Open Access Article
Emily R.
Neil
,
Mark A.
Fox
,
Robert
Pal
,
Lars-Olof
Pålsson
,
Benjamin A.
O'Sullivan
and
David
Parker
*
Department of Chemistry, Durham University, South Road, Durham, DH1 3LE, UK. E-mail: david.parker@dur.ac.uk
First published on 24th July 2015
A series of bright, europium(III) complexes has been prepared based on an achiral heptadentate triazacyclononane ligand bearing two strongly absorbing, coordinated aralkynyl pyridyl moieties. The binding of chiral carboxylates, including α-hydroxy acids such as lactate and mandelate, has been monitored by emission spectroscopy and is signalled by the switching on of strong circularly polarised emission. In each case, an R-chiral carboxylate gave rise to emission typical of a Δ complex, most clearly shown in the form of the ΔJ = 4 transition manifold around 700 nm. Variations in the sign and magnitude of the CPL allow the enantiomeric purity and absolute configuration of the acid to be assessed in a sample. Analysis of the relative energies of the parent aqua complexes and their stereoisomeric adducts has been aided by lifetime measurements and density functional theory calculations.
The chiroptical behaviour of strongly emissive lanthanide(III) complexes has dominated CPL probe development, and time-gating techniques allow the long-lived signal from the lanthanide(III) centre to be observed selectively.4–6 The emissive lanthanide excited state can be perturbed in a variety of different ways, including changes in local solvent structure, sensitivity to energy transfer and static or dynamic charge transfer quenching processes.7 In particular, changes in the ligand field can occur arising from reversible binding to the metal or the ligand.8–10 The latter modulation is of particular use to signal the presence of chiral species in solution.
The emission spectra of LnIII complexes are sensitive to changes in the coordination environment that determine the ligand field. Such behaviour can be considered to arise from perturbation of the electric susceptibility tensor and its anisotropy that defines the optical behaviour of the lanthanide complex in solution. At the same time, the magnetic susceptibility tensor, characterising the behaviour of a given lanthanide(III) complex in a magnetic field, serves to rationalise the magnetic properties of the complex, i.e. its susceptibility; the anisotropy of this tensor is of paramount importance in rationalising NMR behaviour, primarily determining the paramagnetic shift and EPR characteristics.11–13
In europium emission spectra, the oscillator strength of the magnetic-dipole allowed ΔJ = 1 transition (ca. 590 nm) is generally considered to be independent of the ligand environment. The ΔJ = 2 and ΔJ = 4 transitions (ca. 615 and 700 nm respectively) are electric-dipole (ED)-allowed and are hypersensitive to ligand perturbation. To a first approximation, their intensities are proportional to the square of the ligand dipolar polarisabilities. A ligand polarisation model has been advocated14 to develop our understanding of lanthanide optical emission behaviour, in which electric-quadrupole-allowed transitions (e.g.5D0 to 7F2/4) gain ED strength via a quadrupole (on the Ln3+ ion)-induced dipole (ligand) coupling mechanism. The induced dipoles on the ligands are created by direct coupling to the ED components of the radiation field. Thus, 4f–4f ED strength has been directly linked to ligand dipolar polarisabilities and to the anisotropies of these polarisabilities.15
For Eu(III) complexes, perturbation of the ligand field has a particularly significant impact on the emission profile. Thus, variation of the axial donor in square antiprismatic complexes has a major effect on the relative intensity of the 7F2 ← 5D0 transition,16 and has been exploited in the signalling of reversible anion binding to the metal centre in aqueous media. Several practical examples of anion sensing have emerged, including the assay of citrate, lactate and bicarbonate in bio-fluids.17–20 More recently, reversible binding to certain acute phase proteins in serum, e.g. α1-AGP, has been reported, in which a glutamate side chain carboxylate that is close to the main hydrophobic binding pocket binds to the Eu centre.21,22 In each case, the interaction is signalled by modulation of the total emission spectrum, and can be calibrated to measure changes in the intensity ratio of two or more emission bands. However, such analyses are not normally sensitive to chiral aspects that arise from stereoselective interactions. For this issue to be addressed, chiroptical spectroscopic methods need to be employed.
