Priya Ranjan Sahoo and
Satish Kumar*
Department of Chemistry, St. Stephen’s College, University Enclave, Delhi – 110007, India. E-mail: satish@ststephens.edu
First published on 1st February 2016
A light controlled reversible switch for copper ion was synthesized by substituting photochromic naphthopyran with a salicylaldimine moiety. The naphthopyran based photoreversible receptor was characterized using IR, NMR, HRMS and single crystal X-ray crystallographic techniques. The photochromic properties of the receptor under light irradiation were investigated by UV-visible spectroscopy. The affinity towards transition metal ions in both closed and open forms were determined. The open form of the receptor displayed an increased affinity towards copper ions. A 3.25 × 104 fold difference in binding affinity for copper ions between the closed and open forms in aqueous methanol solution suggested that the receptor can act as a selective photoswitch for copper ions. Theoretical investigations at the molecular level supported the experimental observations.
Photochromic molecules have been investigated extensively for potential applications in digital electronics, optical sensors, data recording devices, spintronics, logic gate, optical lenses, quantum computing and environmental monitoring to prevent the toxic effects of metal ion pollution.9–15 Photoreversible frameworks such as chromene,16 spirooxazine,17 spiropyran,18–22 spiroindoline and others23,24 showed an enhanced affinity towards heavy metal coordination on incorporation of heteroatoms.25 Photochromism is an interesting phenomenon,26 where the structural alternation takes place between two different forms having different absorption bands in a reversible manner. Light stimulation alters the structural arrangement of photochromic molecules into two different forms, namely the closed and open forms. The polar open form attracts and coordinates polar species such as metal ions.17 The polar open form having a suitably positioned hetero atom (ortho to the phenolic oxygen atom) is expected to enhance the coordination of the metal ion. Therefore, in this paper, a host naphthopyran receptor was designed by incorporating a salicylaldimine unit at a suitable position for improved metal ion coordination. The receptor is expected to swiftly respond to UV-light irradiation and display good fatigue resistance owing to the presence of the naphthopyran unit. The presence of a suitably positioned functional group Schiff’s base (–CH
N) and –OH in the parent molecule adjacent to the phenolic oxygen atom may force the vulnerable C–O single bond to break in the presence of metal ion and lead to an open form complex with a visible color change. In a first-of-its-kind, we have designed a naphthopyran chelator, with excellent switching ability. To our knowledge, photoreversible naphthopyran-based Cu2+ detection has been rarely reported. For example, a recent report based on detection of trivalent metal ions and Cu2+ ions appeared in the literature;27 however, the sensor was not selective. A couple of reports are also available in the literature for Ca2+ and Pb2+ ions.28,29
Compound 4 was prepared as per the procedure given in the literature (Scheme S1†).
CH–), 8.11 (d, 1H, J = 8 Hz, ArH), 7.93 (s, 1H, ArH), 7.84 (d, 1H, J = 8 Hz, ArH), 7.71 (d, 1H, J = 7.6 Hz), 7.57–7.38 (m, 8H, ArH), 7.34 (t, 4H, J = 7.2, ArH), 7.22 (t, 2H, J = 14.8, ArH & ArC
CH), 7.02 (t, 2H, J = 7.6 Hz) 6.73 (d, 1H, J = 10 Hz, ArC
CH). 13C NMR (100 MHz, CDCl3): δ = 160.7 (N
CH), 157.0, 150.9, 143.0, 141.7, 141.4, 140.6, 140.1, 139.2, 139.1, 136.3, 135.7, 135.2, 134.4, 131.8, 130.7, 130.1, 126.3, 122.9, 117.5, 85.3 (Cspiro–O). Elemental analysis: calculated for (C32H23NO2) C: 84.74, H: 5.11, N: 3.09, found C: 84.48, H: 4.96, N: 3.09. HR-MS (MALDI-MS): C32H23NO2, m/z = calculated 453.1729 M+ found 453.1585.
