Research Article  Open Access
G. R. Ramkumaar, S. Srinivasan, T. J. Bhoopathy, S. Gunasekaran, "Vibrational Spectroscopic Studies of Tenofovir Using Density Functional Theory Method", Journal of Chemistry, vol. 2013, Article ID 126502, 12 pages, 2013. https://doi.org/10.1155/2013/126502
Vibrational Spectroscopic Studies of Tenofovir Using Density Functional Theory Method
Abstract
A systematic vibrational spectroscopic assignment and analysis of tenofovir has been carried out by using FTIR and FTRaman spectral data. The vibrational analysis was aided by electronic structure calculations—hybrid density functional methods (B3LYP/6311++G(d,p), B3LYP/631G(d,p), and B3PW91/631G(d,p). Molecular equilibrium geometries, electronic energies, IR intensities, and harmonic vibrational frequencies have been computed. The assignments proposed based on the experimental IR and Raman spectra have been reviewed and complete assignment of the observed spectra have been proposed. UVvisible spectrum of the compound was also recorded and the electronic properties such as HOMO and LUMO energies and were determined by timedependent DFT (TDDFT) method. The geometrical, thermodynamical parameters, and absorption wavelengths were compared with the experimental data. The B3LYP/6311++G(d,p), B3LYP/631G(d,p), and B3PW91/631G(d,p)based NMR calculation procedure was also done. It was used to assign the ^{13}C and ^{1}H NMR chemical shift of tenofovir.
1. Introduction
A recent addition to the antiretroviral armamentarium is the nucleotide analogue tenofovir disoproxil fumarate (Viread), approved for use in the USA and the European Union. Tenofovir is unique among the NRTIs in that it is an acyclic nucleoside phosphonate, analogous to the monophosphate form of the other NRTIs [1]. Tenofovir disoproxil fumarate is an oral prodrug of tenofovir that is rapidly converted into tenofovir upon absorption [2, 3]. Tenofovir has activity in vitro against both HIV1 and HIV2 [4, 5], and in resting and activated T cells, monocytes and macrophages [5, 6]. Crossresistance within the NRTI class of drugs has important clinical consequences for patients who are highly treatment experienced, or for those patients in whom primary HIV infection is associated with the transmission of a resistant virus [7].
Literature survey reveals that to the best of our knowledge, neither the complete IR, Raman spectra, nor the quantum mechanical calculations for molecular structure of tenofovir have been reported so far. In the present communication, we report detailed quantum chemical studies of the molecular structure and IR, Raman spectra of tenofovir using basis set. Information about the geometry and structure of the molecule, together with analysis of the IR, Raman spectra, based on frequency and intensity should help in understanding the structural and spectral characteristics. The band assignments have made by assuming C_{1} point group symmetry. Density Functional Theory (DFT) calculations have been performed to support our wave number assignments.
2. Experimental Details
The compound tenofovir in powder form was procured from Reputed pharmaceutical company, Chennai, India with more than 98% purity and was used as such without further purification to record FTIR and FTRaman spectra. The FTIR spectrum of the compound was recorded in the region 4000–450 cm^{−1} in evacuation mode on Bruker IFS 66V spectrophotometer using KBr pellet technique (solid phase) with 4.0 cm^{−1} resolution. The FTRaman spectrum was recorded using 1064 nm line of Nd: YAG laser as excitation wavelength in the region 5000–10 cm^{−1} on Bruker IFS 66V spectrometer equipped with FRA 106 Raman module was used as an accessory. The UVvis spectral measurements were carried out using a varian cary 5EUVNIR spectrophotometer. The spectral measurements were carried out at sophisticated instrumentation Analysis Facility, IIT, Chennai, India.
