Journal of Spectroscopy

Volume 2013 (2013), Article ID 408506, 13 pages

http://dx.doi.org/10.1155/2013/408506

Research Article

Binding of Coumarin 334 with β-Cyclodextrin and with C-Hexylpyrogallol[4]arene: Opposite Fluorescence Behavior

Chandrasekaran Sowrirajan and Enoch Israel Vijayaraj Muthu Vijayan

Department of Chemistry, Karunya University, Coimbatore, Tamil Nadu 641 114, India

Received 26 May 2013; Revised 19 August 2013; Accepted 22 August 2013

Academic Editor: Piotr Przybylski

Copyright © 2013 Chandrasekaran Sowrirajan and Enoch Israel Vijayaraj Muthu Vijayan. 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.

Abstract.

We report here the structure of the host-guest complexes of Coumarin 334 (C334) with β-cyclodextrin (β-CD) and with C-hexylpyrogallol[4]arene (C-HPA) and the effect of acidity on the neutral-cation equilibrium of C334 in water and in the presence of the host molecules. The structures of the host-guest complexes are proposed on the basis of the change of fluorescence on the addition of β-CD or C-HPA to C334 and by 2D ROESY spectroscopy. Opposite fluorescence behaviors, that is, quenching of fluorescence in β-CD and enhancement of fluorescence in C-HPA are observed. Time-resolved fluorescence analysis is done for the complexation, and biexponential decay pattern is observed. The possible strong inclusion complexation with C-HPA is explained. The ground and the excited state values for the protonation equilibrium of C334 in water and the difficulty of protonation in the presence of the host molecules are discussed.

1. Introduction

Being well-known laser dyes, with intriguing electronic and photonic properties suitable for many technological applications, Coumarin dyes have been extensively used to study the dynamics of several chemical and photochemical processes [1–6]. The photophysical behavior of Coumarin dyes is an active area of research [7–11]. The absorption and emission maxima of the aminocoumarins are very sensitive to the solvent polarity. Due to this property, many researchers have used aminocoumarin dyes as fluorescence probes in studying many physicochemical processes [12–15]. Multiwavelength laser sources, dye laser, have advantages such as low cost and high conversion efficiency [16, 17]. Photophysical properties of Coumarin dyes have been extensively studied for the past several years [18–21]. Coumarin and its metabolites are nonmutagenic [22]. Coumarins have also been reported to have biomedical applications [23–25]. Coumarin 334 (C334), chemically known as 10-acetyl-2,3,6,7-tetrahydro-1H,5H,11H-1-benzopyrano[6,7,8-ij]quinolizin-11-one, is a laser dye with rigid structure which is a well-known fluorophore [26], and its structure is shown in Figure 1(a). Since, as mentioned above, Coumarin dyes offer room for the extensive study of their properties in various environments, and the properties of C334 have not been explored in the presence of confined space like cyclodextrin, we have chosen it for the present study.

(a)

(b)

(c)

Figure 1: (a) Structure of C334. (b) Structure of β-CD. (c) Structure of C-HPA.

Cyclodextrins, which are naturally occurring cyclo-oligosaccharides mainly containing 6 to 8 glucopyranose moieties (α-, β-, and γ-cyclodextrin, resp.), provide space for molecular encapsulation since they have a hydrophobic inner cavity with a capacity to encapsulate small organic molecules [27–30]. These molecules are soluble in water due to the presence of primary and secondary hydroxyl groups to the exterior and also increase the water solubility of the corresponding host-guest complexes. Pyrogallol[4]arenes, a class of calixarenes containing pyrogallol units, form hexameric capsules in the solid state [31] as well as in solution in the presence of specific guests [32]. Cyclodextrins and calixarenes as host structures differ in some important aspects; that is, calixarenes are made of aromatic rings flexible at their connecting bonds and prone to flipping, whereas the glucopyranose units in cyclodextrins remain rigid. These host molecules encapsulating the guests need to be investigated in detail as the stoichiometry, the binding constant, and the mode of binding can decide various the physicochemical and the excited state properties of the guest molecules. The structural representation of β-cyclodextrin (β-CD) and C-hexylpyrogallol[4]arene (C-HPA) is given in Figures 1(b) and 1(c), respectively.