Similarly, closed and open form (TC) geometries complexed to copper ions were also optimized using MPW1PW91/6-31G(d)/LanL2dz and B3LYP/6-31G(d)/Lanl2dz methods.
:
ethyl acetate (1
:
1) solvent in the presence of a catalytic amount of HCl to produce yellow crystals of naphthopyran receptor 1 in 47% yield. The receptor was characterized by 1H and 13C NMR spectroscopy, MALDI-MS and FT-IR spectroscopy (Fig. S1–S3, ESI†).
Suitable crystals of naphthopyran receptor 1 for single crystal X-ray diffraction were obtained through the slow evaporation method using ethyl acetate as the solvent. The receptor 1 crystallized as monoclinic crystals with P21/n space group (Fig. 1). The asymmetric unit of receptor 1 revealed the presence of short intramolecular hydrogen bond contacts between O4 and N2 [2.562(3) Å]. The aromatic ring of the salicylaldimine moiety and the naphthopyran unit displayed a torsion angle (C26–C3–C8–C17) of 77.6(2)°. The aromatic benzene rings attained a perfect orthogonal shape with respect to the naphthopyran unit. The bond lengths and bond angles observed in the crystal structure are listed in Tables S3 and S4.† The crystal packing diagram of receptor 1 revealed several intermolecular short contacts (Fig. S4 and Table S2, ESI†) particularly between O4–H32, O4–H19, C22–H25 and H34–C25, C3, C20. The high stability or rigidity of the crystal structure can be ascribed to the presence of short intermolecular contacts. The two phenyl groups held each other to the spiro carbon atom in two different planes and are present away from the substituted phenol unit to provide a chance for hetero atoms to achieve effective interaction. Intermolecular π⋯π stacking interactions with centroid (C3–C20–C12–C26–C27–C25) to centroid (C6–C16–C7–C19–C17–C14) distance 3.676(2) Å (Fig. S5, ESI†) and intermolecular edge to face interactions with a distance of 2.551(2) Å (Fig. S6, ESI†) were also observed between the aromatic rings of naphthopyran.
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| Fig. 1 ORTEP34 view of receptor 1 with displacement ellipsoids at the 50% probability level. An intramolecular H-bonding of 2.562(3) Å (shown by the dotted line) between O4–N2 (CCDC). | ||
Normally, the photoswitching behavior of a photochromic molecule is largely dependent on Cspiro–O bond length and probably considered as one of the most important parameters in the conversion of the closed form to the open form. The crystal structure of receptor 1 provided a value of 1.462 Å for the Cspiro–O bond length, which indicated that receptor 1 is a reasonably good photochrome. The absorption spectra of receptor 1 was recorded in different solvents and observed an absorption band in the 280–390 nm region. The UV light irradiation of a solution of receptor 1 in different solvents resulted in an absorption band in the 390–530 nm range (Fig. 2). The thermal decay of the open form to the closed spiro form was monitored with time. The thermal decay of the open form followed first order reaction kinetics (eqn (1)). The experimental data obtained was fitted to the first order reaction kinetic equation to obtain the rate constant values in different solvents (Table 1, Fig. S8 and S9†), where At, Aeq and A0 are absorbance of the open form at time t, infinity and zero after UV light irradiation.29 The thermal bleaching data was also interpolated to mono-exponential (eqn (2)) and bi-exponential functions (eqn (3)). The slow decaying component of the open form was negligible leading to a better fit with the monoexponential function (Fig. S10†).35–39
![]() | (1) |
A = A1 exp(−kdect) + R
| (2) |
A = A1 exp(−k1dect) + A2 exp(−k2dect) + R
| (3) |
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Fig. 2 UV-visible spectra of ring opening of naphthopyran receptor 1 ([1] = 2.5 × 10−5 M) in methanol : water (1 : 1, pH = 7.6, 1.0 mM HEPES) at 25 °C. | ||
| Solvent | EA | THF | DCM | i-PrOH | Acetone | MeCN | MeOH | DMSO |
|---|---|---|---|---|---|---|---|---|
| kT/s−1 at 25 °C | 0.030 | 0.032 | 0.033 | 0.019 | 0.051 | 0.031 | 0.070 | 0.063 |
| ε | 2.38 | 6.02 | 7.85 | 8.93 | 17.9 | 20.7 | 37.5 | 32.7 |
The rate constant data obtained was correlated with the dielectric constant values, which suggested that receptor 1 exhibits solvent independent photochromism (Table 1).