3. Computational Details
To provide complete information regarding the structural characteristics and the fundamental vibrational modes of tenofovir of B3LYP/6311++G(d,p), B3LYP/631G(d,p), and B3PW91/631G(d,p) correlation functional calculations have been carried out. The calculations of geometrical parameters in the ground state were performed using the Gaussian 03 [9] programs, invoking gradient geometry optimization [10] on Intel core i4/2.93 GHZ processor. The geometry optimization was carried out using the initial geometry generated from standard geometrical parameters at B3LYP and B3PW91 methods adopting 631G(d,p) and 6311++G(d,p) basis sets to characterize all stationary points as minima. The optimized structural parameters of the compound tenofovir were used for harmonic vibrational frequency calculations resulting in IR and Raman frequencies together with intensities. In DFT methods, Becke’s three parameter exchangefunctional (B3) [11, 12] combined with gradientcorrected correlation functional of Johnson and Frisch [13] and Burke et al. [14–19] by implementing the splitvalence polarized 631G(d,p) basis set [20, 21] have been utilized for the computation of molecular structure optimization, vibrational frequencies, thermodynamic properties, and energies of the optimized structures. The timedependent density functional theory (TDDFT) methods were used for the calculation of the UVvis spectra. The IR and UVvis spectra were calculated and visualized using the SWizard program [22]. The ^{13}C and ^{1}H NMR chemical shifts of the title compound were calculated using the keyword NMR in the DFTB3LYP and B3PW91 levels.
4. Results and Discussion
4.1. Molecular Geometry
To compare the structural parameters of tenofovir and with the available experimental data, they are subjected to geometry optimization in their ground state. For each method, geometry optimizations were performed. The requested convergence on the maximum density matrix was 1026 a.u. the threshold value of the maximum displacement was 0.0018 A° and that of the maximum force was 0.00045 Hartree/Bohr using the Berny analytical gradient optimization routine [10, 23]. The nature of stationary points is checked by diagonalising the Hessian matrix to determine the number of imaginary wave numbers (zero for local minimum). The optimized bond lengths and bond angles of tenofovir calculated by B3LYP/6311++G(d,p), B3LYP/631G(d,p), and B3PW91/631G(d,p) levels are listed in Table 1, in accordance with the atom numbering scheme shown in Figure 1. Table 1 shows the comparison of the calculated optimized structure parameters for tenofovir with those experimentally available data [8]. It is observed that most of the optimized structure parameters are slightly larger than the available data values. The bond lengths and bond angles computed by the DFTB3LYP and B3PW91 levels show excellent agreement with the available computed values.

The bond distance of carboncarbon in the benzene ring in the range of 1.524 Å confirms the doublebond character and in the range of 1.370 Å supports the singlebond character. The bond distances of C–N and C–O were in the expected range and agree with the experimental values. Although there is a slight difference between the calculated and experimental structure parameters, the calculated geometric parameters represent a good approximation, and they are the bases for calculating other parameters such as atomic charges, NMR chemical shift values, vibrational modes, and thermodynamic properties.
4.2. BondOrder Analysis
The bond order of tenofovir is presented in Table 2. Bond order is related to bond strength. The bonds with the higher bond order values have short bond length and vice versa. The bondorder analysis may predict that the weakest bonds may be cleaved preferentially and they may possess a relatively low pibond character. From Table 2, it is noted that bond between O2–C4 possess relatively low pibond character with lowbondorder value of 0.848 obtained DFTB3LYP method, respectively. The P16–O19 bond order values are in the range 1.947, which depict the double bond character, while the C4–C5 and N8–C9 bondorder value is approximately unity, which shows the singlebond character. The optimized geometrical values are in support of the bondorder analysis.

