# Electronic Absorption Spectra of Some Triazolopyrimidine Derivatives

Authors: Hussein Moustafa; M. F. Shibl; Rifaat Hilal; Laila I. Ali; Sheimaa Abdel Halim
Journal: International Journal of Spectroscopy
 (2011)

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## Abstract

The electronic absorption spectra of  triazolo pyrimidine  and some of its derivatives were measured in polar as well as nonpolar solvents. Assignment of the observed transitions is facilitated via molecular orbital calculations. Charge density distributions, dipole moments, and the extent of delocalization of the MOS were used to interpret the observed solvent effects. The observed transitions are assigned as charge transfer (CT), localized, and delocalized according to the contribution of the various configurations in the CI-states. The correspondence between the calculated and experimental transition energies is satisfactory.


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## Body

## 1. Introduction

Pyrimidine and fused heterocyclic pyrimidine derivatives have attracted a great deal of interest due to their biochemical and pharmaceutical activities. Triazolopyrimidines, in particular, were tested for their medicinal, bactericidal, and fungicidal activity [1–3]. Wide variety of interesting biological activities were observed for those compounds, such as anticancer [4], antiviral [5], anti-H1V-1 activity [6], anti-inflammatory [7] and antimicrobial activities [8]. In addition, several substituted dihydronaphthothieno pyrimidine derivatives showed antimicrobial activities against Bacillus subtilis, Escherichia coli, Aspergillus niger, and Candida albicans [9], and their ester-containing derivatives demonstrated more antimicrobial activities than the corresponding cyano-containing analogs.The UV spectra of pyrimidines have been investigated [10]. The spectrum, in general, depends on the state of the nucleus, whether it is fully aromatic, partly reduced, or fully reduced and on the position, number, and nature of any chromophoric substituent attached to it. Furthermore, it also depends greatly on presence of ionic species in solution being measured. The UV absorption spectra of pyrimidines show two main band systems centered at 243 and 298 nm in cyclohexane. The second band is ascribed to an n-π* transition on account of the hypsochromic shift observed as changing solvent from cyclohexane to water. The lone pair become engaged in H-bonding in water so that the absorbed radiation must be of higher energy, that is, of lower wavelength. Loakes et al. [11, 12] studied the spectra of some triazolopyrimidines and discussed the effect of varying the acidity of the medium on the observed spectra. Effect of alkyl substitution on the spectra of some triazolopyrimidines was recently investigated [13] qualitatively.A detailed series of MO studies at the HMO level have been carried out on purines, pyrazolopyrimidines, triazolopyrimidines, and pyrazolopyrimidines [14–16]. The aim of such qualitative MO calculation is to ascertain the extent of aromaticity in the studied compounds. More recently, the electronic structure of a model triazolopyrimidine structure has been performed at the RHF and DFT levels of theory [17]. This study aimed at exploring the electronic structure of platinum complexes of triazolopyrimidines. A similar high level calculation has also been reported for the Ruthenium triazolopyrimidine complexes [18].In part I of this work [19], the ground state geometries of some Triazolopyrimidines were optimized at the density functional level of theory (DFT). Molecular structures were fully optimized using B3LYP/6-31G basis set. The effects of substituents on the geometry and electronic structural features of triazolo pyrimidine were examined.The electronic structure of molecules usually manifests itself in the electronic absorption and emission spectra. This manifestation enables the detailed understanding of the forces that govern the electronic structure of the studied Triazolopyrimidines. Although several investigations have been published that dealt with the electronic spectra of pyrimidines, yet there is no systematic study of substituents and solvent effects on the observed spectra. Such study is of critical importance in understanding their electronic structure that underlines their biological activity.The aim of our paper is to explore (1) the type and extent of conjugative interaction between different subsystems of Triazolopyrimidines, (2) the effect of solvent polarity on the observed spectra and, hence, predict the relative stabilities, extent of charge transfer character, and assignment of the observed electronic transitions, and (3) the effect of para-phenyl substitution, using electron-donating and withdrawing groups on the observed electronic spectra of Triazolopyrimidines.