The fatigue resistance properties of receptor 1 were investigated in methanol (Fig. S11†) and a methanol
:
water solvent system (1
:
1, pH 7.6, 1.0 mM HEPES). A solution of receptor 1 in methanol or methanol
:
water (1
:
1, pH 7.6, 1.0 mM HEPES) was treated five times with UV light followed by ring closure under dark conditions. The absorption maxima at 445 nm versus time was plotted with light in, a switch-on and switch-off manner, which suggested remarkable fatigue resistance (Fig. 3).
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Fig. 3 Five cycles of UV irradiation of 1 ([1] = 3.6 × 10−5 M) at 25 °C followed by visible light irradiation (absorbance at 445 nm) in methanol : water (1 : 1, pH 7.6, 1.0 mM HEPES). | ||
The advantage of receptor 1 is the presence of a salicylaldimine moiety at a unique position, which can be exploited for selective binding of metal ions. Therefore, receptor 1 was evaluated for its affinity towards transition metal ions by naked eye detection. A pale yellow color visible to the naked eye was observed in the presence of one equivalent of copper ions in aqueous buffered methanol solution (1
:
1, pH 7.6, 1.0 mM HEPES) (Fig. 4). A more intense color was observed in pure methanol solution (Fig. S12†). No change in color was observed in the presence of other metal ions.
The selective complex formation between copper ions and receptor 1 was further investigated using UV-visible spectroscopy. A spectral shift to 400 nm was observed in the absorption spectra of receptor 1 after addition of one equivalent of copper ions (Fig. 5 and S13†), while no spectral change was observed on addition of other metal ions.
In order to assign the observed spectral shift in the presence of copper ions to the open form complex or to the closed form complex in a methanol
:
water solvent system (1
:
1, pH 7.6, HEPES), a UV-visible spectrum of the receptor 1 in the presence of one equivalent of triethylamine was recorded. The shift in the UV-visible spectra of receptor 1 (Fig. S14†) to 400 nm was observed. This shift in the spectra of receptor 1 suggested that the spectral shift observed in a solution of copper ions and receptor 1 was due to the formation of a complex between the closed form of receptor 1 with copper ions.
In order to obtain the affinity of the closed form of receptor 1 towards copper ions in the dark, titration experiments were performed and the data obtained was used for calculation of the association constant using HypSpec software (Fig. 6).40 Different binding models were considered to fit the experimental data to observe best fit model (Scheme 2). When a 1
:
1 binding model was considered between copper ions and receptor 1, a best fit model was attained between the observed and the calculated data (Fig. 7). The association constant log
β value of 2.036 ± 0.004 (Kassociation = 1.08 × 102 M−1) suggested that the closed form of receptor 1 has an affinity for copper ions. The 1
:
1 complex stoichiometry between copper ions and receptor 1 was further confirmed by a Job’s plot (Fig. 8).
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Fig. 6 UV-visible spectra of 1 upon addition of a solution of copper ions in methanol : water (1 : 1, pH 7.6, 1.0 mM HEPES). | ||
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Fig. 7 Observed and calculated absorbance of receptor 1 at 374 nm upon addition of copper ions in 1.0 mM HEPES : methanol (1 : 1 at pH 7.6), [1] = 2.5 × 10−5 M and [Cu2+] = 0–3.9 mM. | ||
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Fig. 8 Job’s plot for determination of stoichiometry of complex formed between receptor 1 and copper ions in methanol : water (1 : 1, pH 7.6, 1.0 mM HEPES). | ||
In addition, the copper ion induced change in the UV-visible spectra of receptor 1 was not significantly affected by the presence of other divalent or trivalent cations (Fig. 9).
