Sobia Younas‡
a,
Aqdas Riaz‡a,
Haq Nawaz*a,
Muhammad Irfan Majeed*a,
Muhammad Adnan Iqbala,
Nosheen Rashidb,
Areeba Altafa,
Umar Sohail Shoukata,
Faisal Jamila,
Aafia Sehara,
Sania Munira,
Mahrosh Javeda and
Muhammad Imranc
aDepartment of Chemistry, University of Agriculture Faisalabad, Faisalabad 38000, Pakistan. E-mail: haqchemist@yahoo.com; irfan.majeed@uaf.edu.pk
bDepartment of Chemistry, University of Education, Faisalabad Campus, Faisalabad 38000, Pakistan
cDepartment of Chemistry, Faculty of Science, King Khalid University, P.O. Box 9004, Abha 61413, Saudi Arabia
First published on 4th December 2023
In the present study, Raman spectroscopy (RS) along with density functional theory (DFT) calculations have been performed for the successful characterization and confirmation of the formation of three different selenium-based N-heterocyclic carbene (NHC) complexes from their respective salts. For this purpose, mean RS features and DFT calculations of different ligands and their respective selenium NHC complexes are compared. The identified characteristic RS and DFT features, of each of these ligands and their selenium complexes, show that the polarizability of benzimidazolium rings increases after complex formation with selenium. This has been shown by the enhanced intensity of the associated Raman peaks, therefore, confirming the formation of newly formed bonds. The complex formation is also confirmed by the identification of several new peaks in the spectra of complexes and these Raman bands were absent in the spectra of the ligands. Moreover, Raman spectral data sets are analyzed using a multivariate data analysis technique of Principal Component Analysis (PCA) to observe the efficiency of the RS analysis. The results presented in this study have proved the RS technique, along with DFT, an undoubtedly fast approach for the confirmation of synthesis of selenium based NHC-complexes.
Since then, the synthesis of novel NH-free carbene ligands and their corresponding metallic compounds such as with silver and selenium have become an area of extensive research.5 Various researches have shown that protein-rich foods such as eggs, fish and meat also contain huge amounts of selenium, with its antioxidant activity through enzymes such as glutathione peroxidase.6 Many of the applications regarding selenium-containing NHC complexes have also been studied in effective cancer treatment, anti-septic agents, antibiotics, antioxidants and stress relieving medicines.7,8
The various organoselenium complexes are being synthesized in several ways and for their exact characterization, different physical methods such as melting point and spectroscopic analytical approaches, for instance, Electrospray Ionization Mass Spectrometry (ESI-MS), Fourier-transform infrared spectroscopy (FT-IR), Nuclear Magnetic Resonance (NMR) spectroscopy and X-ray crystallography are being used.9,10 However, available literature reveals that these above-illustrated approaches do not provide a direct detection pathway within one certain analytic cycle as these techniques have many limitations like consumption, require more sample, expensive, often require complex sample preparation and various intermediate steps which are expensive and laborious.11,12 Raman spectroscopy has been used to minimize the limitations of the above illustrated techniques as it is inexpensive, based on nondestructive interaction between light with chemical bonds within a material, requires no complex sample preparation and requires sample only in a small amount. Raman spectroscopy has also been used to study crystallinity, chemical structure, polymorphism, phase, molecular interactions and to minimize the limitations in the characterizations of organometallic compounds such as dimethylselone, seleno urea, organo selenols, organo selenium carbene, organo selenium halides and transition organo selenium compounds.11,13,14
This paper unravels a significant indication of the successful formation of selenium complexes from their particular NHC salts through Raman spectral (RS) analysis along with the support of DFT analysis with great precision. Raman spectroscopy is a molecular vibrational spectroscopic technique that provides vastly valuable evidence about the structures of the molecules based on the Raman scattering effect.15 This spectroscopic technique provides sensitive information which is specific to the distinct fingerprint of constituent particles in a sample under observation,16 thus enabling the detection of analytes.17 This broadened scope of the Raman spectral technique over the other traditional techniques include its good spatial resolution in spectroscopic information with non-destructive identification of target components under ordinary conditions.18
In the current study, the successful structural elucidation of three different selenium-carbene coordination complexes (with respect to nitrogen attached side chains) has been accomplished through the RS technique along with the DFT method to further explore Raman spectroscopy for such applications. Raman spectroscopy along with a multivariate data analysis technique, Principal Component Analysis (PCA), has been employed for the characterization of three structurally different (differing in substituent at nitrogen) ligands/benzimidazolium salts (ligand-I, ligand-II and ligand-III) and their respective organometallic compounds mono-NHC-selenium complexes (complex-I, complex-II and complex-III). This investigation has led to the advancement in Raman-based approaches for differentiation between a variety of ligands and their particular complexes and also provides an understanding of confirmation of the formation of coordinate covalent bonds in these complexes.