In this paper, we report (i) the stoichiometry and the strength of binding of C334 with β-CD and with C-HPA, (ii) the mode of binding of the guest with the hosts, and (iii) the effect of acidity on C334 and the influence of the molecular encapsulators on the prototropic equilibrium of C334. We used two-dimensional ROESY NMR spectroscopy [33] for characterizing the structure of the host-guest complexes of C334 with β-CD and C-HPA, the absorption spectroscopy, and the fluorescence spectroscopy for the understanding the mode and the strength of binding.

2. Experimental

2.1. Chemicals and Solvents

β-Cyclodextrin and Coumarin 334 were purchased respectively from Hi Media and Sigma-Aldrich and used as received. Phosphoric acid and sodium hydroxide, used for adjustment of pH, were products of Qualigens. A modified Hammett’s acidity scale [34] was used for the measurement of and pH below 2. C-Hexylpyrogallol[4]arene was prepared, by the reaction of heptaldehyde and pyrogallol (products of Sigma-Aldrich), following the literature procedure [34]. All the solvents used (Merck) were of spectral grade which were used as received.

2.2. Preparation of C334-β-CD and C334-C-HPA Solid Complexes

C334 (0.35 g, 1.24 mmol) was dissolved in acetonitrile, and an equimolar amount of β-CD (1.40 g) was dissolved in doubly distilled water in 50 mL beakers separately. A solution of C334 was added slowly to the solution of β-CD at room temperature in an Ultra-sonicator and maintained for 30 min. Then the mixture was warmed to 50°C for 10 min and kept at room temperature for two days. The solid obtained was collected and analyzed.

An equimolar amount of C334 (0.3 g, 1.05 mmol) and C-HPA (0.94 g) was dissolved in methanol in 50 mL beakers separately. A solution of C334 was added slowly to the solution of C-HPA at room temperature in an Ultra-sonicator and maintained for 30 min. Then, the mixture was warmed to 50°C for 10 min and kept at room temperature for two days. The obtained solid was collected and analyzed.

2.3. Preparation of Test Solutions

Test solutions were prepared by appropriate dilution from a stock solution of 1.7647 × 10⁻⁴ mol dm⁻³ of C334. Owing to the poor solubility of C334 in water, the stock solution was made in methanol. The test solutions were having the concentration of methanol as 1%. Stock solutions of the β-CD in the concentration of 1.2 × 10⁻² mol dm⁻³ and a stock solution of 2 × 10⁻⁵ mol dm⁻³ of CHPA were used for the preparation of test solutions. Various concentrations of sulfuric acid (0.25, 0.5, 1.0, 2.0, 3.0, and 4.0 mol dm⁻³) were used to vary the acid strength, and values were interpreted from a modified Hammett’s acidity scale. All reagents and solvents were of spectral grade which were used without further purification. Doubly distilled water was used throughout the experiments. All experiments were carried out at ambient temperature of °C. The test solutions were homogeneous after all additives were added, and the absorption and the fluorescence spectra were recorded against appropriate blank solutions.