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Fig. 9 The copper ion induced absorbance change (1 + Cu2+) in the UV-visible spectra of receptor 1 in the presence of divalent or trivalent cations in methanol : water (1 : 1, pH 7.6, 1.0 mM HEPES). | ||
To check the practical utility of receptor 1 for the recognition of copper ions, filter paper strips were prepared. The test strips were immersed in solutions of different metal ions. A change in color visible to the naked eye was observed in the presence of copper ions (Fig. 10).
In order to investigate whether the stereoisomers of the open form also interact with metal ions. Solutions of receptor 1 in methanol
:
water (1
:
1, pH 7.6, 1.0 mM HEPES) were photoirradiated in the presence of different concentrations of metal ions. The rate of thermal decay of the open form to the closed form were determined in the presence of different concentrations of metal ions. The thermal decay data were plotted as a function of time and fit to the first order reaction kinetics to obtain the rate constant data (Table 2, Fig. S15 and S16†). The rate constant data suggested a decrease in the rate constant value of receptor 1 in the presence of increasing concentrations of copper ions. Such a decrease in the thermal bleaching rate constant value of receptor 1 was not observed in the presence of other metal ions. The results indicated the formation of a complex between the open form isomer and the copper ions.
:
water (1
:
1, pH 7.6, 1.0 mM HEPES)
| [Mn+]/M | 9.9 × 10−7 | 1.4 × 10−6 | 2.4 × 10−6 | 4.7 × 10−6 | 2.0 × 10−5 | 3.3 × 10−5 |
|---|---|---|---|---|---|---|
| Cu2+ | 0.0728 | 0.0691 | 0.0631 | 0.0611 | 0.0574 | 0.0551 |
| Zn2+ | 0.0678 | 0.0690 | 0.0689 | 0.0695 | 0.0751 | 0.0758 |
| Mn2+ | 0.0695 | 0.0683 | 0.0682 | 0.0705 | 0.0676 | 0.0726 |
| Ni2+ | 0.0695 | 0.0611 | 0.0688 | 0.0699 | 0.0638 | 0.0645 |
| Fe3+ | 0.0615 | 0.0587 | 0.0641 | 0.0695 | 0.0717 | 0.0708 |
| Fe2+ | 0.0534 | 0.0595 | 0.0644 | 0.0693 | 0.0691 | 0.0712 |
| Co2+ | 0.0601 | 0.0767 | — | 0.0695 | 0.0626 | 0.0657 |
| Cd2+ | 0.0678 | 0.0690 | 0.0689 | 0.0694 | 0.0664 | 0.0676 |
| Hg2+ | 0.0666 | 0.0642 | 0.0665 | 0.0682 | 0.0680 | 0.0652 |
| Ag+ | 0.0685 | 0.0615 | 0.0683 | 0.0696 | 0.0621 | 0.0716 |
| Eu3+ | 0.0806 | 0.0700 | 0.0721 | 0.0682 | 0.0701 | 0.0716 |
| Gd3+ | 0.0610 | 0.0625 | 0.0534 | 0.0695 | 0.0625 | 0.0718 |
| Pb2+ | 0.0683 | 0.0707 | 0.0690 | 0.0702 | 0.0683 | 0.0722 |
Absorption spectra of the open form of receptor 1 in the presence of one equivalent of metal ions were analysed. The analysis revealed a small bathochromic shift in the absorption spectra of receptor 1 in the presence of copper ions (Fig. 11), while no bathochromic shift was observed in the presence of other metal ions (Fig. S17†). The small bathochromic shift in the presence of copper ions indicated the interaction between the phenolic oxygen of the naphthopyran unit and the copper ions. Similar interactions between phenolic oxygen and metal ions have also been reported in the literature.29 The interaction between the phenolic oxygen of the naphthopyran unit and the copper ions also indicated a more polar nature of the excited state.29 However, since the bathochromic shift is small, the difference in polarity between the open and closed forms is small. This interaction seems to stabilize the open form of the naphthopyan receptor or may lead to a different open form stereoisomer distribution, which may be responsible for a reduction in the rate constant values.29 The maximum absorbance value obtained for receptor 1 on exposure to UV light in the presence of copper ions was plotted against the concentration of copper ions. A slight increase was observed indicating the stabilization of the open form by copper ions (Fig. S18†).
