Rudolph Wolfram W, Fischer Dieter, Irmer Gert
Department of Hospital Infection Control, Technical University Dresden, Universitätsklinikum Carl Gustav Carus Dresden, Dresden, Germany.
Institute of Polymer Research Dresden, Dresden, Germany.
Appl Spectrosc. 2021 Apr;75(4):395-411. doi: 10.1177/0003702820986861. Epub 2021 Jan 19.
Qualitative and quantitative Raman and infrared measurements on sodium nitrate (NaNO) solutions have been carried out over a wide concentration range (5.56 × 10-7.946 mol/L) in water and heavy water. The Raman spectra were measured from 4000 cm to low wavenumbers at 45 cm. Band fit analysis on the profile of the 1047 cm band, ν(a) measured at high resolution at 0.90 cm produced a small contribution at 1027 cm of the isotopomer NOO(aq). The effect of solute concentration on the Raman and infrared bands has been systematically recorded. Extrapolation of the experimental data resulted in values for all the nitrate bands of the "free", i.e., fully hydrated (aq). However, even in dilute solutions, the vibrational symmetry of the hydrated (aq) is broken and the antisymmetric N-O stretch, which is degenerate for the isolated anion, is split by 56 cm. At concentrations >2.5 mol/L, direct contact between Na and was observed and accompanied by large band parameter changes. DFT calculations on (HO) ( = 1-3) led to optimized geometries and vibrational frequencies which reproduced the measured ones within an accuracy of 1%. A hydrated gas phase species Na(HO) was optimized resulting in the geometry and symmetry of the nitrate, which is bound in an antisymmetric bidentate fashion with the nitrate possessing C. The ν Na(OH) breathing mode in aqueous solution appears at 189 cm, whereas in heavy water, ν Na(OD) is shifted to 175.6 cm due to the isotope effect. DFT calculations on hydrated Na(OH) gas phase clusters provided realistic Na hydrate structures with = 4 and 5, which resembled the measured frequency of ν Na OH mode quite well. Quantitative Raman analysis employing the symmetric stretching band, ν(a) , has been carried out down to concentrations as low as 5.56 × 10mol/L. The in-plane deformation mode ν(e') in the Raman scattering at higher concentrations has been used as an indicator band for directly coordinated .
在水和重水中,对硝酸钠(NaNO₃)溶液进行了定性和定量的拉曼光谱及红外光谱测量,测量浓度范围很广(5.56×10⁻⁷.⁹⁴⁶ mol/L)。拉曼光谱在4000 cm⁻¹至低波数范围以45 cm⁻¹的分辨率进行测量。对在0.90 cm⁻¹高分辨率下测量的1047 cm⁻¹谱带(ν(a))轮廓进行谱带拟合分析,结果表明,同位素异构体NO₃⁻(aq)在1027 cm⁻¹处有一小贡献。系统记录了溶质浓度对拉曼光谱和红外光谱谱带的影响。对实验数据进行外推,得到了“自由”即完全水合(aq)的所有硝酸根谱带的值。然而,即使在稀溶液中,水合(aq)的振动对称性也会被打破,孤立阴离子简并的反对称N - O伸缩振动会分裂56 cm⁻¹。在浓度>2.5 mol/L时,观察到Na⁺与NO₃⁻之间的直接接触,并伴有谱带参数的大幅变化。对(H₂O)ₙ(n = 1 - 3)进行密度泛函理论(DFT)计算,得到了优化的几何结构和振动频率,其与测量值的重现精度在1%以内。对水合气相物种Na⁺(H₂O)ₙ进行优化,得到了硝酸根的几何结构和对称性,硝酸根以反对称双齿方式结合,具有C₂ᵥ对称性。水溶液中ν Na⁺(OH₂)的呼吸模式出现在189 cm⁻¹处,而在重水中,由于同位素效应,ν Na⁺(OD₂)移至175.6 cm⁻¹。对水合Na⁺(OH₂)气相团簇进行DFT计算,得到了n = 4和5时逼真的Na⁺水合物结构,其与测量的ν Na⁺ OH模式频率相当吻合。采用对称伸缩谱带ν(a)进行定量拉曼分析,测量浓度低至5.56×10⁻⁷ mol/L。在较高浓度下,拉曼散射中的面内变形模式ν(e')被用作直接配位的指示谱带。