2.4. Instrumentation

Absorption measurements were performed with a double beam UV-visible spectrophotometer (Jasco-V 630) using 1 cm path length cells. A spectrofluorimeter (Perkin-Elmer LS55) equipped with a 120 W Xenon lamp for excitation served the measurement of fluorescence. Both the excitation and the emission bandwidths were set up at 4 nm. Time-resolved fluorescence measurements were done on a time-correlated single photon counting spectrofluorometer (Jobin-Yvon IBH, Ti Saphhire Laser-Spectraphysics, LED Source: 470 nm ps-ns resolution). Ultra-sonicator PCI 9L 250H, India, was used for sonication. pH studies were carried out using Elico LI 120 pH meter, India. 2D ROESY spectra were recorded on a Bruker AV III instrument operating at 500 MHz with DMSO-d₆ as solvent for C334-β-CD complex and CDCl₃ for C334-C-HPA complex. The chemical shift values are reported in ppm. Tetramethylsilane (TMS) was used as an internal standard. The chemical shift values were obtained downfield from TMS in part per million (ppm). The 2D ROESY experiments were performed on the prepared solid complexes of C334-β-CD and C334-C-HPA. The mixing time for ROSEY spectra was 200 ms under the spin lock condition.

3. Results and Discussion

3.1. The Study of Complexation of C334 with β-CD or C-HPA

The absorbance spectra of C334 in the varying concentrations (0 to 1.2 × 10⁻² mol dm⁻³) of β-CD are shown in Figure 2(a). The absorbance increases with the increase in the amount of β-CD with a marked and continuous red shift to a final 7 nm. The absorbance and the fluorescence spectral data for the interaction of C334 with β-CD are given in Table 1. This is quite opposed to the usual blue shift of absorbance on complexation with β-CD [30]. The blue shift is expected as the molecule dislodges from a polar solvent environment to the nonpolar cavity of β-CD when it forms an inclusion complex. The red shift we observe in the present case of C334 may be due to the surfactant action of β-CD on C334 surrounding and possibly forming hydrogen bonds with it. The magnitude of red shift is significantly large as the C334 molecule itself is polar [35]. The absorbance increases indicating that sufficiently strong interaction between C334 and β-CD indeed occurs. The observed absorption spectral data were used in the following equation:

Table 1: Absorption and fluorescence spectral data of C334 with various amounts of β-CD.

Concentration of -CD, mol dm⁻³
Absorption maximum, nm
Absorbance, a.u.
Emission maximum, nm

0
461.0
0.0638
503.0

1.0 × 10⁻³
464.0
0.0637
504.0

2.0 × 10⁻³
468.0
0.0655
504.0

8.0 × 10⁻³
468.0
0.0717
504.0

1.0 × 10⁻²
468.0
0.0783
504.0

1.2 × 10⁻²
468.0
0.0832
504.0

Excitation wavelength: 461 nm.

(a)

(b)

(c)

(d)

Figure 2: (a) Absorbance spectra of C334 with varying concentrations of β-CD. (b) 1/ versus 1/[β-CD] plot of C334-β-CD complex. (c) Fluorescence spectra of C334 with varying concentrations of β-CD. (d) Stern-Volmer plot of C334-β-CD complex.

Here, is the intensity of absorbance of C334 in water, is the intensity of absorbance at the various concentrations of β-CD, is the intensity of absorbance at the highest concentration of β-CD, and is the binding constant. The plot between 1/() and 1/[β-CD] is shown in Figure 2(b). The 1 : 1 stoichiometry was observed by the linearity in the plot with the correlation coefficient () 0.9954, and the binding constant () was calculated as 99.11 mol⁻¹ dm³.

Figure 2(c) shows the fluorescence spectra of C334 with varying amounts of β-CD in solution. Upon the addition of β-CD, the fluorescence of C334 is starting to get quenched and the quenching continues up to the maximum concentration of β-CD. This is quite opposite to the usual enhancement of fluorescence on β-CD complexation of fluorophores. Hence, the fluorophore may not form an inclusion complex. Moreover, the expected blue shift is not observed. Instead, we observe a 1 nm red shift (although weak). The Stern-Volmer plot [36] by using (2), made for the quenching of fluorescence of C334 by β-CD, is shown in Figure 2(d). The quenching constant, , [37] is calculated from (3). The quenching constant was calculated as 4.66 × 10⁹ mol⁻¹ dm³ sec⁻¹.

