{"title":"在全光纤激光系统中,通过掺镱PCF ROD放大器实现突发模式放大,产生具有飞秒多微束结构的mJ突发能量","authors":"Bappa Karmakar , A. Aryshev , Joydeep Karmakar , Madhuri Aggarwal , B.K. Sahu , P.K. Mukhopadhyay , Subhendu Ghosh , Sunil Kumar","doi":"10.1016/j.optcom.2025.132481","DOIUrl":null,"url":null,"abstract":"<div><div>We report generation of burst-mode infrared pulses (1030 nm) with a total energy of approximately 3 mJ, achieved using chirped pulse amplification (CPA) in Yb-doped photonic crystal fiber (PCF) rod amplifiers, seeded with a multi-microbunch pulse structure. The individual pulse energy within the burst ranged from ∼111 μJ (maximum) to ∼14 μJ (minimum). These pulses were successfully compressed to an estimated pulse width of ∼335 fs using a grating-based compressor. The seed source was an in-house developed Yb-doped fiber oscillator, passively mode-locked at 130 MHz using the nonlinear polarization rotation (NPR) technique. A commercial semiconductor optical amplifier (SOA) was employed as a high-efficiency pulse picker, enabling the selection of user-defined multi-micro pulse structures within a 4 μs time window at a 10 Hz burst repetition rate representing a three-time scale burst pulses. The selected pulse structure was amplified through multiple stages, culminating in two Yb-doped PCF rod amplifiers. Through optimization of the pulsed pump configuration, we maximized the gain for the leading pulses within the burst train. The resulting output comprised a multi-MHz repetition rate pulse train with the central lobe compressed to pulse width of ∼335 fs and peak individual pulse energy of <em>∼</em>111 ± 4 μJ, contributing to a total burst energy of ∼3.1 ± 0.09 mJ. These high-energy, ultrafast burst pulses are currently being utilized to generate high-current electron bursts from photocathode in the Delhi Light Source (DLS), a pre-bunched free electron laser facility under development at IUAC, New Delhi.</div></div>","PeriodicalId":19586,"journal":{"name":"Optics Communications","volume":"596 ","pages":"Article 132481"},"PeriodicalIF":2.5000,"publicationDate":"2025-09-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Burst mode amplification through Yb doped PCF ROD amplifier to generate mJ burst energy with femtosecond multi-micro bunch structure in all fiber laser system\",\"authors\":\"Bappa Karmakar , A. Aryshev , Joydeep Karmakar , Madhuri Aggarwal , B.K. Sahu , P.K. Mukhopadhyay , Subhendu Ghosh , Sunil Kumar\",\"doi\":\"10.1016/j.optcom.2025.132481\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We report generation of burst-mode infrared pulses (1030 nm) with a total energy of approximately 3 mJ, achieved using chirped pulse amplification (CPA) in Yb-doped photonic crystal fiber (PCF) rod amplifiers, seeded with a multi-microbunch pulse structure. The individual pulse energy within the burst ranged from ∼111 μJ (maximum) to ∼14 μJ (minimum). These pulses were successfully compressed to an estimated pulse width of ∼335 fs using a grating-based compressor. The seed source was an in-house developed Yb-doped fiber oscillator, passively mode-locked at 130 MHz using the nonlinear polarization rotation (NPR) technique. A commercial semiconductor optical amplifier (SOA) was employed as a high-efficiency pulse picker, enabling the selection of user-defined multi-micro pulse structures within a 4 μs time window at a 10 Hz burst repetition rate representing a three-time scale burst pulses. The selected pulse structure was amplified through multiple stages, culminating in two Yb-doped PCF rod amplifiers. Through optimization of the pulsed pump configuration, we maximized the gain for the leading pulses within the burst train. The resulting output comprised a multi-MHz repetition rate pulse train with the central lobe compressed to pulse width of ∼335 fs and peak individual pulse energy of <em>∼</em>111 ± 4 μJ, contributing to a total burst energy of ∼3.1 ± 0.09 mJ. These high-energy, ultrafast burst pulses are currently being utilized to generate high-current electron bursts from photocathode in the Delhi Light Source (DLS), a pre-bunched free electron laser facility under development at IUAC, New Delhi.</div></div>\",\"PeriodicalId\":19586,\"journal\":{\"name\":\"Optics Communications\",\"volume\":\"596 \",\"pages\":\"Article 132481\"},\"PeriodicalIF\":2.5000,\"publicationDate\":\"2025-09-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Optics Communications\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0030401825010090\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optics Communications","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0030401825010090","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"OPTICS","Score":null,"Total":0}
Burst mode amplification through Yb doped PCF ROD amplifier to generate mJ burst energy with femtosecond multi-micro bunch structure in all fiber laser system
We report generation of burst-mode infrared pulses (1030 nm) with a total energy of approximately 3 mJ, achieved using chirped pulse amplification (CPA) in Yb-doped photonic crystal fiber (PCF) rod amplifiers, seeded with a multi-microbunch pulse structure. The individual pulse energy within the burst ranged from ∼111 μJ (maximum) to ∼14 μJ (minimum). These pulses were successfully compressed to an estimated pulse width of ∼335 fs using a grating-based compressor. The seed source was an in-house developed Yb-doped fiber oscillator, passively mode-locked at 130 MHz using the nonlinear polarization rotation (NPR) technique. A commercial semiconductor optical amplifier (SOA) was employed as a high-efficiency pulse picker, enabling the selection of user-defined multi-micro pulse structures within a 4 μs time window at a 10 Hz burst repetition rate representing a three-time scale burst pulses. The selected pulse structure was amplified through multiple stages, culminating in two Yb-doped PCF rod amplifiers. Through optimization of the pulsed pump configuration, we maximized the gain for the leading pulses within the burst train. The resulting output comprised a multi-MHz repetition rate pulse train with the central lobe compressed to pulse width of ∼335 fs and peak individual pulse energy of ∼111 ± 4 μJ, contributing to a total burst energy of ∼3.1 ± 0.09 mJ. These high-energy, ultrafast burst pulses are currently being utilized to generate high-current electron bursts from photocathode in the Delhi Light Source (DLS), a pre-bunched free electron laser facility under development at IUAC, New Delhi.
期刊介绍:
Optics Communications invites original and timely contributions containing new results in various fields of optics and photonics. The journal considers theoretical and experimental research in areas ranging from the fundamental properties of light to technological applications. Topics covered include classical and quantum optics, optical physics and light-matter interactions, lasers, imaging, guided-wave optics and optical information processing. Manuscripts should offer clear evidence of novelty and significance. Papers concentrating on mathematical and computational issues, with limited connection to optics, are not suitable for publication in the Journal. Similarly, small technical advances, or papers concerned only with engineering applications or issues of materials science fall outside the journal scope.