4.3. Electronic Properties
The energies of four important molecular orbitals of tenofovir: the highest and second highest occupied MOs (HOMO and HOMO−1), the lowest and the second lowest unoccupied MOs (LUMO and LUMO+1) were calculated and are presented in Table 3. The lowest singlet→singlet spinallowed excited states of tenofovir were taken into account for the TDDFT calculation in order to investigate the properties of electronic absorption. The experimental values are obtained from the UV/visible spectra recorded in methanol as reported earlier [24]. The calculations were also performed with methanol solvent effect. The calculated absorption wavelengths (), oscillator strength, excitation energies, and the experimental wavelengths are also given in Table 3. The energy gap between HOMO and LUMO is a critical parameter in determining molecular electrical transport properties [25]. In the electronic absorption spectrum of tenofovir, there are three absorption bands with a maximum 268.67, 250, and 230.69 nm. The strong absorption band 268.67 nm is caused by the and the other two moderately intense bands are due to transitions. The transitions are expected to occur relatively at lower wavelength, due to the consequence of the extended aromaticity of the benzene ring. The HOMO and LUMO of tenofovir are represented in Figure 2.

4.4. Natural Population Analysis
The calculation of effective atomic charges plays an important role in the application of quantum mechanical calculations to molecular systems. Our interest here is in the comparison of different methods (B3LYP and B3PW91) to describe the electron distribution in tenofovir as broadly as possible, and to assess the sensitivity of the calculated charges to changes in the choice of the quantum chemical method. The calculated natural atomic charge values from the natural population analysis (NPA) and Mulliken population analysis (MPA) procedures using the B3LYP/6311++G(d,p), B3LYP/631G(d,p), and B3PW91/631G(d,p) methods are listed in Table 4. The NPA from the naturalbonding orbital (NBO) method is better than the MPA scheme. Table 4 compares the atomic charge site of tenofovir from both MPA and NPA methods. The NPA of tenofovir shows that the presence of three oxygen atoms in the nitrate moiety [O17 = −0.979 (B3LYP/6311++G(d,p)), −1.023 (B3LYP/631G(d,p)) and −1.023 (B3PW91/631G(d,p)); O18 = −0.983 (B3LYP/6311++G(d,p)), −1.027 (B3LYP/631G(d,p)) and −1.027 (B3PW91/631G(d,p)); O19 = −1.070 (B3LYP/6311++G(d,p)), −1.092 (B3LYP/631G(d,p)) and −1.087 (B3PW91/631G(d,p))] imposes large positive charges on the Phosphorus atom [P16 = 2.265 (B3LYP/6311++G(d,p)), 2.388 (B3LYP/631G(d,p) and 2.373 (B3PW91/631G(d,p))]. However, the nitrogen atoms N6, N8, N10, and N12 possess large negative charges, resulting in the positive charges on the carbon atoms C7, C9, C11, C13, and C14. Moreover, there is no difference in charge distribution observed on all hydrogen atoms except the H30, H31, H32, and H33 hydrogen atoms. The positive charge on H30, H31, H32, and H33 hydrogen atoms is due to the negative charge accumulated on the N15, O17, and O18 atoms.

4.5. Vibrational Spectra
The experimental FTIR, calculated (B3LYP, B3PW91) and FTRaman and vibrational spectra were shown in Figures 3 and 4. Since the calculated vibrational wave numbers were known to be higher than the experimental ones, they were scaled down by the wavenumber linear scaling procedure of Yoshida et al. [26] by using the expression: Comparison of the frequencies calculated at B3LYP and B3PW91 with experimental values (Table 5) reveals the overestimation of the calculated vibrational modes due to the neglect anharmonicity in real system. According to the theoretical calculations, tenofovir has a nonplanar structure of C_{1} point group symmetry. The molecule has 33 atoms and 93 normal modes of vibration active in both IR and Raman. Since the title molecule possess C_{1} point group symmetry, all the modes of vibration belong to A species only. The Chemcraft program was used to display the vibrational modes. Vibrational wave number assignments were made on the basis of combining the results of Chemcraft program with the symmetry, and taking the atomic displacements into consideration based on the frequency calculation and also made in analogy with the structurally related molecules.

