• Photonics Research
  • Vol. 4, Issue 3, 0A22 (2016)
Tianwu Wang1, Elena A. Romanova2, Nabil Abdel-Moneim3, David Furniss3, Anna Loth3, Zhuoqi Tang3, Angela Seddon3, Trevor Benson3, Andrei Lavrinenko1, and Peter Uhd Jepsen1、*
Author Affiliations
  • 1Department of Photonics Engineering (DTU Fotonik), Technical University of Denmark, DK-2800 Kgs. Lyngby, Denmark
  • 2Saratov State University, Department of Physics, Astrakhanskaya 83, Saratov 410012, Russia
  • 3Faculty of Engineering, University of Nottingham, University Park, Nottingham NG7 2RD, UK
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    DOI: 10.1364/prj.4.000a22 Cite this Article Set citation alerts
    Tianwu Wang, Elena A. Romanova, Nabil Abdel-Moneim, David Furniss, Anna Loth, Zhuoqi Tang, Angela Seddon, Trevor Benson, Andrei Lavrinenko, Peter Uhd Jepsen. Time-resolved terahertz spectroscopy of charge carrier dynamics in the chalcogenide glass As30Se30Te40 [Invited][J]. Photonics Research, 2016, 4(3): 0A22 Copy Citation Text show less

    Abstract

    Broadband (1.6–18 THz) terahertz time-domain spectroscopy (THz-TDS) and time-resolved terahertz spectroscopy (TRTS) were performed on a 54 μm thick chalcogenide glass (As30Se30Te40) sample with a two-color laser-induced air plasma THz system in transmission and reflection modes, respectively. Two absorption bands at 2–3 and 5–8 THz were observed. TRTS reveals an ultrafast relaxation process of the photoinduced carrier response, well described by a rate equation model with a finite concentration of mid-bandgap trap states for self-trapped excitons. The photoinduced conductivity can be well described by the Drude–Smith conductivity model with a carrier scattering time of 12–17 fs, and we observe significant carrier localization effects. A fast refractive index change was observed 100 fs before the conductivity reached its maximum, with 2 orders of magnitude larger amplitude than expected for the optically induced THz Kerr effect, indicating that free carriers are responsible for the transient index change.
    ϵ(ω)=ϵ+A1ω12ω2iγ1ω+A2ω22ω2iγ2ω,(1)

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    Δr˜(ω,tpp)=(1r˜0r˜0)Z0dσ˜(ω,tpp)1+n+Z0dσ˜(ω,tpp),(2)

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    Δσ(tpp)=Δr·n212Z0d,(3)

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    N˙he=σ1I(t)γcoolNhe,N˙e=γcoolNheσcNe(NtrapNte),N˙te=σcNe(NtrapNte),N˙th=γthNh,N˙h=γcoolNhhγthNh,N˙hh=σ1I(t)γcoolNhh,(4)

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    Δσ(t)Ne(t)/me*+Nte(t)/mte*.(5)

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    σ(ω)=ωp2ϵ0τ1iωτ(1+c1iωτ),(6)

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    Tianwu Wang, Elena A. Romanova, Nabil Abdel-Moneim, David Furniss, Anna Loth, Zhuoqi Tang, Angela Seddon, Trevor Benson, Andrei Lavrinenko, Peter Uhd Jepsen. Time-resolved terahertz spectroscopy of charge carrier dynamics in the chalcogenide glass As30Se30Te40 [Invited][J]. Photonics Research, 2016, 4(3): 0A22
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