Repulsion forces in vibrational spectroscopy—I. Spectral shifts in vibrational spectra of condensed media caused by repulsion forces

1992 ◽  
Vol 48 (6) ◽  
pp. 861-866 ◽  
Author(s):  
Sviatoslav A. Kirillov
2019 ◽  
Vol 10 (1) ◽  
Author(s):  
Kazuki Hashimoto ◽  
Venkata Ramaiah Badarla ◽  
Akira Kawai ◽  
Takuro Ideguchi

Abstract Vibrational spectroscopy, comprised of infrared absorption and Raman scattering spectroscopy, is widely used for label-free optical sensing and imaging in various scientific and industrial fields. The two molecular spectroscopy methods are sensitive to different types of vibrations and provide complementary vibrational spectra, but obtaining complete vibrational information with a single spectroscopic device is challenging due to the large wavelength discrepancy between the two methods. Here, we demonstrate simultaneous infrared absorption and Raman scattering spectroscopy that allows us to measure the complete broadband vibrational spectra in the molecular fingerprint region with a single instrument based on an ultrashort pulsed laser. The system is based on dual-modal Fourier-transform spectroscopy enabled by efficient use of nonlinear optical effects. Our proof-of-concept experiment demonstrates rapid, broadband and high spectral resolution measurements of complementary spectra of organic liquids for precise and accurate molecular analysis.


2020 ◽  
Vol 8 (21) ◽  
pp. 10796-10812 ◽  
Author(s):  
Francesco Silvio Gentile ◽  
Marianna Pannico ◽  
Mauro Causà ◽  
Giuseppe Mensitieri ◽  
Giulio Di Palma ◽  
...  

This paper reports an interpretation of the FTIR and Raman spectra of the HKUST-1 MOF in light of an ab initio theoretical analysis of the vibrational spectra of the framework.


2013 ◽  
Vol 20 (5) ◽  
pp. 683-690 ◽  
Author(s):  
Hongxin Wang ◽  
Yoshitaka Yoda ◽  
Weibing Dong ◽  
Songping D. Huang

The conventional energy calibration for nuclear resonant vibrational spectroscopy (NRVS) is usually long. Meanwhile, taking NRVS samples out of the cryostat increases the chance of sample damage, which makes it impossible to carry out an energy calibration during one NRVS measurement. In this study, by manipulating the 14.4 keV beam through the main measurement chamber without moving out the NRVS sample, two alternative calibration procedures have been proposed and established: (i) anin situcalibration procedure, which measures the main NRVS sample at stage A and the calibration sample at stage B simultaneously, and calibrates the energies for observing extremely small spectral shifts; for example, the 0.3 meV energy shift between the 100%-57Fe-enriched [Fe4S4Cl4]=and 10%-57Fe and 90%-54Fe labeled [Fe4S4Cl4]=has been well resolved; (ii) a quick-switching energy calibration procedure, which reduces each calibration time from 3–4 h to about 30 min. Although the quick-switching calibration is notin situ, it is suitable for normal NRVS measurements.


2016 ◽  
Vol 18 (1) ◽  
pp. 414-425 ◽  
Author(s):  
Eliano Diana ◽  
Karl Gatterer ◽  
Sidney F. A. Kettle

DFT has been used to model azide complexes and related model systems, in order to provide an understanding of azide vibrational spectra. The spectra are controlled by the charge distributions and the metal involved. This means that a group theory-based approach will seldom enable an interpretation, even though the azide groups are commonly vibrationally coupled.


2011 ◽  
Vol 65 (4) ◽  
Author(s):  
Radu Silaghi-Dumitrescu

AbstractThe electronic and vibrational properties of [Fe(NHis)4(SCys)] sites responsible for the catalysis of superoxide reduction in two types of superoxide reductase (SOR), one-iron superoxide reductase (1Fe-SOR) and two-iron superoxide reductase (2Fe-SOR), were compared previously (Clay et al., 2003); the differences between these two classes of SOR, examined by UV-VIS and NIR absorption, VTMCD, and vibrational spectroscopy techniques, were interpreted as being indicative of weaker Fe-S bonds in 2Fe-SOR in comparison with 1Fe-SOR. Here, we report on density functional (DFT) and semi-empirical (ZINDO/S-CI) calculations exploring the extent of this difference in bonding between the two classes of SOR. The differences observed experimentally between the electronic spectra of the two SORs are shown to probably arise either from different degrees of torsion between the Fe—ligand bonds or from differences in length of the Fe—carboxylate bond, but are shown to be incompatible with any significant differences in Fe—S bond lengths. The differences observed in the vibrational spectra between the two SORs are shown to correlate with differences in the Fe-S bond length of no more than 0.01 Å, which in turn arise from slight differences in the polarity of the medium surrounding the iron active site in the two proteins.


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