## 2. Experimental

### 2.1. Compounds

Compounds studied were prepared and purified by standard procedures cited in the literature [20] see Scheme 1.Scheme 1


### 2.2. Solvents

Polar (methanol) and nonpolar (dioxane) solvents were obtained from Merck, AR-grade and were used without any further purification.


### 2.3. Apparatus

Spectra were scanned on a Perkin Elmer lambda 4B spectrophotometer using 1.0 cm fused silica cells. The machine records linearly in percent transmittance over the range 190–900 nm.


## 2.1. Compounds

Compounds studied were prepared and purified by standard procedures cited in the literature [20] see Scheme 1.Scheme 1


## 2.2. Solvents

Polar (methanol) and nonpolar (dioxane) solvents were obtained from Merck, AR-grade and were used without any further purification.


## 2.3. Apparatus

Spectra were scanned on a Perkin Elmer lambda 4B spectrophotometer using 1.0 cm fused silica cells. The machine records linearly in percent transmittance over the range 190–900 nm.


## 3. Method of Calculation

Molecular orbital calculations, employing full geometry optimization, were performed on the ground states of the molecules studied, at the DFT- B3LYP/6-31G [21, 22] level of theory using Gaussian  .03 program [23]. Excited states were treated theoretically using ZINDO/S [24].


## 4. Result and Discussion

### 4.1. The Electronic Absorption Spectra of(1)

The electronic absorption spectra in nonpolar (Dioxane) and polar (methanol) solvents are presented in Figure1. The charge density maps of the occupied and vacant MOs considered in the present analysis are presented in Figure 5. Tables 1 and 2 present a comparison of the experimentally observed and theoretically computed spectra in addition to a quantitative assignment of all transitions observed.Table 1
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-phenyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmfμPolarNonpolarλ, nmλ, nmI56-570.51933820.0015.675937537556–580.8130II56-570.8703500.5580.9529362360III56-570.9123200.76222.533832032556–590.6463000.14495.5869300301IV55–570.50354–570.520V56–590.8642860.043713.6527289298VI54–570.7752520.20828.5341248250VII55–580.4722230.04665.093321222354–580.759Table 2
State energies, configurations, type of transition, and assignment of all transitions for 3-Acetyl-1-phenyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I56-57π-π*Delocalized band3.313.2556–58π-π*Delocalized bandII56-57π-π*Delocalized band3.443.54III56-57π-π*Delocalized band3.823.8856–59π-π*CT: N- aryl →Triazolo-pyrimidineIV55–57π-π*CT: N- aryl →Triazolo-pyrimidine4.124.1354–57π-π*CT: N- aryl →Triazolo-pyrimidineV56–59π-π*Delocalized band4.164.34VI54–57π-π*CT: N- aryl →Triazolo-pyrimidine4.964.92VII55–58π-π*CT: N- aryl →Triazolo-pyrimidine5.565.5654–58π-π*CT: N- aryl →Triazolo-pyrimidineFigure 1
Electronic absorption spectra of(1).The spectrum, in dioxane, is composed of three main band systems. The long wavelength system is composed of two bands centered at 375 and 360 nm and the medium envelope composed of three bands centered at 325, 301, and 298 nm. The third band system is composed of two bands centered at 250 and 223 nm. Increasing solvent polarity causes blue shift of all observed bands. Furthermore, increasing solvent polarity causes a marked decrease in the intensity of all bands. All the observed bands may be assigned toπ-π* transitions as reflected from their intensities (4000–30000). This is in general agreement with previously published analysis of the spectra of triazoles [25].Excited configurations, considered in this paper, are those which result from an electron excitation between the highest three occupied molecular orbitalsΨ54–Ψ56 and the lowest three unoccupied molecular orbitals Ψ57–Ψ59. The configuration interaction matrix is solved, and the configuration interaction state functions are given in Table 1.The long wave length absorption band has been computed theoretically at 382 nm and composed of two configurations, namely,ϕ56-1ϕ57 and ϕ56-1ϕ58. The configuration ϕ56-1ϕ57 represents 27% of this state whereas ϕ56-1ϕ58 represents 66%. Both configurations are delocalized.The second (π,π*)1 state is computed theoretically at 350 nm which is in good agreement with the experimentally observed value of 360 nm. This state is composed of one configuration, namely, ϕ56-1ϕ57, and possesses the same polarity as the ground state, hence, shows no pronounced solvent effect.The third (π,π*)1 state is computed theoretically at 320 nm and composed of one configuration, ϕ56-1ϕ57. This band shows a blue shift on increasing solvent polarity, that is, solvent dependent. This is maybe attributed to the relatively high polarity of the excited state as compared to that of the ground state. This state may be assigned as a delocalized transition.The fourth (π,π*)1 state is computed theoretically at 300 nm. This state is composed of three configurations, namely, ϕ56-1ϕ59, ϕ55-1ϕ57, and ϕ54-1ϕ57. This state shows no solvent dependence and assigned as a charge transfer band (CT) from N-aryl to triazolo pyrimidine moiety.The fifth (π,π*)1 state computed at 298 nm in dioxane, 289 nm in methanol and is computed theoretically at 286 nm. This state possesses a high polarity as compared to that of the ground state (≈13.6 D), and hence solvent dependence on band position is expected. This state is also assigned as a delocalized transition.The last two states computed theoretically appear at 252 nm and 223 nm. Both states areπ-π* and assigned as CT bands from N-aryl to triazolo pyrimidine (c.f. Tables 1 and 2).