Fig. 1 Structural formulas of benzimidazolium salts (ligand-I, ligand-II and ligand-III) and their respective selenium-N-heterocyclic carbene complexes (complex-I, complex-II and complex-III). |
Fig. 4 Comparison of mean Raman spectra of ligand-II (L2) with the mean spectrum of complex-II (C2). |
Observed L1 (cm−1) | DFT b3lyp L1 (cm−1) | Observed C1 (cm−1) | DFT b3lyp C1 (cm−1) | Observed L2 (cm−1) | DFT b3lyp L2 (cm−1) | Observed C2 (cm−1) | DFT b3lyp C2 (cm−1) | Observed L3 (cm−1) | DFT b3lyp L3 (cm−1) | Observed C3 (cm−1) | DFT b3lyp C3 (cm−1) | Peak assignment | References |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
a Abbreviations = (o-p = out-of-plane); (i-p = in-plane); (sym = symmetrical); (def = deformation); (wag = wagging); (sci = scissoring); (Bz = benzene); (str = stretching). | |||||||||||||
267 | 270 | 267 | 268 | 267 | 267 | 267 | 265 | 266 | 266 | — | — | (C–C–C) o-p bending | 22 |
286 | 283 | 286 | 287 | 281 | 281 | 281 | 281 | 280 | 280 | 280 | 280 | CH2 rocking | 23 |
— | — | — | — | — | — | — | — | 293 | — | 293 | 291 | CH2 rocking | 23 |
— | — | — | — | 311 | 308 | — | — | 309 | 310 | — | — | Def vibrations in C–C–C | 24 |
331 | 340 | 331 | 328 | 331 | 334 | 331 | 326 | 331 | 330 | 331 | 330 | Ring wag + chain def | 25 |
367 | 369 | 367 | 372 | 370 | 366 | 370 | 369 | — | — | — | — | C–C def | 26 |
— | — | — | — | 385 | 376 | 385 | 390 | — | — | — | — | Bz ring bending modes | 27 |
— | — | — | — | — | — | — | — | 421 | 421 | 421 | 421 | Ring rotation 5-member ring | 25 and 28 |
— | — | — | — | 434 | 434 | 434 | 441 | 434 | 434 | 434 | 432 | C–C def of aliphatic chain | 23 and 26 |
458 | 458 | 458 | 457 | — | — | — | — | 457 | 459 | 457 | 462 | C–C–C o-p bend | 29 |
476 | 476 | 476 | 476 | 474 | 475 | 474 | 475 | — | — | — | — | C–C skeleton def | 30 |
— | — | — | — | — | — | — | — | 499 | 498 | 499 | 498 | C–N o-p bend benzimidazole | 25 |
539 | 546 | 539 | 539 | — | — | — | — | 532 | — | 532 | — | C–N–C def aliphatic chain | 31 |
— | — | — | — | 548 | 546 | 548 | 547 | — | — | — | — | Wag mode of NO2 | 32 |
— | — | — | — | 577 | 577 | 577 | 579 | 572 | 582 | 572 | 582 | Ring def benzimidazole | 23 |
— | — | — | — | — | — | — | — | 609 | 609 | 609 | 609 | C–C–C def i-p vibration mode of bz | 33 |
617 | 615 | 617 | 619 | — | — | — | — | — | — | — | — | C–C–C symmetric bend phenyl ring | 34 |
— | — | — | — | 627 | 626 | — | — | — | — | — | — | C–C–C def i-p benzimidazole | 33 and 34 |
— | — | — | — | — | — | 651 | 651 | — | — | — | — | Phenyl ring vibrations | 35 |
713 | 713 | 713 | 713 | 713 | — | 713 | 713 | 713 | 713 | 713 | 713 | C–N o-p str of 5-membered ring | 23 |
736 | 738 | 736 | 737 | — | — | — | — | — | — | — | — | Bz C–H sym wag | 36 |
750 | 752 | 750 | 750 | — | — | 750 | 750 | — | — | — | — | Bz o-p bend benzimidazole | 23 and 37 |
779 | 782 | 779 | 781 | 780 | 784 | 780 | 787 | 782 | 780 | 782 | 780 | C–H o-p bend benzimidazole | 22, 23 and 37 |
822 | 825 | 822 | 820 | 826 | 827 | 826 | 826 | 822 | 822 | C–C str | 26 | ||
840 | — | 840 | 840 | — | — | — | — | 843 | 846 | 843 | 845 | C–C str | 38 |
— | — | — | — | 863 | 863 | — | — | — | — | — | — | NO2 sci | 32 |
878 | — | 878 | — | — | — | — | — | — | — | — | — | C–H o-p bend benzimidazole | 23 and 39 |
— | — | — | — | 887 | 876 | — | — | 890 | 895 | — | — | C–H o-p bend | 22 |
897 | 898 | — | — | — | — | 895 | 896 | — | — | — | — | CH2 sci | 40 |
— | — | — | — | 942 | 938 | 942 | — | — | — | — | — | Imidazole i-p bend | 37 |
