Impact factor of Chinese Physics C is 3.6 in 2023 Impact factor of Chinese Physics C is 3.6 in 2022 2021 Impact Factor 2.944
Advanced Search
×
近期发现有不法分子冒充我刊与作者联系，借此进行欺诈等不法行为，请广大作者加以鉴别，如遇诈骗行为，请第一时间与我刊编辑部联系确认（《中国物理C》（英文）编辑部电话：010-88235947,010-88236950），并作报警处理。
本刊再次郑重声明：
（1）本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
（2）本刊采编系统作者中心是投稿的唯一路径，该系统为ScholarOne远程稿件采编系统，仅在本刊投稿网网址（https://mc03.manuscriptcentral.com/cpc）设有登录入口。本刊不接受其他方式的投稿，如打印稿投稿、E-mail信箱投稿等，若以此种方式接收投稿均为假冒。
（3）所有投稿均需经过严格的同行评议、编辑加工后方可发表，本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿，并收取发表费用，均为假冒。
                  
《中国物理C》（英文）编辑部
2024年10月30日
Chinese Physics C> 2017, Vol. 41> Issue(10) : 108101 DOI: 10.1088/1674-1137/41/10/108101

Effect of cavity length detuning on the output characteristics for the middle infrared FEL oscillator of FELiChEM

  • 1.

     National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230029, China

  • FELiChEM is an infrared free electron laser (FEL) facility currently under construction, which consists of two oscillators generating middle-infrared and far-infrared laser covering the spectral range of 2.5-200 μm. In this paper, we numerically study the output characteristics of the middle-infrared oscillator with accurate cavity length detuning. Emphasis is put on the temporal structure of the micropulse and the corresponding spectral bandwidth. Taking the radiation wavelengths of 50 μm and 5 μm as examples, we show that the output pulse duration can be tuned in the range of 1-6 ps with corresponding bandwidth of 13%-0.2% by adjusting the cavity length detuning. In addition, a special discussion on the comb structure is presented, and it is indicated that the comb structure may arise in the output optical pulse when the normalized slippage length is much smaller than unity. This work has reference value for the operation of FELiChEM and other FEL oscillators.
      PCAS:
  • 加载中

  • References

    [1] P. Emma et al, Nat. Photon., 4:641(2010)
    [2] E. Allaria et al, J. Synchrotron Rad., 22:485(2015)
    [3] DENG Hai-Xiao et al, Chinese Physics C, 38:028101(2014)
    [4] J. M. Ortega, Nucl. Instrum. Methods A, 341:138(1994)
    [5] N. Vinokurov, J. of IRMMTHz Waves, 32:1123(2011)
    [6] L. Giannessi et al, Phys. Rev. Lett., 106.14:144801(2011)
    [7] Z. T. Zhao et al, Nature Photonics, 6 (6):360-363(2012)
    [8] J. M. Ortega, M. Bergher, R. Chaput et al, Nucl. Instrum. Methods A, 285:97-103(1989)
    [9] W. Schollkopf et al, First lasing of the IR FEL at the FritzHaber Institut, Berlin. Proc. of FEL Conference. Nara, Japan. 2012, p. 1-4
    [10] W. Schollkopf et al, The new IR and THz FEL Facility at the Fritz Haber Institute in Berlin. Proc. of SPIE, 9512:95121L-1(2015)
    [11] P. W. van Amersfoort, R. W. B. Best, R. van Buuren et al, Nucl. Instrum. Methods A, 296:217-221(1990)
    [12] P. W. van Amersfoort, R. J. Bakker, J. B. Bekkers et al, Nucl. Instrum. Methods A, 318:42-46(1992)
    [13] Heting Li, Yalin Lu, Zhigang He, Qika Jia, and Lin Wang, J. of IRMMTHz Waves, 37:649-657(2016)
    [14] Y.-C. Huang, Appl. Phys. Lett., 96:2315039(2010)
    [15] He-Ting Li, Qi-Ka Jia, Shan-Cai Zhang, Lin Wang, and Yong-Liang Yang, Chinese Physics C, 41:018102(2017)
    [16] Kim, Kwang-Je, Phys. Rev. Lett., 66:2746(1991)
    [17] N. Piovella et al, Physical Review E, 52 (5):5470(1995)
    [18] G. Dattoli et al, IEEE J. Quantum Electron, 17:1371(1981)
    [19] G. Dattoli et al, Journal of Applied Physics, 101:103109(2007)
    [20] P. L. Ottaviani et al, Nucl. Instrum. Methods A, 834:108-117(2016)
    [21] R. Bonifacio et al, J. of IRMMTHz Waves, 28 (9):699-704(2007)
    [22] S. Reiche, Nucl. Instrum. Methods A, 429:243(1999)
    [23] Vander slot P et al, Phys. Rev. Lett., 102:244802(2009)
    [24] W. B. Colson, Nucl. Instrum. Methods A, 250:168-175(1986)
    [25] B. A. Richman, J. M. J. Madey, E. Szamers, Phys. Rev. Lett., 16:1682(1989)
    [26] G. M. H. Knippels et al, Phys. Rev. Lett., 75:1755(1995)

