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Chalcogenide-halides of niobium (V). 1. Gas-phase structures of NbOBr3, NbSBr3, and NbSCl3. 2. Matrix infrared spectra and vibrational force fields of NbOBr3, NbSBr3, NbSCl3, and NbOCl3

Chalcogenide-halides of niobium (V). 1. Gas-phase structures of NbOBr3, NbSBr3, and NbSCl3. 2. Matrix infrared spectra and vibrational force fields of NbOBr3, NbSBr3, NbSCl3, and NbOCl3
Chalcogenide-halides of niobium (V). 1. Gas-phase structures of NbOBr3, NbSBr3, and NbSCl3. 2. Matrix infrared spectra and vibrational force fields of NbOBr3, NbSBr3, NbSCl3, and NbOCl3
The molecular structures of NbOBr3, NbSCl3, and NbSBr3 have been determined by gas-phase electron diffraction (GED) at nozzle-tip temperatures of 250 degreesC, taking into account the possible presence of NbOCl3 as a contaminant in the NbSCl3 sample and NbOBr3 in the NbSBr3 sample. The experimental data are consistent with trigonal-pyramidal molecules having C-3v symmetry. Infrared spectra of molecules trapped in argon or nitrogen matrices were recorded and exhibit the characteristic fundamental stretching modes for C-3v species. Well resolved isotopic fine structure (Cl-35 and Cl-37) was observed for NbSCl3, and for NbOCl3 which occurred as an impurity in the NbSCl3 spectra. Quantum mechanical calculations of the structures and vibrational frequencies of the four YNbX3 molecules (Y = O, S; X = Cl, Br) were carried out at several levels of theory, most importantly B3LYP DFT with either the Stuttgart RSC ECP or Hay-Wadt (n + 1) ECP VDZ basis set for Nb and the 6-311 G* basis set for the nonmetal atoms. Theoretical values for the bond lengths are 0.01-0.04 Angstrom longer than the experimental ones of type r(a), in accord with general experience, but the bond angles with theoretical minus experimental differences of only 1.0-1.5degrees are notably accurate. Symmetrized force fields were also calculated. The experimental bond lengths (r(g)/Angstrom) and angles (angle(alpha)/deg) with estimated 2sigma uncertainties from GED are as follows. NbOBr3: r(Nb=O) = 1.694(7), r(Nb-Br) = 2.429(2), angle(O=Nb-Br) = 107.3(5), angle(Br-Nb-Br) = 111.5(5). NbSBr3: r(Nb=S) = 2.134(10), r(Nb-Br) = 2.408(4), angle(S=Nb-Br) = 106.6(7), angle(Br-Nb-Br) = 112.2(6). NbSCl3: Nb=S) = 2.120(10), r(Nb-Cl) = 2.271(6), angle(S=Nb-Cl) = 107.8(12), angle(Cl-Nb-Cl) = 111.1(11).
electron-diffraction, molecular-structure, tetrahydrothiophene tht, crystal
0020-1669
1296-1305
Nowak, Izabela
c9bcbba8-2462-4fc8-8e0d-fc23a2068dbc
Page, Elizabeth M.
2cf990e9-fa42-4e86-99bb-52d19797e85c
Rice, David A.
93617f71-33ff-4bc6-8f4c-ed2b74467e52
Richardson, Alan D.
57a0569b-02fb-4d58-a86c-bbc8b8e38399
French, Richard J.
5c812f5d-6f7b-41da-a1b4-7aa73fcd9ca8
Hedberg, Kenneth
1d7a62a1-cda6-4d5d-b3ff-3ca281cd9f8b
Ogden, J. Steven
5a99fd42-75e7-4f7b-a347-ac2b1717b8b3
Nowak, Izabela
c9bcbba8-2462-4fc8-8e0d-fc23a2068dbc
Page, Elizabeth M.
2cf990e9-fa42-4e86-99bb-52d19797e85c
Rice, David A.
93617f71-33ff-4bc6-8f4c-ed2b74467e52
Richardson, Alan D.
57a0569b-02fb-4d58-a86c-bbc8b8e38399
French, Richard J.
5c812f5d-6f7b-41da-a1b4-7aa73fcd9ca8
Hedberg, Kenneth
1d7a62a1-cda6-4d5d-b3ff-3ca281cd9f8b
Ogden, J. Steven
5a99fd42-75e7-4f7b-a347-ac2b1717b8b3

Nowak, Izabela, Page, Elizabeth M., Rice, David A., Richardson, Alan D., French, Richard J., Hedberg, Kenneth and Ogden, J. Steven (2003) Chalcogenide-halides of niobium (V). 1. Gas-phase structures of NbOBr3, NbSBr3, and NbSCl3. 2. Matrix infrared spectra and vibrational force fields of NbOBr3, NbSBr3, NbSCl3, and NbOCl3. Inorganic Chemistry, 42 (4), 1296-1305. (doi:10.1021/ic020405f).

Record type: Article

Abstract

The molecular structures of NbOBr3, NbSCl3, and NbSBr3 have been determined by gas-phase electron diffraction (GED) at nozzle-tip temperatures of 250 degreesC, taking into account the possible presence of NbOCl3 as a contaminant in the NbSCl3 sample and NbOBr3 in the NbSBr3 sample. The experimental data are consistent with trigonal-pyramidal molecules having C-3v symmetry. Infrared spectra of molecules trapped in argon or nitrogen matrices were recorded and exhibit the characteristic fundamental stretching modes for C-3v species. Well resolved isotopic fine structure (Cl-35 and Cl-37) was observed for NbSCl3, and for NbOCl3 which occurred as an impurity in the NbSCl3 spectra. Quantum mechanical calculations of the structures and vibrational frequencies of the four YNbX3 molecules (Y = O, S; X = Cl, Br) were carried out at several levels of theory, most importantly B3LYP DFT with either the Stuttgart RSC ECP or Hay-Wadt (n + 1) ECP VDZ basis set for Nb and the 6-311 G* basis set for the nonmetal atoms. Theoretical values for the bond lengths are 0.01-0.04 Angstrom longer than the experimental ones of type r(a), in accord with general experience, but the bond angles with theoretical minus experimental differences of only 1.0-1.5degrees are notably accurate. Symmetrized force fields were also calculated. The experimental bond lengths (r(g)/Angstrom) and angles (angle(alpha)/deg) with estimated 2sigma uncertainties from GED are as follows. NbOBr3: r(Nb=O) = 1.694(7), r(Nb-Br) = 2.429(2), angle(O=Nb-Br) = 107.3(5), angle(Br-Nb-Br) = 111.5(5). NbSBr3: r(Nb=S) = 2.134(10), r(Nb-Br) = 2.408(4), angle(S=Nb-Br) = 106.6(7), angle(Br-Nb-Br) = 112.2(6). NbSCl3: Nb=S) = 2.120(10), r(Nb-Cl) = 2.271(6), angle(S=Nb-Cl) = 107.8(12), angle(Cl-Nb-Cl) = 111.1(11).

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Published date: 24 February 2003
Keywords: electron-diffraction, molecular-structure, tetrahydrothiophene tht, crystal

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Local EPrints ID: 20054
URI: http://eprints.soton.ac.uk/id/eprint/20054
ISSN: 0020-1669
PURE UUID: 12a6aaeb-a325-466c-b725-8eac39386781

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Date deposited: 24 Feb 2006
Last modified: 15 Mar 2024 06:21

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Contributors

Author: Izabela Nowak
Author: Elizabeth M. Page
Author: David A. Rice
Author: Alan D. Richardson
Author: Richard J. French
Author: Kenneth Hedberg
Author: J. Steven Ogden

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