(a)
(b)
(c)
(d)
The CH and OH stretching modes are expected to be observed at the high wave number region. The CH stretching bands are observed between 3106 cm^{−1} and 3051 cm^{−1} in FTIR spectrum. The CH stretching modes in the ring and methylene groups were identified and their effect in tenofovir was examined. Let us start considering the contribution of theoretical methods B3LYP/6311++G(d,p), B3LYP/631G(d,p) and B3PW91/631G(d,p), the OH stretching mode is predicted at 3650 cm^{−1}, 3583 cm^{−1} in B3PW91 and 3620 cm^{−1}, 3563 cm^{−1} in B3LYP and 3629 cm^{−1}, 3619 cm^{−1} in B3LYP/6311++G(d,p) after scaling. This OH stretching mode is affected in the presence of water molecules. The CH_{2} scissoring and wagging mode was also identified. A major coincidence of theoretical values with that of experimental evaluations is found in the asymmetric and symmetric vibrations of the methylene (–CH_{2}–) moiety. The –CH_{2}– wagging mode at 1330 cm^{−1} in FTRaman deviates positively by 20 cm^{−1} from the reported value of 1350 cm^{−1} [25] and theoretically coincide with 1321 cm^{−1} in B3LYP and 1334 cm^{−1} in B3PW91. The vibrational frequency 1455 cm^{−1} in B3LYP and 1449 cm^{−1} in B3PW91 is found neater to FTIR–CH_{2}– scissoring mode of 1447 cm^{−1}.
The scaled NH_{2} asymmetric and symmetric stretching vibrations of theoretical values are 3570 cm^{−1} and 3456 cm^{−1}. The computed NH_{2} scissoring vibration at 1588 cm^{−1} in B3LYP and 1595 cm^{−1} in B3PW91 is in agreement with the expected characteristic value, 1600 cm^{−1} [27, 28]. In the presence of water molecules in the tenofovir, the NH stretching vibrations were red shifted by 10 cm^{−1}. But however, the NH_{2} scissoring mode does not get affected. Notice that the most evident discrepancies between the experimental and calculated spectra are associated with the stretching modes showing the effect of water molecules. List of selected observed and calculated bands of tenofovir was presented in Table 5.
5. ^{13}C and ^{1}HNMR Chemical Shift Assignment
The ^{13}C and ^{1}H NMR simulated theoretically with the aid of ChemDraw Ultra 10.0 is shown in Figures 5(a) and 5(b). Table 6 present the predicted chemical shift values of tenofovir obtained by the B3LYP/6311++G(d,p), B3LYP/631G(d,p), B3PW91/631G(d,p) and ChemDraw Ultra 10.0 software package and its assignment along with the shielding values. In general, highly shielded electrons appear downfield and vice versa. The predicted chemical shift values by the theoretical methods both DFT values slightly deviates from the computed values of ChemDraw Ultra. The carbon atom C11 appearing at very higher chemical shift value (177.0 in B3LYP/6311++G(d,p), 157.1 ppm in B3LYP/631G(d,p) and 152.6 ppm in B3PW91/631G(d,p)) due to negative charge of two nitrogen atoms (N10 and N12). Similarly C7, C9, and C13 appearing at higher chemical shift values (163.5, 174.7 and 166.4 ppm in B3LYP/6311++G(d,p), 143.3, 155.1 and 144.9 ppm in B3LYP/631G(d,p), 141.1, 152.6 and 143.1 ppm in B3PW91/631G(d,p)) are due to nitrogen atoms N6, N8, and N15, respectively.

(a)
(b)
The carbon atoms C7, C9, C11, C13, and C14 are electropositive and possess more positive charges than the other carbon atoms, and hence the shielding is very small and appears upfield (see Table 6). In both molecules, the DFTcalculated atomic charges revealed that the more electronrich atoms are C1, C3, C4, and C5; they are highly shielded atoms and hence appear at downfield (lower chemical shift). The carbon atoms in the benzene ring are deshielded than the carbon atoms in Aliphatic, so that the benzene carbon atoms in purine appear at higher chemical shift values than the aliphatic carbon atoms that were made by DFT methods. In this study, a good correlation between atomic charges and chemical shift was made. It is to be noted that ^{13}C NMR chemical shifts for tenofovir which agree with the ChemDraw Ultra.
