2010
DOI: 10.1021/ic902524u
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Spectroscopic and Structural Studies of Difluorophosphoryl Azide F2P(O)N3, Difluorophosphoryl Isocyanate F2P(O)NCO, and Difluorophosphoric Acid Anhydride, F2(O)POP(O)F2

Abstract: Difluorophosphoryl azide, F(2)P(O)N(3), was fully characterized by (19)F, (31)P, (14)N, and (15)N NMR, as well as by IR (gas, Ar-matrix), and Raman (liquid, solid) spectroscopy. For comparison the vibrational spectra of the isoelectronic difluorophosphoryl isocyanate, F(2)P(O)NCO was also studied. Both molecules were found to exist as single rotamers in the gas, liquid, and solid states. Their solid-state structures were determined by X-ray crystallography as the rotamers with the P=O bond being cis to the pse… Show more

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Cited by 21 publications
(20 citation statements)
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“…In the IR spectra, the observed strongest bands at 2290 cm –1 (gas phase) and 2288.6 cm –1 (Ne matrix), belong to the antisymmetric stretching vibration of the NCO group [ν as (NCO)], which appears as a very weak band at 2283 cm –1 in the Raman spectrum. The band position is red‐shifted comparing to that of F 2 P(O)NCO (gas‐phase IR: 2309 cm –1 , Ar matrix IR: 2306.9 cm –1 , liquid Raman: 2307 cm –1 ), but it is blue‐shifted compared to that of OP(NCO) 3 (liquid IR: 2265 cm –1 ) . These shifts coincide with the electronegativity order F > Cl > NCO.…”
Section: Resultsmentioning
confidence: 81%
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“…In the IR spectra, the observed strongest bands at 2290 cm –1 (gas phase) and 2288.6 cm –1 (Ne matrix), belong to the antisymmetric stretching vibration of the NCO group [ν as (NCO)], which appears as a very weak band at 2283 cm –1 in the Raman spectrum. The band position is red‐shifted comparing to that of F 2 P(O)NCO (gas‐phase IR: 2309 cm –1 , Ar matrix IR: 2306.9 cm –1 , liquid Raman: 2307 cm –1 ), but it is blue‐shifted compared to that of OP(NCO) 3 (liquid IR: 2265 cm –1 ) . These shifts coincide with the electronegativity order F > Cl > NCO.…”
Section: Resultsmentioning
confidence: 81%
“…It is noteworthy that in the Raman spectrum of the liquid the P=O stretching vibration shifts to 1292 cm –1 , indicating the presence of intermolecular interactions including the phosphoryl oxygen atom in the condensed phase. The P–N stretching vibration (νPN) in Cl 2 P(O)NCO (747.1 cm –1 , Ne matrix) is slightly lower in frequency than that in F 2 P(O)NCO (751.8 cm –1 , Ar matrix) . The in‐plane and out‐of‐plane deformation modes of the NCO group in the Ne matrix are observed at 629.7 and 611.5 cm –1 , and the asymmetric and symmetric stretching vibrations of the ClPCl units in the liquid state occur at 597 and 517 cm –1 , respectively.…”
Section: Resultsmentioning
confidence: 96%
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“…The structure of F 2 P(O)N 3 in the solid state occupies C s symmetry within the error range. [14] Concerning the geometrical parameters of the isocyanate group the NÀ C and CÀ O lengths are the same within error limits for the isocyanates bound to a phosphorus atom in the formal oxidation state + V. However, in the phosphorus(III) isocyanate Cl 2 PNCO [11] the NÀ C [b] ∡(NCO) [b] ∡(YÀ PÀ Y) [a] Distances r in Å, angles and dihedral angles in deg. [b] For the azides the analogous parameters are given.…”
Section: Solid-state Structurementioning
confidence: 99%