Consider the following:

where is the lifetime of the quencher.

The time-resolved fluorescence profiles of C334 in the presence and absence of β-CD are shown in Figure 3. Table 2 lists out the time-resolved fluorescence spectral data of C334 in the presence and absence of β-CD. The biexponential decay of C334 having (1.03 ns) and (3.05 ns) with relative amplitude 60.79 and 39.21 is not significantly altered upon the addition of β-CD; that is, the tri-exponential decay can be expected which, in this case, is not observed.

Table 2: Time-resolved fluorescence spectral data of C334 in water and in β-CD.

Concentration of -CD, mol dm⁻³
Energy states
Lifetime (s)
Relative amplitude

Standard deviation (s)

0
T1
1.03 × 10⁻⁹
60.79
1.14
2.10 × 10⁻¹¹

T2
3.05 × 10⁻⁹
39.21
4.12 × 10⁻¹¹

1.0 × 10⁻³
T1
1.16 × 10⁻⁹
63.52
1.02
1.85 × 10⁻¹¹

T2
3.57 × 10⁻⁹
36.48
3.88 × 10⁻¹¹

Excitation wavelength: 470 nm.

Emission wavelength: 504 nm.

Figure 3: Time-resolved fluorescence spectra of C334 in β-CD.

The ¹H NMR spectral values of β-CD, C334, and C-HPA are given in Table 3. In the ¹H NMR spectrum of C334-β-CD inclusion complex, the H4 proton in the chromone ring resonates at 8.34 ppm. The aromatic proton of C334 resonates at 7.24 ppm. In the quinolizidine ring, the signals due to methylene protons of 10 and 12 which are attached to the tertiary nitrogen are observed at 3.30 ppm which is very close to that of the H4 signal of β-CD at 3.33 ppm. The other methylene protons at positions 8 and 14 are deshielded to 2.71 ppm as well as 9 and 13 protons observed upfield at 1.88 ppm.

Table 3: 1H NMR spectral data of β-CD, C334, and C-HPA.

-CD
C334
C-HPA

Position of protons
Chemical shift, (ppm)
Nature of protons
Position of protons
Chemical shift, (ppm)
Nature of protons
Chemical shift, (ppm)

H3
3.30
Methyl protons
21
2.62
C-Hexyl chain

H4
3.33
Chromone proton
4-CH
8.35
Methyl protons
0.93

H2
3.56
Aromatic proton
17-CH
7.24
Methylene protons
1.28–1.45

H6
3.60
Methylene protons
9 and 13
1.90
CH in the linked pyrogallol units
2.21–2.28

H5
3.64
Methylene protons
8 and 14
2.69

Primary hydroxyl
4.46
Methylene protons
10 and 12
3.33
Aromatic ring

H1
4.83

Aromatic protons
7.49

Secondary hydroxyl
5.68 and 5.74

Hydroxyl protons
6.86, 6.90, and 8.80

Figure 4 shows the 2D ROESY NMR spectrum of C334-β-CD solid inclusion complex. There are cross peaks observed for the interaction of C334 methylene protons in hexahydroquinolizidine ring with the H1, H4, H5, and H6 protons and hydroxyl groups of β-CD. The cross peak indicated by the circle corresponds to the interaction of 8 and 14 methylene protons of C334 with H4 proton of β-CD. The cross peaks marked by the rectangle correspond to the 9 and 13 methylene protons of C334 interacting with the H4 proton and hydroxyl groups of β-CD. The H6, H5, and H1 protons of β-CD correlate with the 10 and 12 methylene protons of C334 (marked by a triangle) and the same protons cross-correlated with the primary hydroxyl groups of β-CD are denoted as the diamond symbol. From these correlation peaks, it is evident that the C334-β-CD interaction occurs with the hexahydroquinolizidine ring of C334 interacting with β-CD.

Figure 4: 2D ROESY NMR spectrum showing C334-β-CD complex.