Table 6 gives the ^{1}H NMR predicted chemical shift values obtained by the DFT methods and ChemDraw Ultra 10.0 software program [8] along with assignments. The predicted shielding values for each atom in the tenofovir molecule by B3LYP/6311++G(d,p), B3LYP/631G(d,p), and B3PW91/631G(d,p) are given in Table 6. The predicted chemical shift values by the ChemDraw Ultra software program are in good agreement with the two DFT methods.
The spectrum of tenofovir showed a singlet at 7.0 ppm for the proton of the aromatic (H31) group, which is in good agreement with the chemDraw ultra value. Triplet is predicted at 2.9, 2.3, and 2.3 ppm for the methyl group of hydrogen atoms (H25, H26, and H27). This higher chemical shift for methyl group hydrogen is mainly due to the carbon atom (C5). The predicted value of singlet peak at higher chemical shift at 16.2 ppm for methine group of the indole proton (H24). Doublet is predicted at 7.0 ppm for the aromatic group of hydrogen atoms (H30 and H31). This higher chemical shift for methyl group hydrogen is mainly due to the nitrogen atom (N15). The hydrogen atoms of methylene group attached with C1 and C3 atoms show a multiplet at 3.4–3.9 ppm, which is due to the presence of oxygen and nitrogen atoms, respectively. In all the DFT methods predict the chemical shifts value of the hydrogen in hydroxyl group(H32, H33) is contradicting to chemDraw ultra value, but other hydrogen atoms fairly agrees.
6. Thermodynamic Properties
Several calculated thermodynamic parameters at room temperature are presented in Table 7. According to Koopmanns’ theorem, ionization potential (I) is the negative of the highest occupied molecular orbital (HOMO) energy, that is, I = −EHOMO, and affinity potential (A) is the negative of the lowest unoccupied molecular orbital (LUMO) energy, that is, A = −ELUMO, which are summarized in Table 7.

Knowledge of permanent dipole moment of a molecule provides a wealth of information to determine the exact molecular conformation. The total dipole moment value of tenofovir in both DFTs and B3PW91 methods was observed. The variations in the entropy and zeropoint vibrational energies seem to be insignificant.
7. Conclusion
The geometry of tenofovir was optimized with both DFT and B3PW91 methods using 631G(d,p) and 6311++G(d,p) basis sets. The complete molecular structural parameters and thermodynamic properties of the optimized geometry of the compound have been obtained from DFT calculations. The vibrational frequencies of the fundamental modes of the compound have been precisely assigned and analyzed and the theoretical results were compared with the experimental vibrations. The bond order and atomic charges of the title molecule have been studied by DFT and B3PW91 methods. The energies of important MOs, absorption wavelength (), oscillator strength, and excitation energies of the compound were also determined from TDDFT method and compared with the experimental values. This study predicted that the molecular geometry, vibrational wave numbers and ^{13}C and ^{1}H NMR chemical shifts for tenofovir could be successfully elucidated by the B3LYP/6311++G(d,p), B3LYP/631G(d,p) and B3PW91/631G(d,p) methods using Gaussian program. Thus, the present investigation provides complete vibrational assignments, structural informations and electronic properties of the compound which may be useful to upgrade the knowledge on tenofovir.