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Fig. 11 Normalized UV-visible spectra of receptor 1 on irradiation with light of 265 nm in the presence and absence of one equivalent of copper ions in methanol : water (1 : 1, pH 7.6, 1.0 mM HEPES). | ||
In the absence of a stable open form isomer, it is difficult to calculate the association constant directly. Therefore, a binding model based on the rate constant of thermal decay of the open form in the absence and presence of metal ions was used to calculate the association constant, as reported in the literature29 (Fig. S19†). The rate constant was plotted against the reciprocal of the concentration of copper ions to observe a straight line (Fig. 12). A value of 3.51 × 106 M−1 was obtained. A ratio of 3.25 × 104 was obtained between the open and closed forms of receptor 1, which indicated that receptor 1 can act as a photoswitch for copper ions.
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Fig. 12 A plot of observed variation in the fading rate constant as a function of the reciprocal of Cu2+ ions. [1] = 1.70 × 10−5 M in methanol : water (1 : 1, 1.0 mM HEPES, pH 7.6 at 25 °C). | ||
To further check the utility of receptor 1, fluorescence spectra were recorded in the presence of different metal ions. However, no fluorescence change was detected in the fluorescence spectrum in the presence of one equivalent of metal ions (Fig. S20†).
A detailed knowledge of the reactants, products, intermediate and transition state at the molecular level can help to understand the photochemistry and mechanism of the complex formation. Therefore, DFT calculations were also employed to investigate the photochemistry and the process of copper ion binding to receptor 1. The Cspiro–O bond length has a direct influence on the ring opening process in photochromic molecules. A photochromic system with Cspiro–O bond lengths greater than 1.46 Å generally display good photochromic properties.41 Therefore, calculations were performed with different DFT methods to obtain a geometry, which provides a Cspiro–O bond length close to the experimentally observed value. The Cspiro–O bond length obtained from single crystal X-ray data and equilibrium geometry calculated using different DFT methods were correlated to assess a suitable method to predict the photochemistry of the naphthopyran receptor 1. PBEPBE/6-31G(d) and B3LYP/6-31G(d) were observed to be the most accurate method among the three DFT methods [B3LYP/6-31G(d), PBEPBE/6-31G(d) and MPW1PW91/6-31G(d)] utilized in this study (Table S5†). PBEPBE/6-31G(d) was the fastest method among the three methods used in the study. Several ground state geometries of the closed form of receptor 1 were optimized, the geometry obtained through the single crystal X-ray data was predicted as the most stable geometry by all three DFT methods. The crystal structure of receptor 1 indicated the presence of an intramolecular hydrogen bond. The intramolecular H-bond must be broken to achieve complexation with copper ions. Therefore, it is important to estimate the strength of this hydrogen bond. In order to estimate the strength of the H-bond, the structure of receptor 1 was optimized in such a manner that a hydrogen atom attached to the oxygen atom of the salicylaldimine moiety could not make a H-bond with the nitrogen atom, an increase in energy of receptor 1 by 14.41 kcal mol−1 [B3LYP/6-31G(d)] was observed (Fig. S21a†). In another study, the lowest energy optimized structure of the closed form of receptor 1 was selected. The hydrogen atom attached to the oxygen atom of the salicylaldimine moiety was dihedrally rotated by 180° such that it is not in a position to make a hydrogen bond with the nitrogen atom. The resultant geometry was not optimized further (Fig. S21b†) and the single point energy was calculated, an increase in energy of receptor 1 by 17.56 kcal mol−1 was observed. The two theoretical observations provided an estimate of the hydrogen bond strength in receptor 1.