  • Access

    加载中

Get Citation
Zhou-Yu Zhao, He-Ting Li and Qi-Ka Jia. Effect of cavity length detuning on the output characteristics for the middle infrared FEL oscillator of FELiChEM[J]. Chinese Physics C, 2017, 41(10): 108101. doi: 10.1088/1674-1137/41/10/108101
Zhou-Yu Zhao, He-Ting Li and Qi-Ka Jia. Effect of cavity length detuning on the output characteristics for the middle infrared FEL oscillator of FELiChEM[J]. Chinese Physics C, 2017, 41(10): 108101.  doi: 10.1088/1674-1137/41/10/108101 shu
Milestone
Received: 2017-04-06
Revised: 2017-07-05
Fund

    Supported by National Natural Science Foundation of China (21327901, 11205156)

Article Metric

Article Views(1750)
PDF Downloads(37)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Effect of cavity length detuning on the output characteristics for the middle infrared FEL oscillator of FELiChEM

    Corresponding author: He-Ting Li,
  • 1. National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230029, China
  • Received Date: 2017-04-06
  • Accepted Date: 2017-07-05
  • Available Online: 2017-10-05
Fund Project:  Supported by National Natural Science Foundation of China (21327901, 11205156)

Abstract: FELiChEM is an infrared free electron laser (FEL) facility currently under construction, which consists of two oscillators generating middle-infrared and far-infrared laser covering the spectral range of 2.5-200 μm. In this paper, we numerically study the output characteristics of the middle-infrared oscillator with accurate cavity length detuning. Emphasis is put on the temporal structure of the micropulse and the corresponding spectral bandwidth. Taking the radiation wavelengths of 50 μm and 5 μm as examples, we show that the output pulse duration can be tuned in the range of 1-6 ps with corresponding bandwidth of 13%-0.2% by adjusting the cavity length detuning. In addition, a special discussion on the comb structure is presented, and it is indicated that the comb structure may arise in the output optical pulse when the normalized slippage length is much smaller than unity. This work has reference value for the operation of FELiChEM and other FEL oscillators.

    HTML

Reference (26)

目录

Link
IOPScience
SCOAP3
arXiv
Chinese Physical Society
Journal information
Introduction
Editorial Board
Others
Subscribe
Contact us
QQ: 1307685413
Tel: +86-010-88235947
Fax: +86-010-88233126
E-mail: cpc@ihep.ac.cn

  • CPC Website

  • IOP Website

  • CPC WeChat

Copyright © Institute of High Energy Physics, Chinese Academy of Sciences, 19B Yuquan Road, Beijing 100049, China 京ICP备05002789号-1

Supported by: Beijing Renhe Information Technology Co. Ltd  E-mail: info@rhhz.net

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return