References
 L. Naesens, R. Snoeck, G. Andrei, J. Balzarini, J. Neyts, and E. De Clercq, “HPMPC (cidofovir), PMEA (adefovir) and related acyclic nucleoside phosphonate analogues: a review of their pharmacology and clinical potential in the treatment of viral infections,” Antiviral Chemistry & Chemotherapy, vol. 8, no. 1, pp. 1–23, 1997. View at: Google Scholar
 M. Arimilli, C. Kim, and N. Bischofberger, “Synthesis, in vitro biological evaluation and oral bioavailability of 9[2(phosphonomethoxy)propyl]adenine (PMPA) prodrugs,” Antiviral Chemistry & Chemotherapy, vol. 8, no. 6, pp. 557–564, 1997. View at: Google Scholar
 L. Naesens, N. Bischofberger, P. Augustijns et al., “Antiretroviral efficacy and pharmacokinetics of oral bis(isopropyloxycarbonyloxymethyl)9(2phosphonylmethoxypropyl)adenine in mice,” Antimicrobial Agents and Chemotherapy, vol. 42, no. 7, pp. 1568–1573, 1998. View at: Google Scholar
 J. Balzarini, A. Holy, J. Jindrich et al., “Differential antiherpesvirus and antiretrovirus effects of the (S) and (R) enantiomers of acyclic nucleoside phosphonates: potent and selective in vitro and in vivo antiretrovirus activities of (R)9(2phosphonomethoxypropyl) 2,6diaminopurine,” Antimicrobial Agents and Chemotherapy, vol. 37, no. 2, pp. 332–338, 1993. View at: Google Scholar
 B. L. Robbins, R. V. Srinivas, C. Kim, N. Bischofberger, and A. Fridland, “Antihuman immunodeficiency virus activity and cellular metabolism of a potential prodrug of the acyclic nucleoside phosphonate 9R(2 phosphonomethoxypropyl)adenine (PMPA), bis(isopropyloxymethylcarbonyl)PMPA,” Antimicrobial Agents and Chemotherapy, vol. 42, no. 3, pp. 612–617, 1998. View at: Google Scholar
 B. L. Robbins, J. J. Greenhaw, M. C. Connelly, and A. Fridland, “Metabolic pathways for activation of the antiviral agent 9(2 phosphonylmethoxyethyl)adenine in human lymphoid cells,” Antimicrobial Agents and Chemotherapy, vol. 39, no. 10, pp. 2304–2308, 1995. View at: Google Scholar
 V. Miller and B. A. Larder, “Mutational patterns in the HIV genome and crossresistance following nucleoside and nucleotide analogue drug exposure,” Antiviral Therapy, vol. 6, supplement 3, pp. 25–44, 2001. View at: Google Scholar
 Carl Kemnitz 2002 Chemoffice ultra 10, Trial version.
 M. J. Frisch, G. W. Trucks, H. B. Schlegel et al., Gaussian Inc., Woodbridge, Conn, USA, 2004.
 H. B. Schlegel, “Optimization of equilibrium geometries and transition structures,” Journal of Computational Chemistry, vol. 3, no. 2, pp. 214–218, 1982. View at: Publisher Site  Google Scholar
 A. D. Becke, “Densityfunctional exchangeenergy approximation with correct asymptotic behavior,” Physical Review A, vol. 38, no. 6, pp. 3098–3100, 1988. View at: Publisher Site  Google Scholar
 C. Lee, W. Yang, and R. G. Parr, “Development of the ColleSalvetti correlationenergy formula into a functional of the electron density,” Physical Review B, vol. 37, no. 2, pp. 785–789, 1988. View at: Publisher Site  Google Scholar
 B. G. Johnson and M. J. Frisch, “Analytic second derivatives of the gradientcorrected density functional energy. Effect of quadrature weight derivatives,” Chemical Physics Letters, vol. 216, no. 12, pp. 133–140, 1993. View at: Publisher Site  Google Scholar
 K. Burke, J. P. Perdew, and Y. Wang, “Derivation of a generalized gradient approximation: the PW91 density functional,” in Electronic Density Functional Theory; Recent Progress and New Directions, J. F. Dobson, G. Vignale, and M. P. Das, Eds., Plenum Press, 1998. View at: Google Scholar