A racemic mixture of LnIII complexes in an achiral environment does not exhibit CPL. However, following addition of a chiral agent a net CPL signal may be obtained. For the cases where a chiral anion or protein can bind reversibly to the metal centre of a racemic complex, the formation of diastereoisomeric complexes of differing relative stability will lead to an induced CPL signal whose relative intensity will be dependent on the selectivity of binding and the conformational rigidity of the complex on the emission timescale. The intrinsic ‘brightness’ of the observed species is also a key practical aspect, as the acquisition of the total emission (IL + IR) and the CPL (IL − IR) signals should be as rapid as possible. Owing to the relative simplicity of Eu(III) total emission spectra, arising from the absence of degeneracy of the 5D0 emissive state, these changes are best observed with europium complexes.
Recently, a new series of very bright Eu(III) complexes has been introduced, in which 1,4,7-triazacyclononane (9-N3) serves as the core ligand structure with various substituted pyridyl-alkynylaryl groups acting as the sensitising chromophore.23–27 In particular, complexes that are coordinatively unsaturated based on heptadentate ligands have been prepared28 and can bind reversibly to anions in aqueous media. In this work, we compare and contrast the behaviour of the Eu(III) complexes of the ligands L1–L4, and trace the key ligand structural features that distinguish their ability to serve as effective chiral probes for CPL.
Photophysical data, summarising the behaviour of the four Eu(III) complexes in methanol (Table 1), highlights the differences between the complexes. The high absorbance of each complex in the range 332 to 352 nm arises from the strong ICT band.23,28 The amide complex, [Eu·L2]3+, possesses a modest overall emission quantum yield (2%-presumably due to less favourable intramolecular energy transfer) whereas the other complexes have quantum yields in the range 18 to 20%. These are high values, especially for systems with both a coordinated secondary amine group and a bound water molecule. The presence of a coordinated amine NH oscillator has been shown to be particularly effective at quenching the Eu(III) excited state, via efficient vibrational coupling.32,33 Such excited-state quenching explains the faster emission decay rate compared to the N-benzyl complex, [Eu·L4]+, where the observed rate of emission is nearly twice as slow in methanol. Measurements of the rate constants defining the decay rate of Eu(III) emission in water and D2O allowed solvation states to be estimated. Such data shows that the complexes of L1–3 are octadentate, with one bound water molecule. The N-benzyl complex, [Eu·L4]+, does not possess a bound water molecule, presumably because of the increased steric demand imposed by the additional benzylic substituent. It represents an unusual example of a seven-coordinate Eu(III) complex in aqueous solution, although the emission quantum yield is less than [Eu·L3]+, perhaps due to a less efficient energy transfer step.
| [Eu·L1]+ | [Eu·L2]3+ | [Eu·L3]+ | [Eu·L4]+ | |
|---|---|---|---|---|
| a Data for [Eu·L1]+ is taken from ref. 28; errors on k values are ±10% and ±20% on quantum yield values; b q values in water were determined as defined in ref. 32, using the equation q = 1.2{(k(H2O) − k(D2O) − 0.26 − 0.075n} where n is the number of NH oscillators for secondary amide groups coordinated to Eu via the amide carbonyl. | ||||
| λ/nm | 332 | 348 | 352 | 348 |
| ε/mM−1 cm−1 | 38.6 | 40.0 | 35.0 | 36.0 |
| Φ | 0.19 | 0.02 | 0.20 | 0.18 |
| k/ms−1 | 2.94 | 2.17 | 2.56 | 1.20 |
| kH2O/ms−1 | 2.97 | 3.85 | 3.70 | 2.00 |
| kD2O/ms−1 | 2.04 | 2.33 | 2.63 | 1.89 |
| q | 0.8 | 1.3 | 1.0 | 0 |
:
1 binding model by non-linear least-squares fitting, to give an estimate of the association constant. Direct observation of the 1
:
1 adduct was obtained by electrospray mass spectrometry (ESI), for examples with added lactate, mandelate and α-hydroxycyclohexylacetate. The limited water solubility of the Eu complexes of the mono-cationic complexes meant that these systems were examined in 50% aqueous methanol. Overall, the observed emission intensity increased as anion was added; changes in spectral form were most significant with [Eu·L1]+,28 and were least marked with the complexes of L2–4. The overall changes in emission spectral form were the same for enantiopure and racemic samples of the added chiral anion (ESI, Fig. S2b†).