Figure 5(a) shows the absorption spectra of C334 with the increasing concentrations from 0 to 5.77 × 10⁻⁶ mol dm⁻³ of C-HPA. The absorption spectral data are compiled in Table 4. The absorbance increases upon increasing the concentration of C-HPA. Additionally, a blue shift of 3 nm is observed in the absorption spectrum due to the influence of C-HPA. The blue shift is a characteristic of inclusion complexation with a hydrophobic cavity engulfing fluorophores. The 1 : 1 stoichiometry was observed from (1), and the linear plot is shown in Figure 5(b) with the correlation coefficient () 0.97, and the calculated binding constant () was 9.5 × 10⁵ mol⁻¹ dm³.

Table 4: Absorption and fluorescence spectral data of C334 with various amounts of C-HPA.

Concentration of C-HPA, mol dm⁻³
Absorption maximum, nm
Absorbance, a.u.
Emission maximum, nm

0
462.0
0.0252
504.0

1.77 × 10⁻⁶
461.0
0.0320
504.0

2.57 × 10⁻⁶
460.0
0.0370
504.0

3.37 × 10⁻⁶
460.0
0.0402
503.0

4.17 × 10⁻⁶
460.0
0.0415
503.0

4.97 × 10⁻⁶
460.0
0.0450
503.0

5.77 × 10⁻⁶
459.0
0.0474
503.0

Excitation wavelength: 461 nm.

(a)

(b)

(c)

(d)

Figure 5: (a) Absorbance spectra of C334 with varying concentrations of C-HPA. (b) 1/ versus 1/[C-HPA] plot of C334-C-HPA complex. (c) Fluorescence spectra of C334 at different concentrations of C-HPA. (d) Nonlinear plot for the increase in fluorescence intensity of C334-C-HPA complex.

The fluorescence spectra of C334 in the presence of C-HPA are shown in Figure 5(c). The fluorescence spectral data are given in Table 4. A fluorescence enhancement of C334 is observed at the addition of C-HPA, which is a result of complexation inside the cavity of the host molecule. Although it is less, a 1 nm blue shift is observed for the enhanced spectrum from the spectrum of C334 in water. The increase in the intensity of fluorescence on C334-C-HPA complexation is nonlinear, as shown in Figure 5(c) and the data are fit using a nonlinear curve fitting for the following equilibrium:

where represents C334 (guest), represents C-HPA (host), and refers to the inclusion complex. The binding constant () for the 1 : 1 complex is determined as  mol⁻¹ dm³ from the fitting of data in the following equation [38]:

where is the initial concentration of guest, is the initial concentration of host, is the binding constant of the 1 : 1 complex, and is the intensity difference between the uncomplexed and complexed fluorophore. The binding curve for the C334-C-HPA binding is shown in Figure 5(d). This corresponds to a 1 : 1 stoichiometry of the guest and the host.

Figure 6 shows the time-resolved fluorescence decay of C334 in the presence and absence of C-HPA. The relative amplitude of the two states is altered on the complexation of C334 with C-HPA. The complex may not be influential enough to alter the excited states in a significant way; the time resolved spectral data are compiled in Table 5.

Table 5: Time-resolved fluorescence spectral data of C334 in C-HPA.

Concentration of C-HPA, mol dm⁻³
Energy states
Lifetime (s)
Relative amplitude

Standard deviation (s)

0
T1
1.03 × 10⁻⁹
60.79
1.14
2.10 × 10⁻¹¹

T2
3.05 × 10⁻⁹
39.21
4.12 × 10⁻¹¹

1.8 × 10⁻⁷
T1
1.01 × 10⁻⁹
64.32
0.10
1.93 × 10⁻¹¹

T2
3.11 × 10⁻⁹
35.68
4.53 × 10⁻¹¹

3.4 × 10⁻⁶
T1
9.43 × 10⁻¹⁰
66.64
0.10
1.72 × 10⁻¹¹

T2
2.86 × 10⁻⁹
33.36
3.94 × 10⁻¹¹

Excitation wavelength: 470 nm.