### 4.2. The Electronic Absorption Spectra of(2)

Figure2 presents the electronic absorption spectra of (2)in polar as well as nonpolar solvents. The spectrum, in nonpolar solvent, shows an envelope that covers the area 320–380 nm and contains two bands centered at 376 nm and 325 nm, and another envelope covers the area 220–280 nm showing two main bands centered at 275 nm and 225 nm. Increasing solvent polarity decreases the intensity of all observed bands with a red shift of the long wavelength 325 nm band in dioxane to 340 nm (≈15 nm). The three occupied MOs ψ57–ψ59 and two vacant MOs ψ60–ψ61 are considered in the CI computations. Tables 3 and 4 compare the experimentally observed and theoretically computed transitions, assignment, configurations involved and their coefficients. The (π,π*)1 states observed experimentally are well reproduced theoretically. All the observed transition are π-π* as indicated from their intensities (4000–20000).Table 3
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-p-tolyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmFμPolarNonpolarλ, nmλ, nmI59-600.8133710.56125.244937537659–610.484II59-600.8973260.83624.1182340325III59–610.8952740.58138.5551275275IV58–610.5562240.02734.916822022557–610.653Table 4
State energies, configurations, type of transition, and assignment of all transitions for 3-Acetyl-1-p-tolyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I59-60π-π*Delocalized band3.303.3459–61π-π*Delocalized bandII59-60π-π*Delocalized band3.823.80III59–61π-π*Delocalized band4.514.53IV58–61π-π*CT: N- aryl → Triazolo-pyrimidine,5.515.5457–61π-π*CT: N- aryl → Triazolo-pyrimidineFigure 2
Electronic absorption spectra of(2).The first (π,π*)1 is transition centered at 371 nm is composed of two configurations, namely, ψ59-1ψ60 and ψ59-1ψ61. Both configurations are assigned as delocalized bands.The second (π,π*)1 computed theoretically at 326 nm and composed of only one configuration, ψ59-1ψ60. This state is much more polar than the ground state and is expected to show solvent dependence (≈15 nm).The last two bands are computed theoretically at 274 nm and 224 nm which agree with the experimentally observed spectra in both polar and nonpolar solvents. The band at 274 nm may be assigned as a delocalized transition whereas the band at 224 is assigned to a CT transition from the N-aryl moiety to the triazolo pyrimidine subsystem (cf. Tables4 and 5).Table 5
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-(4-methoxy-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmFμPolarNonpolarλ, nmλ, nmI62-630.85053610.52345.0213368355II62–640.79533260.308610.1508312313III61–630.839263.50.358410.6888262263IV61–630.8452280.054315.9894227225