The ring opening process, which involves cleavage of the Cspiro–O bond, was investigated by performing energy calculations as a function of the Cspiro–O distance ranging from 1.6 to 2.8 Å in the gas phase using Gaussian 09 software.30 The intermediate structure at each point was optimized using DFT/B3LYP/6-31G(d) method. A plot shown in Fig. 13 was obtained which indicated an energy maxima at R = 2.1. The structure corresponding to energy maxima at R = 2.1 was used to obtain the transition state of the ring opening process (Fig. 13 and S22†).32 Frequency calculations were performed to confirm the transition state through the presence of single negative frequency. The energy of activation for the ring opening process of naphthopyran derivative 1 was calculated (Fig. 14) by three different DFT methods to provide an average value of 18.31 kcal mol−1. The high value of the activation energy suggested inaccessibility of the ring opening process at room temperature. The Cspiro–O distance was observed to be 3.19 Å at TS1, which indicated that the bond is considerably broken (Fig. 14).
![]() | ||
| Fig. 13 Relative energy (kcal mol−1) values along the Cspiro–O closed form to the open form (CC) path calculated using B3LYP/6-31G(d). | ||
![]() | ||
| Fig. 14 Calculated structure of the transition state of receptor 1 using the DFT/B3LYP/6-31G(d) method. | ||
The stereoisomer (CC) of the open form of receptor 1 can lead to other stereoisomers through cis–trans rearrangement of two of the three bonds that link the two aromatic units. The photochromic properties of receptor 1 can be better understood , if the isomerization process is explored in detail. Therefore, it is important to understand the relative stability and activation energy required for the isomerization process. Fig. 15 shows the entire photoisomerization potential energy pathway calculated using the B3LYP/6-31G(d) method involved in the conversion of the closed form of receptor 1 to the various open form stereoisomers. The process initiates with the breaking of the Cspiro–O bond to yield CC isomer via transition state TS1. The CC stereoisomer in turn gets converted into a more stable TC stereoisomer through cis–trans isomerization passing through the TS2 transition state. The conversion of the CC isomer to TC requires significantly lower activation energy in comparison to the ring opening process (Table 3). The conversion of TC to TT requires 15.81 kcal mol−1 activation energy, while the difference in stability between the TC and TT isomers is of the order 2.79 kcal mol−1. Therefore, it is reasonable to conclude that the conversion of TC to TT is inaccessible at room temperature. The process of conversion of ring closed structure to ring open stereoisomer CT passes through a high activation energy in comparison to the CC isomer. Therefore, it may be concluded that the ring closed structure provides the CC isomer preferentially. The energy of various isomers of the closed and open forms were calculated using different quantum chemical methods and the relative energy is reported in Table 3 (Table S6† lists the total energy). The energy, calculated using B3LYP and PBEPBE methods was observed to be almost similar, while the MPW1PW91 method provided a significantly different energy.