Emission wavelength: 504 nm.

Figure 6: Time-resolved fluorescence spectra of C334 in C-HPA.

In ¹H NMR spectrum of C334-CHPA inclusion complex, the methylene protons (12 and 10) attached to the tertiary nitrogen is centered at 3.33 ppm as multiplet. The methylene protons at the positions 8 and 14 resonate as triplets with the chemical shift of 2.75 and 2.85 ppm, respectively. The upfield shifted multiplet centered at 1.96 ppm is assigned to the methylene protons of 9 and 13. The chromone proton resonates at 8.34 ppm, and the aromatic proton signal is observed at 7.46 ppm.

The cross peaks observed in the 2D ROESY NMR spectrum of C334-C-HPA inclusion complex are shown in Figure 7. The circle shows the correlation of methylene protons 8 and 14 present in the hexahydroquinolizidine ring with the aromatic proton of C-HPA. The aromatic proton at H17 of C334 correlates with the hydroxyl protons of C-HPA and are marked by a rectangle. Similarly, the same proton of C334 interacts with the CH proton in the phenyl rings linked position of C-HPA (which is marked by a triangle). The chromone proton (H4) of C334 correlates with the hydroxyls of C-HPA as shown by the diamond symbol. These correlation peaks suggest that the part of C334 binding with the C-HPA is the hexahydroquinolizidine part.

Figure 7: 2D ROESY NMR spectrum of the C334-C-HPA complex.

3.2. Effect of Acidity

Figure 8(a) shows the effect of pH on the absorption spectrum of C334 in water. Decrease of pH from 4.6 down to leads to a large blue shift of absorbance spectrum. The absorption band at 461 nm decreases in absorbance, and new bands are formed at 298 nm due to the formation of monocation of C334. This occurs at increased proton concentration. There is an isosbestic point at around 375 nm owing to the equilibrium between the neutral and the protonated forms of C334 concentration of neutral and protonated species at a given pH. The protonation of the nitrogen of the quinolizidine moiety is likely involving the lone pair of electrons on nitrogen. The ground state value can be obtained for this equilibrium from [39]

where is the total concentration of the compound in both forms, and , , , and are the molar extinction coefficients of the protonated and neutral forms at wavelengths and , respectively (291 and 461 nm in this case). The for the equilibrium of protonated-neutral forms is calculated using (8). The calculated for the neutral-cation equilibrium of C334 in water is .

(a)

(b)

(c)

Figure 8: (a) Absorbance spectra of C334 at various pH in water. (b) Absorbance spectra of C334 at various pH in β-CD. (c) Absorbance spectra of C334 at various pH in C-HPA.

Consider the following:

The effect of pH on the absorption spectrum of C334 in β-CD is shown in Figure 8(b). Upon the decrease of pH, the absorption at 465 nm indeed decreases with the corresponding increase of absorbance at 261 nm due to the formation of monocation. However, the isosbestic point is not met by all the spectra (at various pH). The ground state for the neutral-monocation equilibrium of C334 in the presence of β-CD is . This is quite similar to the value obtained for the same equilibrium in water.

Figure 8(c) shows the effect of C-HPA on the absorption spectrum of C334 over a range from pH 5.2 to . Decrease of absorbance from pH 5.2 is observed for the absorption band at 458 nm with a corresponding increase at 268 nm. There is an isosbestic point at 400 nm indicating the equilibrium between neutral and protonated forms of C334. The ground state for this equilibrium in the presence of C-HPA is determined as . The slightly smaller value compared to that in water is due to the restricted environment offered by the host molecule for protonation.