967 | 963 | 967 | 969 | — | — | — | — | 963 | 959 | 963 | 967 | CH3 wag | 26 and 40 |
1019 | 1015 | 1019 | 1019 | 1014 | 1009 | 1014 | 1018 | 1016 | 1023 | 1023 | 1023 | C–C–C trigonal bend benzimidazole | 39 |
— | — | — | — | 1049 | 1045 | — | — | — | — | — | — | Ring def 5-member | 25 |
— | — | — | — | — | — | — | — | 1071 | 1071 | — | — | C–C str mode of aliphatic | 23 and 41 |
— | — | — | — | 1098 | 1089 | 1098 | 1089 | — | — | — | — | C–N str | 18 |
1138 | 1139 | 1130 | 1135 | — | — | 1130 | 1130 | 1137 | 1143 | 1137 | 1137 | C–C str aliphatic vibration | 41 |
— | — | — | — | 1144 | 1141 | 1156 | 1154 | — | — | — | — | C–H sym bend benzimidazole | 42 |
— | — | 1186 | 1182 | 1175 | 1169 | 1183 | 1182 | 1183 | 1183 | 1183 | 1183 | i-p C–H bend benzimidazole | 37 |
1215 | 1213 | 1215 | 1212 | — | — | — | — | — | — | — | — | C–C str aliphatic chain | 23 and 26 |
— | — | — | — | — | — | — | — | 1225 | 1225 | 1214 | 1218 | C–N str benzimidazole | 43 and 44 |
— | — | 1246 | 1244 | — | — | — | — | — | — | — | — | C–C str aliphatic side chain | 23 and 26 |
— | — | — | — | 1258 | 1256 | 1269 | 1269 | 1260 | 1256 | — | — | i-p bz ring def | 27 |
— | — | 1297 | 1298 | 1283 | 1290 | 1293 | 1298 | 1294 | 1294 | 1294 | 1294 | CH2 def aliphatic chain | 23 and 26 |
1313 | 1313 | — | — | 1318 | 1318 | — | — | 1313 | 1313 | — | — | C–H def of CH2 | 45 |
1342 | 1340 | 1342 | 1342 | 1342 | 1340 | C–H def in bz ring | 27 and 37 | ||||||
1351 | 1351 | 1351 | 1351 | 1354 | 1358 | 1369 | 1367 | 1354 | 1352 | 1354 | 1362 | Ring str imidazole | 27 and 37 |
— | — | 1416 | 1417 | — | — | 1411 | 1411 | — | — | 1412 | 1410 | CSe | 46 |
1434 | 1432 | 1445 | 1443 | 1434 | 1432 | 1448 | 1448 | 1433 | 1427 | 1446 | 1438 | CH def | 41 and 47 |
— | — | — | — | 1590 | 1589 | 1590 | 1588 | — | — | — | — | C–C–C str mode of vibration in phenyl ring | 33 |
1610 | — | 1610 | — | 1613 | 1618 | 1613 | 1617 | 1611 | — | 1611 | — | CC str mode benzimidazole | 18, 22, 37 and 48 |
As selenium forms a double bond with the carbene carbon of benzimidazole ring, vanishing of charge on ligand-I which is salt of bromide ion, transforms polarity of the ring into polarizability, as a result enhancing Raman spectral features at 331 cm−1 (imidazole ring wagging accompanied with the attached chains deformation), 713 cm−1 (C–N out of plane stretching vibrations of imidazole rings), 750 cm−1 (out-of-plane bending of benzene in benzimidazole), 736 cm−1 (wagging of C–H in benzene ring). The most significant differentiating features have been manifested through dashed lines at 1416 cm−1 in C1, probably due to CSe vibrations while a strong peak appearance at 1186 cm−1 is the indication of activation of C–H in-plane bending of benzimidazole ring and a shoulder peak at 1342 cm−1 is due to C–H deformation in benzene ring after complex formation. Notably, these vibrations/spectral features are absent in the L1 structure. Selenium complex formation has resulted in some of the spectral features to decrease in intensities or diminish completely in mean Raman spectra of complexes such as a band in ligand at 1313 cm−1 (C–H deformation of CH2 in aliphatic side chains) is vague in complex and a large peak at 1610 cm−1 in ligand has become a relatively small peak in C1 which indicates the reduced CC stretching vibrations of benzimidazole ring after C1 formation. In the same way, relatively intense bands at 779 cm−1 and 878 cm−1 (C–H out of plane bending in benzimidazole) in the spectrum of C1 also confirm selenium complex formation.