### 4.3. The Electronic Absorption Spectra of(3)

Figure3 presents the electronic spectra of (3) in methanol and dioxane as solvents. The spectrum in dioxane is composed of two long wavelength bands centered at 355 nm and 313 nm and two short wavelength bands centered at 263 nm and 225 nm. The spectrum, in methanol, is similar to that of dioxane except that the long wavelength band shows a marked red shift of about 13 nm. All observed transitions may be assigned to be π-π* transition as reflected from their intensities (8000–26000). The effect of OCH3 substitution on the observed spectrum is intensification and slight perturbation of band position, a typical behavior due to its inductive effect.Figure 3
Electronic absorption spectra of(3).The long wavelength band computed theoretically centered at 361 nm is composed of one configuration,ψ62-1ψ63, and is assigned as a delocalized band. All the observed transitions are predicted theoretically. The assignments of all transition are listed in Tables 5 and 6.Table 6
State energies, configurations, type of transition, and assignment of all transitions for 3-Acetyl-1-(4-methoxy-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I62-63π-π*Delocalized band3.493.43II62–64π-π*Delocalized band3.963.80III61–63π-π*CT: N- aryl → Triazolo-pyrimidine4.714.71IV61–63π-π*CT: N- aryl → Triazolo-pyrimidine5.515.44


### 4.4. The Electronic Absorption Spectra of(4)

The methyl and methoxy groups are electron donor groups, whereas Cl-atom is an electron donor by its mesomeric effect and is an electron acceptor by its inductive effect. The electronic spectra of(4) in polar and nonpolar solvents are presented in Figures 4(a) and 4(b). The state energies, assignment, type of electronic transition, theoretically computed and experimentally observed band energies are given in Tables 7 and 8.Table 7
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-(4-chloro-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmfμPolarNonpolarλ, nmλ, nmI59-600.4473770.0017.3992—37459–610.824II59-600.8943550.65533.0741358355III59-610.8303100.29247.0622304305IV59–620.9192800.07924.2378298290V56–600.7672430.35836.4620250250VI57–600.6882240.358512.066722722857–620.697Table 8
State energies, configurations, type of transition, and assignment of all transitions of 3-Acetyl-1-(4-chloro-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I59-60π-π*Delocalized band3.323.2959–61π-π*Localized bandII59-60π-π*Delocalized band3.493.49III59–61π-π*Localized band4.074.00IV59–62π-π*CT: N- aryl → Triazolo-pyrimidine4.284.43V56–60π-π*CT: N- aryl → Triazolo-pyrimidine4.965.10VI57–60π-π*CT: N- aryl → Triazolo-pyrimidine5.445.5457–62π-π*CT: N- aryl → Triazolo-pyrimidineFigure 4
Electronic absorption spectra of(4).Figure 5
The charge density maps of the occupied and vacant MOs for1.The spectrum in dioxane show six bands centered at 374 nm, 355 nm, 305 nm, 290 nm, 250 nm, and 228 nm, whereas the spectrum in methanol shows bands centered at 358 nm, 304 nm, 298 nm, 250 nm, and 227 nm. The band at 374 nm in dioxane does not appear in methanol due to the low solubility of the compound. Increasing solvent polarity, on going from dioxane to methanol, decreases the intensities of all bands with a red shift of the band at 290 in dioxane to 298 nm in methanol (≈9 nm). The assignment and coefficient of each configuration in every state are given in Tables 7 and 8.The long wavelength bands, corresponding to states I, II, and III, are localized and delocalized bands, whereas states IV, V, and VI show considerable charge transfer character from N-aryl to triazolopyrimidine.