The effect of pH on the fluorescence spectra of C334 in water is shown in Figure 9(a). The fluorimetric titration curves are shown in Figure 9(b). The fluorescence of C334 gets red shifted on protonation, that is, by increasing the acid concentration. There is quenching of fluorescence of the neutral form initially, and then there is start of appearance of a new band corresponding to the protonated form of C334. In the fluorimetric titration (FT) curve plotted using intensity at 504 nm there is a dip of relative fluorescence intensity. Then, the cation formation curve starts forming. Hence, an initial fluorescence quenching and then a cation formation are quite likely. The excited state value, () for this equilibrium is obtained from the monocation formation curve as . This value is close to the calculated ground state value and this observation leads to the conclusion that the prototropic equilibrium is attained in the ground state itself and remain unaltered in the excited state.

(a)

(b)

Figure 9: (a) Fluorescence spectra of C334 at various pH in water. (b) versus /pH plot of C334 in water.

The effect of pH on fluorescence of C334 in the presence of β-CD is shown in Figure 10(a). The bands corresponding to cation cannot be observed even at very high acidic conditions (less than ). The decrease in relative intensity of fluorescence is shown in Figure 10(b). The monocation formation may be hindered due to the pronounced hydrogen bonding interaction between the hydroxyls of β-CD and the fluorophore and hence the nonavailability of unshared pair of electrons for protonation.

(a)

(b)

Figure 10: (a) Fluorescence spectra of C334 at various pH in β-CD. (b) versus /pH plot of C334 in β-CD.

The fluorescence spectra of C334 at various /pH in the presence of C-HPA are shown in Figure 11(a). The fluorescence quenching curve is shown in Figure 11(b). The cannot be calculated as the band corresponding to cation formation is not observed. Such an argument leads to the conclusion that the complexation of C-HPA hinders protonation of the guest molecule. Based on all the above arguments, the possible structure of the complexes of C334 with β-CD and with C-HPA can be represented as in Figures 12(a) and 12(b), respectively.

(a)

(b)

Figure 11: (a) Fluorescence spectra of C334 at various pH in C-HPA. (b) versus /pH plot of C334 in C-HPA.

(a)

(b)

Figure 12: Schematic picture of the interaction of C334 with β-CD and with C-HPA.

4. Conclusions

The enhancement in the absorbance spectrum of the C334–β-CD complex was observed. The stoichiometry was determined as 1 : 1 from the linearity in the plot of 1/ versus 1/[β-CD], and the binding constant was calculated as 99.1080 mol⁻¹ dm³. C334 showed a fluorescence quenching when it interacted with β-CD. The quenching constant () was calculated as 4.66 × 10⁹ mol⁻¹ dm³ sec⁻¹. The C334-β-CD interaction occurred probably with the hexahydroquinoline ring of C334 interacting with β-CD. Quite contrarily, a fluorescence enhancement of C334 was observed for the interaction of C-HPA, which is a result of host-guest complexation. The increase in the intensity of fluorescence on C334-C-HPA complexation was nonlinear. The stoichiometry of the host: guest complex was 1 : 1 with a binding constant of 9.5 × 10⁵ mol⁻¹ dm³, calculated from the Benesi-Hildebrand equation for the absorption of C334-C-HPA complex. NMR spectral evidences implied that the hexahydroquinoline ring of C334 bound with C-HPA. The calculated for the neutral-cation equilibrium of C334 in water is 0.42, and the excited state value was 0.4. This value was similar to the ground state value, and hence, the prototropic equilibrium might be attained in the ground state itself and was unaltered in the excited state. The monocation formation might be hindered due to the pronounced hydrogen bonding interaction between the hydroxyls of β-CD and the fluorophore. The could not be calculated for the neutral-cation equilibrium in the presence of C-HPA, as the complexation of C-HPA hindered protonation of the guest molecule.

Conflict of Interests

The authors declare that they have no conflict of interests.

Acknowledgment

The authors are sincerely thankful to the Department of Science and Technology; SERB, Government of India, for the funding of the project SR/FT/CS-062/2009.

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