C2Tx as a passive Q-switcher for erbium-doped fiber laser. Optical Fiber Technology, 2020, 58, 102289.</mixed-citation></citation-alternatives></ref><ref id="cit14"><label>14</label><citation-alternatives><mixed-citation xml:lang="ru">Fu B., et al. MXenes: Synthesis, optical properties, and applications in ultrafast photonics. Small, 2021, 17 (11), 2006054.</mixed-citation><mixed-citation xml:lang="en">Fu B., et al. MXenes: Synthesis, optical properties, and applications in ultrafast photonics. Small, 2021, 17 (11), 2006054.</mixed-citation></citation-alternatives></ref><ref id="cit15"><label>15</label><citation-alternatives><mixed-citation xml:lang="ru">Gonzalez-Julian J. Processing of MAX phases: From synthesis to applications. J. of the American Ceramic Society, 2021, 104 (2), P. 659–690.</mixed-citation><mixed-citation xml:lang="en">Gonzalez-Julian J. Processing of MAX phases: From synthesis to applications. J. of the American Ceramic Society, 2021, 104 (2), P. 659–690.</mixed-citation></citation-alternatives></ref><ref id="cit16"><label>16</label><citation-alternatives><mixed-citation xml:lang="ru">Khazaei M., et al. Recent advances in MXenes: From fundamentals to applications. Current Opinion in Solid State and Materials Science, 2019, 23 (3), P. 164–178.</mixed-citation><mixed-citation xml:lang="en">Khazaei M., et al. Recent advances in MXenes: From fundamentals to applications. Current Opinion in Solid State and Materials Science, 2019, 23 (3), P. 164–178.</mixed-citation></citation-alternatives></ref><ref id="cit17"><label>17</label><citation-alternatives><mixed-citation xml:lang="ru">Gogotsi Y., Anasori B. The rise of MXenes. ACS Nano, 2019, 13 (8), P. 8491–8494.</mixed-citation><mixed-citation xml:lang="en">Gogotsi Y., Anasori B. The rise of MXenes. ACS Nano, 2019, 13 (8), P. 8491–8494.</mixed-citation></citation-alternatives></ref><ref id="cit18"><label>18</label><citation-alternatives><mixed-citation xml:lang="ru">Zhang Z., et al. On the formation mechanisms and properties of MAX phases: A review. J. of the European Ceramic Society, 2021, 41 (7), P. 3851–3878.</mixed-citation><mixed-citation xml:lang="en">Zhang Z., et al. On the formation mechanisms and properties of MAX phases: A review. J. of the European Ceramic Society, 2021, 41 (7), P. 3851–3878.</mixed-citation></citation-alternatives></ref><ref id="cit19"><label>19</label><citation-alternatives><mixed-citation xml:lang="ru">Sun Z. Progress in research and development on MAX phases: a family of layered ternary compounds. Int. Materials Reviews, 2011, 56 (3), P. 143–166.</mixed-citation><mixed-citation xml:lang="en">Sun Z. Progress in research and development on MAX phases: a family of layered ternary compounds. Int. Materials Reviews, 2011, 56 (3), P. 143–166.</mixed-citation></citation-alternatives></ref><ref id="cit20"><label>20</label><citation-alternatives><mixed-citation xml:lang="ru">Wu K., et al. High-performance mode-locked and Q-switched fiber lasers based on novel 2D materials of topological insulators, transition metal dichalcogenides and black phosphorus: review and perspective. Optics Communications, 2018, 406, P. 214–229.</mixed-citation><mixed-citation xml:lang="en">Wu K., et al. High-performance mode-locked and Q-switched fiber lasers based on novel 2D materials of topological insulators, transition metal dichalcogenides and black phosphorus: review and perspective. Optics Communications, 2018, 406, P. 214–229.</mixed-citation></citation-alternatives></ref><ref id="cit21"><label>21</label><citation-alternatives><mixed-citation xml:lang="ru">Bazhenov A.Y., et al. Random Laser Based on Materials in the Form of Complex Network Structures. JETP Letters, 2023, 117 (11), P. 814–820.</mixed-citation><mixed-citation xml:lang="en">Bazhenov A.Y., et al. Random Laser Based on Materials in the Form of Complex Network Structures. JETP Letters, 2023, 117 (11), P. 814–820.</mixed-citation></citation-alternatives></ref><ref id="cit22"><label>22</label><citation-alternatives><mixed-citation xml:lang="ru">Wiersma D.S. Disordered photonics. Nature Photonics, 2013, 7 (3), P. 188–196.</mixed-citation><mixed-citation xml:lang="en">Wiersma D.S. Disordered photonics. Nature Photonics, 2013, 7 (3), P. 188–196.</mixed-citation></citation-alternatives></ref></ref-list><fn-group><fn fn-type="conflict"><p>The authors declare that there are no conflicts of interest present.</p></fn></fn-group></back></article>