## 4.1. The Electronic Absorption Spectra of(1)

The electronic absorption spectra in nonpolar (Dioxane) and polar (methanol) solvents are presented in Figure1. The charge density maps of the occupied and vacant MOs considered in the present analysis are presented in Figure 5. Tables 1 and 2 present a comparison of the experimentally observed and theoretically computed spectra in addition to a quantitative assignment of all transitions observed.Table 1
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-phenyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmfμPolarNonpolarλ, nmλ, nmI56-570.51933820.0015.675937537556–580.8130II56-570.8703500.5580.9529362360III56-570.9123200.76222.533832032556–590.6463000.14495.5869300301IV55–570.50354–570.520V56–590.8642860.043713.6527289298VI54–570.7752520.20828.5341248250VII55–580.4722230.04665.093321222354–580.759Table 2
State energies, configurations, type of transition, and assignment of all transitions for 3-Acetyl-1-phenyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I56-57π-π*Delocalized band3.313.2556–58π-π*Delocalized bandII56-57π-π*Delocalized band3.443.54III56-57π-π*Delocalized band3.823.8856–59π-π*CT: N- aryl →Triazolo-pyrimidineIV55–57π-π*CT: N- aryl →Triazolo-pyrimidine4.124.1354–57π-π*CT: N- aryl →Triazolo-pyrimidineV56–59π-π*Delocalized band4.164.34VI54–57π-π*CT: N- aryl →Triazolo-pyrimidine4.964.92VII55–58π-π*CT: N- aryl →Triazolo-pyrimidine5.565.5654–58π-π*CT: N- aryl →Triazolo-pyrimidineFigure 1
Electronic absorption spectra of(1).The spectrum, in dioxane, is composed of three main band systems. The long wavelength system is composed of two bands centered at 375 and 360 nm and the medium envelope composed of three bands centered at 325, 301, and 298 nm. The third band system is composed of two bands centered at 250 and 223 nm. Increasing solvent polarity causes blue shift of all observed bands. Furthermore, increasing solvent polarity causes a marked decrease in the intensity of all bands. All the observed bands may be assigned toπ-π* transitions as reflected from their intensities (4000–30000). This is in general agreement with previously published analysis of the spectra of triazoles [25].Excited configurations, considered in this paper, are those which result from an electron excitation between the highest three occupied molecular orbitalsΨ54–Ψ56 and the lowest three unoccupied molecular orbitals Ψ57–Ψ59. The configuration interaction matrix is solved, and the configuration interaction state functions are given in Table 1.The long wave length absorption band has been computed theoretically at 382 nm and composed of two configurations, namely,ϕ56-1ϕ57 and ϕ56-1ϕ58. The configuration ϕ56-1ϕ57 represents 27% of this state whereas ϕ56-1ϕ58 represents 66%. Both configurations are delocalized.The second (π,π*)1 state is computed theoretically at 350 nm which is in good agreement with the experimentally observed value of 360 nm. This state is composed of one configuration, namely, ϕ56-1ϕ57, and possesses the same polarity as the ground state, hence, shows no pronounced solvent effect.The third (π,π*)1 state is computed theoretically at 320 nm and composed of one configuration, ϕ56-1ϕ57. This band shows a blue shift on increasing solvent polarity, that is, solvent dependent. This is maybe attributed to the relatively high polarity of the excited state as compared to that of the ground state. This state may be assigned as a delocalized transition.The fourth (π,π*)1 state is computed theoretically at 300 nm. This state is composed of three configurations, namely, ϕ56-1ϕ59, ϕ55-1ϕ57, and ϕ54-1ϕ57. This state shows no solvent dependence and assigned as a charge transfer band (CT) from N-aryl to triazolo pyrimidine moiety.The fifth (π,π*)1 state computed at 298 nm in dioxane, 289 nm in methanol and is computed theoretically at 286 nm. This state possesses a high polarity as compared to that of the ground state (≈13.6 D), and hence solvent dependence on band position is expected. This state is also assigned as a delocalized transition.The last two states computed theoretically appear at 252 nm and 223 nm. Both states areπ-π* and assigned as CT bands from N-aryl to triazolo pyrimidine (c.f. Tables 1 and 2).