![]() | ||
| Fig. 15 Potential energy diagram of ring opening/closing process in receptor 1 calculated using DFT/B3LYP/6-31G(d). | ||
| Conformer | B3LYP/6-31G(d) | MPW1PW91/6-31G(d) | PBEPBE/6-31G(d) |
|---|---|---|---|
| a The energy of the most stable isomer is listed. | |||
| Closed | 0 | 0 | 0 |
| TC | 3.67258 | 8.38715 | 3.74273 |
| TT | 6.54806 | 11.2287 | 6.72525 |
| CT | 13.2705 | 17.3813 | 12.9602 |
| CC | 13.7826 | 18.4306 | 13.4280 |
Fig. 2 shows the changes in the absorption spectra of receptor 1 on exposure to UV light (365 nm). To explore and understand the changes in the absorption spectra further, time dependent density functional theory calculations were performed using three different methods [B3LYP/6-31G(d), PBEPBE/6-31G(d) and MPW1PW91/6-31G(d)]. The calculations were performed on the most stable stereoisomer (TC) of the open form. It was observed that B3LYP/6-31G(d) provided a value (450 nm) in agreement with the experimentally observed value. The MPW1PW91/6-31G(d) method provided a value of 432 nm for λmax while the PBEPBE/6-31G(d) calculated value (535.95 nm) was observed to be in disagreement with the experimentally observed one.
A close examination of the data obtained using TD-DFT/B3LYP/6-31G(d) (Fig. 16) revealed that the singlet excitation wavelength was mainly contributed by the HOMO to LUMO (S0 to S1), and HOMO-1 to LUMO (S0 to S3) orbitals. The energy of the HOMO-1 to LUMO transition (2.75 ev, 451 nm) is close to the experimentally observed value (445 nm) of the absorption maxima (Table 4).
![]() | ||
| Fig. 16 Energy diagram of the main orbitals of naphthopyran receptor 1 calculated using TD-DFT/B3LYP/6-31G(d) method. | ||
| S0 to S1 | S0 to S2 | S0 to S3 | S0 to S4 | |
|---|---|---|---|---|
| CIC | H To L (0.62) | H-3 to L (0.54) | H-1 to L (0.51) | H-2 to L (0.62) |
| E (eV) [λ (nm)] | 2.37 (523.72) | 2.71 (456.96) | 2.75 (251) | 2.98 (416) |
| μx | 4.51 | −1.06 | −6.26 | 1.26 |
| μy | −0.04 | −1.51 | −3.44 | 1.00 |
| μz | 0.24 | 0.10 | −0.19 | 0.10 |
| μtotal | 8.03 | 1.34 | 20.07 | 1.02 |
| f | 0.1834 | 0.0352 | 0.5318 | 0.0293 |
Similarly, various geometries of closed and open forms (TC) of receptor 1 complexed to copper ions were also optimized using MPW1PW91/6-31G(d)/LanL2DZ and B3LYP/6-31G(d)/Lanl2DZ methods. Since the TC isomer was observed as the most stable and accessible isomer at room temperature (Table 5). Therefore, the open form geometries of the complex with copper ions were optimized using the TC stereoisomer. The process of complex formation may or may not involve the abstraction of a proton from the phenolic OH group. Therefore, both processes were considered. The most stable geometries are shown in Fig. 17. The energy calculation suggested that the open form of receptor 1 has a high affinity for the copper ion in comparison to the closed form, verifying the experimental observations.
| B3LYP/6-31G(d) | MPW1PW91/6-31G(d) | B3LYP/6-31G(d) | MPW1PW91/6-31G(d) | |
|---|---|---|---|---|
| Total energy | Relative energy | |||
| a Relative E = 1-closed-Cu–TC-Cu.b Relative E = 1-closed-H-Cu–TC-H-Cu. | ||||
| 1-Closed-Cu | −1025401 | −1 025 209 |
0 | 0 |
| 1-Closed-H-Cu | −1025224 | −1 025 033 |
0 | 0 |
| TC-Cu | −1025407 | −1 025 207 |
−5.594981a | 2.01191a |
| TC-H-Cu | −1025236 | −1 025 039 |
−11.05559b | −5.398521b |
![]() | ||
| Fig. 17 The most stable geometries obtained using the DFT/B3LYP-LanL2DZ/6-31G(d) method for the copper ion complex of receptor 1. | ||
Footnote |
| † Electronic supplementary information (ESI) available: Synthesis, computational, crystallographic data and additional absorbance spectra. CCDC 1422523. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5ra24857d |
| This journal is © The Royal Society of Chemistry 2016 |