Comparatively enhanced bands associated with aliphatic side chains at 267 cm−1 and 458 cm−1 (C–C–C out-of-plane bending), 822 cm−1, 840 cm−1, 1215 cm−1, 1246 cm−1 and shift of 1138 cm−1 to 1130 cm−1 (C–C stretching associated with aliphatic chains on both sides of imidazole rings) and at 967 cm−1 (CH3 wagging) are most likely due to the reason that lone pairs at nitrogen atoms become delocalized after complex making, causing less (–I) inductive effect resulting in a lesser amount of polarity and more polarizability of alkyl chains hence enhancing Raman spectral signals in the spectrum of the complex. The bands in the L1 spectrum at 1434 cm−1 and 1313 cm−1 are associated with C–H deformations of CH2 which are characteristic of hydrocarbon chains. Similarly, these Raman spectral features are in correspondence with the Raman spectral features calculated from density functional theory (DFT) as in ESI as Fig. S1.†
The distinct features in mean RS analysis have been observed, in which features related to benzimidazole ring structure at 331 cm−1 (ring wag with chain twisting), 385 cm−1 (benzene ring bending modes), 577 cm−1 (ring deformation), 627 cm−1 (in-plane C–C–C deformation), 750 cm−1 (Bz out-of-plane bending), 780 cm−1 (C–H out of plane bending), 826 cm−1 (C–C str), 942 cm−1 (imidazole in-plane bending), 1014 cm−1 (C–C–C trigonal bending), 1049 cm−1 (ring deformation in 5-member ring), 1342 cm−1 (C–H deformation in benzene ring), 1613 cm−1 (CC stretching mode). On the formation of complex, C2 from L2, the disappearance of charges on imidazole ring takes place which leads to diminishing polarity and consequently enhanced polarizability due to which a few peaks become relatively sharp, such as at 281 cm−1 more CH2 rocking occurs with C–C deformation at 370 cm−1 and at 1014 cm−1, C–C–C trigonal bending enhances in benzimidazole structure. The peak intensity at 1144 cm−1, 1175 cm−1 and 1354 cm−1 has been increased as well as shifted at higher wavenumbers to 1156 cm−1, 1183 cm−1 and 1369 cm−1 respectively, predicting strong C–H symmetric, in-plane bending and ring stretching vibrations in imidazole rings respectively. Moreover, the peak shift from 1253 cm−1 to 1269 cm−1 due to an in-plane benzene ring deformation in benzimidazole ring within selenium complex-II (C2). Similarly changes in peak position on the formation of C2 from L2, shift from 1283 cm−1 to 1293 cm−1, have been recognized as CH2 deformations in the aliphatic chain between two imidazole rings. A new shoulder band appearing at 1342 depicts C–H deformation in the benzene ring.
A strong peak at 1411 cm−1 is assigned to CSe vibrations in C2 as its counterpart feature is absent in the mean Raman spectrum of L2 which provides us with strong evidence of selenium complex formation while phenyl ring presence in only the second pair of ligand–complex (L2–C2) a peak at 1590 cm−1 has been allotted to C–C–C stretching mode of vibration in phenyl ring of side chains which is absent in other first and third ligand–complex pairs (L1–C1 and L3–C3).