## 4.2. The Electronic Absorption Spectra of(2)

Figure2 presents the electronic absorption spectra of (2)in polar as well as nonpolar solvents. The spectrum, in nonpolar solvent, shows an envelope that covers the area 320–380 nm and contains two bands centered at 376 nm and 325 nm, and another envelope covers the area 220–280 nm showing two main bands centered at 275 nm and 225 nm. Increasing solvent polarity decreases the intensity of all observed bands with a red shift of the long wavelength 325 nm band in dioxane to 340 nm (≈15 nm). The three occupied MOs ψ57–ψ59 and two vacant MOs ψ60–ψ61 are considered in the CI computations. Tables 3 and 4 compare the experimentally observed and theoretically computed transitions, assignment, configurations involved and their coefficients. The (π,π*)1 states observed experimentally are well reproduced theoretically. All the observed transition are π-π* as indicated from their intensities (4000–20000).Table 3
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-p-tolyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmFμPolarNonpolarλ, nmλ, nmI59-600.8133710.56125.244937537659–610.484II59-600.8973260.83624.1182340325III59–610.8952740.58138.5551275275IV58–610.5562240.02734.916822022557–610.653Table 4
State energies, configurations, type of transition, and assignment of all transitions for 3-Acetyl-1-p-tolyl-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I59-60π-π*Delocalized band3.303.3459–61π-π*Delocalized bandII59-60π-π*Delocalized band3.823.80III59–61π-π*Delocalized band4.514.53IV58–61π-π*CT: N- aryl → Triazolo-pyrimidine,5.515.5457–61π-π*CT: N- aryl → Triazolo-pyrimidineFigure 2
Electronic absorption spectra of(2).The first (π,π*)1 is transition centered at 371 nm is composed of two configurations, namely, ψ59-1ψ60 and ψ59-1ψ61. Both configurations are assigned as delocalized bands.The second (π,π*)1 computed theoretically at 326 nm and composed of only one configuration, ψ59-1ψ60. This state is much more polar than the ground state and is expected to show solvent dependence (≈15 nm).The last two bands are computed theoretically at 274 nm and 224 nm which agree with the experimentally observed spectra in both polar and nonpolar solvents. The band at 274 nm may be assigned as a delocalized transition whereas the band at 224 is assigned to a CT transition from the N-aryl moiety to the triazolo pyrimidine subsystem (cf. Tables4 and 5).Table 5
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-(4-methoxy-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmFμPolarNonpolarλ, nmλ, nmI62-630.85053610.52345.0213368355II62–640.79533260.308610.1508312313III61–630.839263.50.358410.6888262263IV61–630.8452280.054315.9894227225


## 4.3. The Electronic Absorption Spectra of(3)

Figure3 presents the electronic spectra of (3) in methanol and dioxane as solvents. The spectrum in dioxane is composed of two long wavelength bands centered at 355 nm and 313 nm and two short wavelength bands centered at 263 nm and 225 nm. The spectrum, in methanol, is similar to that of dioxane except that the long wavelength band shows a marked red shift of about 13 nm. All observed transitions may be assigned to be π-π* transition as reflected from their intensities (8000–26000). The effect of OCH3 substitution on the observed spectrum is intensification and slight perturbation of band position, a typical behavior due to its inductive effect.Figure 3
Electronic absorption spectra of(3).The long wavelength band computed theoretically centered at 361 nm is composed of one configuration,ψ62-1ψ63, and is assigned as a delocalized band. All the observed transitions are predicted theoretically. The assignments of all transition are listed in Tables 5 and 6.Table 6
State energies, configurations, type of transition, and assignment of all transitions for 3-Acetyl-1-(4-methoxy-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I62-63π-π*Delocalized band3.493.43II62–64π-π*Delocalized band3.963.80III61–63π-π*CT: N- aryl → Triazolo-pyrimidine4.714.71IV61–63π-π*CT: N- aryl → Triazolo-pyrimidine5.515.44


