• Photonics Research
  • Vol. 4, Issue 3, 00A1 (2016)
Rohit Singh1, Deepu Koshy George2, Chejin Bae3, K. A. Niessen4, and A. G. Markelz4、*
Author Affiliations
  • 1Department of Physics and Astronomy, Depauw University, Greencastle, Indiana 46135, USA
  • 2Department of Physics, Virginia Tech, Virginia 24061, USA
  • 3Department of Electrical Engineering, University at Buffalo, Buffalo, New York 14260, USA
  • 4Department of Physics, University at Buffalo, Buffalo, New York 14260, USA
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    DOI: 10.1364/prj.4.0000a1 Cite this Article Set citation alerts
    Rohit Singh, Deepu Koshy George, Chejin Bae, K. A. Niessen, A. G. Markelz. Modulated orientation-sensitive terahertz spectroscopy[J]. Photonics Research, 2016, 4(3): 00A1 Copy Citation Text show less

    Abstract

    Intramolecular vibrations of large macromolecules reside in the terahertz range. In particular, protein vibrations are closely spaced in frequency, resulting in a nearly continuous vibrational density of states. This density of vibrations interferes with the identification of specific absorption lines and their subsequent association with specific functional motions. This challenge is compounded with the absorption being dominated by the solvent and local relaxational motions. A strategy for removing the isotropic relaxational loss and isolating specific vibrations is to use aligned samples and polarization-sensitive measurements. Here, we demonstrate a technique to rapidlyattain the anisotropic resonant absorbance using terahertz time domain spectroscopy and a spinning sample. The technique, modulated orientation-sensitive terahertz spectroscopy (MOSTS), has a nonzero signal only for anisotropic samples, as demonstrated by a comparison between a silicon wafer and a wire grid polarizer. For sucroseand oxalic acid molecular crystals, the MOSTS response is in agreement with modeled results for the intermolecular vibrations. Further, we demonstrate that, even in the presence of a large relaxational background, MOSTS isolates underlying vibrational resonances.
    abs(θ)=absisotropic+jγj2/vj(vvj)2+γj2[(p⃗qj)·λ(θ)]2,(1)

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    Eout=(1000)(cosθsinθsinθcosθ)×(ei2πνdϵo(ν)00ei2πνdϵe(ν))(cosθsinθsinθcosθ)(Ei0).(2)

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    Eout=Ei2((ei2πνdϵo(ν)ei2πνdϵe(ν))cos(2ωt)+(ei2πνdϵo(ν)+ei2πνdϵe(ν))0).(3)

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    EMOSTSEi2(ei2πνdϵo(ν)ei2πνdϵe(ν)).(4)

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    ϵo(e)(ν)=ϵo(e),+jAo(e),jνo(e),j2ν2i(νγo(e),j/2π)(5)

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    Rohit Singh, Deepu Koshy George, Chejin Bae, K. A. Niessen, A. G. Markelz. Modulated orientation-sensitive terahertz spectroscopy[J]. Photonics Research, 2016, 4(3): 00A1
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