On the other hand, relatively reduced intensities in C2 at some positions such as at 311 cm−1 (ring wag with chain twisting), 434 cm−1 and 474 cm−1 (C–C deformation), 548 cm−1 (wag mode of NO2), 627 cm−1 (in-plane C–C–C deformation), 780 cm−1 (C–H out of plane bending), 887 cm−1 (C–H out-of-plane bending), 942 cm−1 (imidazole in plane bending), 1049 cm−1 (ring deformation in 5-member ring), 1144 cm−1 (C–H symmetric bending benzimidazole), 1318 cm−1 (C–H deformation of CH2), 1354 cm−1 (ring stretch imidazole), the shift of 1434 cm−1 to 1448 cm−1 (CH deformation in side chain) and 1613 cm−1 (CC stretching mode) might be because, in contrast to alkyl side chains (electron-donating effect) in first and third pairs of ligands and complexes (L1–C1 and L3–C3), it has an electron-withdrawing group (nitrobenzene) as a side chain on benzimidazole rings which causes molecule towards somewhat reverse polar effect. Similarly, these Raman spectral features have been found in correspondence with the Raman spectral features calculated from DFT as in ESI as Fig. S2.†
Fig. 5 represents distinct mean Raman spectral features which are characteristic to some specific chemical structural parts of ligand-III (L3) and complex-III (C3). For instance, Raman spectral features at 331 cm−1 (ring wag + chain deformations), 421 cm−1 (ring rotation 5-member ring), 499 cm−1 (C–N out of plane bending), 532 cm−1 (C–N–C deformation aliphatic chain), 572 cm−1 (ring deformation), 609 cm−1 (C–C–C deformation in-plane vibration mode of benzene), 713 cm−1 (C–N out of plane stretching five-membered ring), 782 cm−1 (C–H out of plane bending), 1016 cm−1 (C–C–C trigonal bending), 1183 cm−1 (in-plane C–H bending), 1225 cm−1 (C–N stretching), 1260 cm−1 (in-plane bz ring deformation), 1342 cm−1 (C–H deformation in bz ring), 1354 cm−1 (ring stretch imidazole) and 1611 cm−1 (CC stretching mode) reflect the structural dissimilarities associated with benzimidazole.
Fig. 5 Comparison of mean Raman spectrum of ligand-III (L3) with mean Raman spectrum of complex-III (C3). |
The spectral features at 280 cm−1 and 293 cm−1 (CH2 rocking), 331 cm−1 (ring wagging and chain deformation), 713 cm−1 (C–N out of plane stretching in five-membered ring), 822 and 843 cm−1 (C–C stretching), 1137 cm−1 (C–C stretching, aliphatic vibration), 1183 cm−1 (in-plane C–H bending, benzimidazole), 1294 cm−1 (CH2 deformation, aliphatic chain) in C3 has been intensified. A similar justification goes for this increase in the intensity of some of the C3 Raman spectral features, as for the L1–C1 and L2–C2 ligand/complex pairs and can be associated with increased polarizability and decreased polarity in the complexes. Additional bands appear as well at 822 cm−1 (C–C stretching), 1342 cm−1 (C–H deformation in benzene ring) and 1412 cm−1 (CSe vibrations) which are the most distinguished features indicating stable selenium compound formation from its own salt. Changes in peak positions (shifts in peak positions) have also been observed at 1016 to 1023 cm−1 (C–C–C trigonal bending benzimidazole) and 1225 to 1214 cm−1 (C–N stretching benzimidazole) with an increase in intensity from L3 to C3.
Moreover, at some positions, in L3, few features disappeared or decreased in intensity in C3 as well, including 309 cm−1 (deformation vibrations of C–C–C), 532 cm−1 (C–N–C deformation aliphatic chain), 609 cm−1 (C–C–C deformation in-plane vibration mode of benzene), 782 cm−1 (C–H out of plane bending benzimidazole), 890 cm−1 (C–H out-of-plane bending), 1260 cm−1 (in-plane benzene ring deformation), 1313 cm−1 (C–H def of CH2), 1354 cm−1 (ring stretch imidazole) and shifting from 1433 to 1446 cm−1 (C–H deformation) and 1611 to 1617 cm−1 (CC stretching mode benzimidazole). In the same way, these Raman spectral features have great correspondence with the Raman spectral features calculated from DFT as shown in ESI in Fig. S3.†
Fig. 6(a) shows PCA scatter plot of Raman spectral data of ligand-I (black dots) and its respective selenium complex-I (green dots). Maximum variability in data has been explained by PC-1 explaining the dominant source of variability in the data which is 98.42% while PC-2 clarifies the rest of the variability. To explore the ability of PCA to distinguish ligand/salt samples from their respective complexes, PCA is used to identify and confirm the Raman spectral features associated with the differentiation of two different spectral data sets of ligands and their respective complex.