## 4.4. The Electronic Absorption Spectra of(4)

The methyl and methoxy groups are electron donor groups, whereas Cl-atom is an electron donor by its mesomeric effect and is an electron acceptor by its inductive effect. The electronic spectra of(4) in polar and nonpolar solvents are presented in Figures 4(a) and 4(b). The state energies, assignment, type of electronic transition, theoretically computed and experimentally observed band energies are given in Tables 7 and 8.Table 7
Calculated and observed band maxima, intensities, and dipole transition of 3-Acetyl-1-(4-chloro-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateTheoreticalExperimentalConfigurationCoefficientλ, nmfμPolarNonpolarλ, nmλ, nmI59-600.4473770.0017.3992—37459–610.824II59-600.8943550.65533.0741358355III59-610.8303100.29247.0622304305IV59–620.9192800.07924.2378298290V56–600.7672430.35836.4620250250VI57–600.6882240.358512.066722722857–620.697Table 8
State energies, configurations, type of transition, and assignment of all transitions of 3-Acetyl-1-(4-chloro-phenyl)-1H-[1, 2, 4] triazolo [3, 4-b] quinazolin-5-one.
StateConfigurationTypeAssignment∆E, eVObs.Calc.I59-60π-π*Delocalized band3.323.2959–61π-π*Localized bandII59-60π-π*Delocalized band3.493.49III59–61π-π*Localized band4.074.00IV59–62π-π*CT: N- aryl → Triazolo-pyrimidine4.284.43V56–60π-π*CT: N- aryl → Triazolo-pyrimidine4.965.10VI57–60π-π*CT: N- aryl → Triazolo-pyrimidine5.445.5457–62π-π*CT: N- aryl → Triazolo-pyrimidineFigure 4
Electronic absorption spectra of(4).Figure 5
The charge density maps of the occupied and vacant MOs for1.The spectrum in dioxane show six bands centered at 374 nm, 355 nm, 305 nm, 290 nm, 250 nm, and 228 nm, whereas the spectrum in methanol shows bands centered at 358 nm, 304 nm, 298 nm, 250 nm, and 227 nm. The band at 374 nm in dioxane does not appear in methanol due to the low solubility of the compound. Increasing solvent polarity, on going from dioxane to methanol, decreases the intensities of all bands with a red shift of the band at 290 in dioxane to 298 nm in methanol (≈9 nm). The assignment and coefficient of each configuration in every state are given in Tables 7 and 8.The long wavelength bands, corresponding to states I, II, and III, are localized and delocalized bands, whereas states IV, V, and VI show considerable charge transfer character from N-aryl to triazolopyrimidine.


## 5. Summary and Conclusion

The present analysis of the electronic absorption spectra of the studied Triazolopyrimidines indicates clearly the following.(1)
The spectra are diffuse and reflect the complexity of the molecular forces in this series of molecules. Conjugation extents all over the entire molecular frame work.(2)
The spectra are both solvent and substituent sensitive. Spectra in methanol are, in general, diffuse and less resolved. In case of the parent compound1, the two long wavelength envelopes do not show significant solvent dependence. On the other hand, the short wavelength band systems show marked red shift by increasing solvent polarity. The origin of this shift can be understood by inspecting the charge density maps for the MOs 56 and 59. The occupied MO 56 is localized to a great extent on the phenyl moiety whereas 59 is localized on the quinazolin subsystem. This charge transfer interaction stabilizes the excited state and thus causes the red shift.(3)
The methyl derivative2shows the same behavior as the parent compound1. On the other hand, the methoxy derivative3 shows the opposite trend. Thus, the two band systems are solvent dependent where a marked blue shift is observed. Furthermore, an increase of band intensity is also marked for the short wave length band system. This behavior can be attributed to H-bonding. This blue shift may indicate a specific solute-solvent interaction due to a hydrogen bond between the oxygen atom of the methoxy group and the alcohol OH [26]. Jankulovska et al. [27] in their recent analysis of solvatochromic effects pinpoint the need for a complete model and detailed analysis of the effect of protic solvents. The data at hand is not sufficient for such analysis. Theoretical modelling of solvent-solute interaction seems also necessary [28]. Such analysis will be the subject of future study.(4)
Increasing solvent polarity has thus the general effect of diffusing the observed band envelopes and reducing their intensity. This may be attributed to marked solvent-solute interaction rather than just dipolar effect.(5)
Electron-donating substituents, –CH3 and –OCH3, show the one and same trend. The long wavelength envelope is diffuse and can only be resolved into one peak. It is interesting to note that the –CH3 derivative shows its long wavelength peak at 376 nm whereas that for the –OCH3 derivative is at 355 nm. The second band system shows almost the same trend. Only one peak is observed whose position is blue shifted by 12 nm in case of the –OCH3 as compared to the –CH3 derivative.



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*Source: 394948-2011-04-26.xml*