 J. P. Perdew, “Unified theory of exchange and correlation beyond the local density approximation,” in Electronic Structure of Solids '91, P. Ziesche and H. Eschrig, Eds., pp. 11–20, Academic Verlag, Berlin, Germany, 1991. View at: Google Scholar
 J. P. Perdew, J. A. Chevary, S. H. Vosko et al., “Atoms, molecules, solids, and surfaces: applications of the generalized gradient approximation for exchange and correlation,” Physical Review B, vol. 46, no. 11, pp. 6671–6687, 1992. View at: Publisher Site  Google Scholar
 J. P. Perdew, J. A. Chevary, S. H. Vosko et al., “Erratum: atoms, molecules, solids, and surfaces: applications of the generalized gradient approximation for exchange and correlation,” Physical Review B, vol. 48, no. 7, p. 4978, 1993. View at: Publisher Site  Google Scholar
 J. P. Perdew, K. Burke, and Y. Wang, “Generalized gradient approximation for the exchangecorrelation hole of a manyelectron system,” Physical Review B, vol. 54, no. 23, pp. 16533–16539, 1996. View at: Google Scholar
 J. P. Perdew and Y. Wang, “Accurate and simple analytic representation of the electrongas correlation energy,” Physical Review B, vol. 45, no. 23, pp. 13244–13249, 1992. View at: Publisher Site  Google Scholar
 W. J. Hehre, L. Radom, P. V. R. Schleyer, and A. J. Pople, Ab Initio Molecular Orbital Theory, John Wiley & Sons, New York, NY, USA, 1989.
 Z. DegaSzafran, A. Katrusiak, and M. Szafran, “Molecular structure of the complex of Nmethylmorpholine betaine with 2,4dinitrophenol,” Journal of Molecular Structure, vol. 741, no. 1–3, pp. 1–9, 2005. View at: Publisher Site  Google Scholar
 S. I. Gorelsky, SWizard program, 2005, http://www.sgchem.net/.
 H. B. Schlegel, “An efficient algorithm for calculating ab initio energy gradients using s, p Cartesian Gaussians,” The Journal of Chemical Physics, vol. 77, no. 7, pp. 3676–3681, 1982. View at: Google Scholar
 S. A. Ghorpade, M. S. Sali, A. H. Kategaonkar, D. M. Patel, V. P. Choudhari, and B. S. Kuchekar, “Simultaneous determination of emtricitabine and tenofovir by area under curve and dual wavelength spectrophotometric method,” Journal of the Chilean Chemical Society, vol. 55, no. 1, pp. 115–117, 2010. View at: Google Scholar
 R. M. Silverstein, G. C. Bassler, and T. C. Morrill, Spectrometric Identification of Organic Compounds, John Wiley & Sons, New York, NY, USA, 5th edition, 1981.
 H. Yoshida, K. Takeda, J. Okamura, A. Ehara, and H. Matsuura, “A new approach to vibrational analysis of large molecules by density functional theory: wavenumberlinear scaling method,” Journal of Physical Chemistry A, vol. 106, no. 14, pp. 3580–3586, 2002. View at: Publisher Site  Google Scholar
 R. A. Yadav and I. S. Sing, “Hydrogen bonding in o and methyl phenols,” Indian Journal of Pure and Applied Physics, vol. 23, pp. 626–627, 1985. View at: Google Scholar
 K. B. Wibery and A. Shrake, “A vibrational study of cyclohexane and some of its isotopic derivativesIII. A vibrational analysis of cyclohexane, cyclohexane${d}_{12}$, cyclohexane1,1,4,4${d}_{4}$ and cyclohexane1,1,2,2,4,4,5,5${d}_{8}$,” Spectrochimica Acta A, vol. 29, no. 3, pp. 583–594, 1973. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2013 G. R. Ramkumaar et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.