High Power Laser Science and Engineering, Volume. 7, Issue 1, 010000e6(2019)

Study of backward terahertz radiation from intense picosecond laser–solid interactions using a multichannel calorimeter system On the Cover

H. Liu1,6, G.-Q. Liao2, Y.-H. Zhang1,6, B.-J. Zhu1,6, Z. Zhang1, Y.-T. Li1,6,7, G. G. Scott3, D. Rusby3,4, C. Armstrong3,4, E. Zemaityte3,4, P. Bradford5, N. Woolsey5, P. Huggard8, P. McKenna4, and D. Neely3,4、†,*
Author Affiliations
  • 1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2Key Laboratory for Laser Plasmas (MoE) and School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 3Central Laser Facility, Rutherford Appleton Laboratory, Didcot, Oxfordshire OX11 0QX, UK
  • 4Department of Physics, SUPA, University of Strathclyde, Glasgow G4 0NG, UK
  • 5Department of Physics, York Plasma Institute, University of York, Heslington, York YO10 5DD, UK
  • 6School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
  • 7Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai 200240, China
  • 8Space Science Department, STFC Rutherford Appleton Laboratory, Didcot OX11 0QX, UK
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    Figures & Tables(7)
    Schematic layout of eight-channel THz calorimeter system.
    Linear response of the detector to energy of near-infrared and THz wavelengths.
    (a) Experimental setup of THz radiation spectrum measurement in ultra-intense laser–plasma interaction experiment. (b) Spectral sensitivity of the multichannel calorimeter system.
    (a) The measured BTR energy from a $5~\unicode[STIX]{x03BC}\text{m}$ copper target as a function of the pump laser energy. (b) The measured BTR spectrum with driven laser energy on target varying from 14 J to 54 J from a $5~\unicode[STIX]{x03BC}\text{m}$ copper target.
    (a) The measured BTR energy as a function of copper foil target thickness. (b) The measured BTR spectrum with copper foil target thickness varying from $1~\unicode[STIX]{x03BC}\text{m}$ to $100~\unicode[STIX]{x03BC}\text{m}$.
    (a) The measured BTR energy from a $100~\unicode[STIX]{x03BC}\text{m}$ copper target as a function of delay between pre-pulse and main pulse. (b) The measured BTR spectrum from a $100~\unicode[STIX]{x03BC}\text{m}$ copper target with different delays between pre-pulse and main pulse, no pre-pulse, 400 ps and 1000 ps, respectively.
    • Table 1. Factors for the spectral sensitivity of the multichannel system.

      View table
      View in Article

      Table 1. Factors for the spectral sensitivity of the multichannel system.

      10.5 0.8 0.80.1140.950.66
      2 1 0.8 0.80.1340.780.80
      31.5 0.8 0.80.0970.850.85
      4 30.810.810.1340.800.91
      5 6 0.7 0.70.1570.900.95
      610 0.6 0.60.1340.900.95
      7200.690.690.1140.880.95
      80.116
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    H. Liu, G.-Q. Liao, Y.-H. Zhang, B.-J. Zhu, Z. Zhang, Y.-T. Li, G. G. Scott, D. Rusby, C. Armstrong, E. Zemaityte, P. Bradford, N. Woolsey, P. Huggard, P. McKenna, D. Neely. Study of backward terahertz radiation from intense picosecond laser–solid interactions using a multichannel calorimeter system[J]. High Power Laser Science and Engineering, 2019, 7(1): 010000e6

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    Paper Information

    Special Issue: HIGH ENERGY DENSITY PHYSICS AND HIGH POWER LASERS

    Received: Jul. 22, 2018

    Accepted: Nov. 13, 2018

    Published Online: Mar. 26, 2019

    The Author Email: D. Neely (david.neely@stfc.ac.uk)

    DOI:10.1017/hpl.2018.60

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