14N Nuclear Quadrupole Hyperfine Structure in the Rotational Spectrum of Thionyl Aniline

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Authors

  • N. Heineking
  • J. U. Grabow
  • K. Vormann
  • W. Stahl

External Research Organisations

  • Kiel University
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Details

Original languageEnglish
Pages (from-to)989-992
Number of pages4
JournalZeitschrift fur Naturforschung - Section A Journal of Physical Sciences
Volume46
Issue number11
Publication statusPublished - 1 Nov 1991
Externally publishedYes

Abstract

Nuclear quadrupole hyperfine structures have been resolved in the rotational spectrum of thionyl aniline, C6H5NSO, using pulsed molecular beam microwave Fourier transform spectroscopy. High precision nuclear quadrupole coupling constants, rotational and quartic centrifugal distortion constants have been determined from the analysis of 12 low-J transitions. Coupling constants are ϰaa= +1.5730(14) MHz and (ϰbb-ϰcc)=—5.6499(13) MHz, rotational constants are A =4026.72i5(4) MHz, B = 860.64732(8) MHz, and C = 709.52027(7) MHz, and centrifugal distortion constants are Δj = 36.6(5) Hz,Δ JK = - 107.5 (20) Hz, ΔK = 703(68) Hz, δj, = 8.1 (5) Hz, and δK= 111 (19) Hz (representation I rused).

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Cite this

14N Nuclear Quadrupole Hyperfine Structure in the Rotational Spectrum of Thionyl Aniline. / Heineking, N.; Grabow, J. U.; Vormann, K. et al.
In: Zeitschrift fur Naturforschung - Section A Journal of Physical Sciences, Vol. 46, No. 11, 01.11.1991, p. 989-992.

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abstract = "Nuclear quadrupole hyperfine structures have been resolved in the rotational spectrum of thionyl aniline, C6H5NSO, using pulsed molecular beam microwave Fourier transform spectroscopy. High precision nuclear quadrupole coupling constants, rotational and quartic centrifugal distortion constants have been determined from the analysis of 12 low-J transitions. Coupling constants are ϰaa= +1.5730(14) MHz and (ϰbb-ϰcc)=—5.6499(13) MHz, rotational constants are A =4026.72i5(4) MHz, B = 860.64732(8) MHz, and C = 709.52027(7) MHz, and centrifugal distortion constants are Δj = 36.6(5) Hz,Δ JK = - 107.5 (20) Hz, ΔK = 703(68) Hz, δj, = 8.1 (5) Hz, and δK= 111 (19) Hz (representation I rused).",
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Download

TY - JOUR

T1 - 14N Nuclear Quadrupole Hyperfine Structure in the Rotational Spectrum of Thionyl Aniline

AU - Heineking, N.

AU - Grabow, J. U.

AU - Vormann, K.

AU - Stahl, W.

PY - 1991/11/1

Y1 - 1991/11/1

N2 - Nuclear quadrupole hyperfine structures have been resolved in the rotational spectrum of thionyl aniline, C6H5NSO, using pulsed molecular beam microwave Fourier transform spectroscopy. High precision nuclear quadrupole coupling constants, rotational and quartic centrifugal distortion constants have been determined from the analysis of 12 low-J transitions. Coupling constants are ϰaa= +1.5730(14) MHz and (ϰbb-ϰcc)=—5.6499(13) MHz, rotational constants are A =4026.72i5(4) MHz, B = 860.64732(8) MHz, and C = 709.52027(7) MHz, and centrifugal distortion constants are Δj = 36.6(5) Hz,Δ JK = - 107.5 (20) Hz, ΔK = 703(68) Hz, δj, = 8.1 (5) Hz, and δK= 111 (19) Hz (representation I rused).

AB - Nuclear quadrupole hyperfine structures have been resolved in the rotational spectrum of thionyl aniline, C6H5NSO, using pulsed molecular beam microwave Fourier transform spectroscopy. High precision nuclear quadrupole coupling constants, rotational and quartic centrifugal distortion constants have been determined from the analysis of 12 low-J transitions. Coupling constants are ϰaa= +1.5730(14) MHz and (ϰbb-ϰcc)=—5.6499(13) MHz, rotational constants are A =4026.72i5(4) MHz, B = 860.64732(8) MHz, and C = 709.52027(7) MHz, and centrifugal distortion constants are Δj = 36.6(5) Hz,Δ JK = - 107.5 (20) Hz, ΔK = 703(68) Hz, δj, = 8.1 (5) Hz, and δK= 111 (19) Hz (representation I rused).

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