Fig. 6 (a) PCA scatter plot of Raman spectral data of ligand-I (black dots) and its respective selenium complex-I (green dots), (b) PCA loadings of Raman spectral data set of ligand-I and complex-I. |
Fig. 7(a) shows PCA scatter plot of Raman spectral data of ligand-II (black dots) and its respective selenium complex-II (green dots). In this case, the PC-1 predicts 98.88% variability and only 0.14% variability has been explained by PC-2.
Fig. 8(a) shows the PCA Scatter plot of Raman spectral data sets of ligand-III (black dots) and its respective selenium complex-III (green dots). PC-1 explains a maximum of 99.20% variability which indicates clear differentiation between the Raman spectral data sets of ligand-III and its respective complex.
As scatter plot has provided a chromatic display of two sets of data in two different clusters, but it is unable to provide reasons for such variability in data regarding distinct features. To understand this basis of discrimination in the PCA scatter plot, the loadings of PC-1 against wavenumber (cm−1) have been presented in Fig. 6(b), 7(b) and 8(b), for three different ligands and respective complexes, respectively. The reason for taking PC-1 for loadings is because it has provided maximum variability.
Fig. 6(b) presents the loadings of the PCA of Raman Spectral data sets of ligand-I (L1) compared with the complex-I (C1). The PC loadings are the dimensions of chemical variations, splitting different spectral groups of RS data along their variability. The positive loadings from the top side of the splitting line at zero are associated with the RS data of the ligands which have clusters on the right side in PC-1 of the scatter plot while the negative loadings are associated with the corresponding selenium complexes clustered at the negative side of PC-1. The loading plot expresses the only prominent features of ligands that are distinct from that of complexes. Such spectral loadings re-confirming the structural differences between ligands and their respective complexes as already have been discussed in mean Raman spectra. These differences indicate some kind of structural changes in complexes from their preliminary ligands and hence can be taken as Raman spectral markers of stable complex formation.
The dominant RS features of C1 that appeared in the PCA include 286 cm−1 (CH2 rocking), 331 cm−1 (imidazole ring wagging accompanied with the attached chains deformation), 713 cm−1 (C–N out of plane stretching vibrations of imidazole rings), 822 cm−1, 1130 cm−1, 1215 cm−1 and 1246 cm−1 (all probably associated with C–C stretching in aliphatic chains on both sides of imidazole rings), 967 cm−1 (CH3 wagging), 1186 cm−1 (C–H in-plane bending of benzimidazole ring) and 1297 cm−1 (CH2 deformation in the aliphatic chain). Another and highly differentiating feature at 1416 cm−1 has been attributed to CSe vibrations because of its only presence in a complex structure. In contrast, the most prominent positive loadings associated with ligand-I appear at 779 cm−1 (C–H out of plane bending in benzimidazole), 1019 cm−1 (C–C–C trigonal bending inbenzimidazole), 1138 cm−1 (C–C stretching), 1313 cm−1 and 1434 cm−1 (C–H def), 1351 cm−1 (ring stretch in imidazole) and 1610 cm−1 (CC stretching).
The PCA loadings of Raman spectral data sets of L2–C2 and L3–C3 pairs of ligands and complexes are shown in Fig. 7(b) and 8(b)) which reflect the same reasons of differentiation as has already been elaborated in the above section in the discussion related to Fig. 4 and 5 for ligand-II, &III and their complexes respectively. These unique features in Fig. 7(b) at 311, 345, 434, 474, 548, 627, 680, 780, 887, 942, 1049, 1144, 1318, 1354, 1434 and 1613 cm−1 while in Fig. 8(b) at 309, 532, 609, 782, 890, 1016, 1225, 1260, 1313, 1354, 1433 and 1611 cm−1 act as a fingerprint for a specific structural elucidation of L2 and L3. Similarly visible features at 281, 370, 595, 651, 750, 1014, 1156, 1183, 1269, 1293, 1342, 1369, 1411, 1485, and 1590 cm−1 in Fig. 7(b) and dominant features at 280, 331, 593, 713, 822, 1023, 1137, 1183, 11214, 1294, 1342, 1412 and 1489 cm−1 in Fig. 8(b) belonging to negative loadings enable description of stable metal–ligand bond which means complex formation and these results have also been found compatible with mean Raman spectra results.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra04931k |
‡ First two authors have equal contribution. |
This journal is © The Royal Society of Chemistry 2023 |