![]() | ||
Fig. 1 Variation of the europium(III) emission profile as a function of added anion; (upper): [Eu·L2]3+ (5 μM; λexc 348 nm, H2O, pH 5.5), (left to right) lactate, mandelate and cyclohexylhydroxyacetate; (lower): [Eu·L3]+ (5 μM) (λexc = 352 nm, 50% MeOH in H2O, pH 5.5) plus added anions. Insets show fits to experimental data, following iterative non-linear least-squares fitting to a 1 : 1 binding model (details in the ESI†). No significant differences in measured binding constants were found with enantiomeric carboxylates. | ||
Binding constants (Table 2) were largest for the anions with the bulkier substituents (cyclohexyl > Ph > Me) that are intuitively more hydrophobic, consistent with a major role for anion desolvation in the overall free energy change. Thus, binding constants with cyclohexylhydroxyacetate were the highest in every case. Comparing the behaviour of [Eu·L3]+ and its N-benzyl analogue, [Eu·L4]+, affinity constants were smaller for the latter, q = 0 complex. The favourable free energy term associated with displacement of the weakly Eu-coordinated water and its return to bulk (where it enjoys full hydrogen bonding to other water molecules) presumably accounts for this difference in behaviour. In the lactate series, strongest binding occurred to the most positively charged complex, [Eu·L2]3+; the phosphinate complex, [Eu·L1]+ bound anions most weakly, notably compared to the carboxylate, [Eu·L3]+.
| R-lactate | R-mandelate | R-cyclohexylhydroxyacetate | |
|---|---|---|---|
a Measurement in water only at pH 5.5 to eliminate the possibility of interference from bicarbonate.
b Binding of R-phenylpropionic acid was weak with log K estimated to be less than 1.5 for the complexes of L2–4.
c Errors associated with the fitting analysis of a given data set are given in parentheses; experimental errors were estimated to be ± 0.1 log unit.
d Bicarbonate forms an adduct with each of these complexes,28 and the relative affinity (and sensitivity) fell in the order: [Eu·L2]3+ > [Eu·L3]+ ≫ [Eu·L1]+ > [Eu·L4]+.
|
|||
| [Eu·L1]+ | 2.76(04) [2.41]a | — | — |
| [Eu·L2]3+ | 4.57(05) [4.58]a | 4.61(06)a | 5.06(05)a |
| [Eu·L3]+ | 4.01(04) | 4.52(06) | 5.38(04) |
| [Eu·L4]+ | 3.15(04) | 3.85(04) | 4.41(05) |
These stability data are based on total emission changes for all stereoisomeric anion adducts, irrespective of their configuration or constitution. By examining the change in gem with added anion concentration, information is gained on the stability of the major chiral species, i.e. the Δ over the Λ isomeric species. Such a comparison was undertaken for [Eu·L3]+ with R-mandelate, by measuring the variation in g with added anion compared to the total emission change. The experiment was carried out in methanol solution to optimise the CPL signal intensity (Fig. 2). In pure methanol solution, binding affinities are higher due to the smaller free energies of anion solvation. A slightly higher stability constant was found (log
K = 5.79 vs. 5.44) in this case, consistent with a slightly higher binding affinity for the favoured isomer (vide infra: this has a Δ configuration for the R-mandelate). Similar behaviour occurred for the other systems described here.
Further information on the constitution of the anion adduct in each case can be gained by examining the emission decay rates of the anion adducts in water and D2O. A coordinated α-hydroxy-carboxylate in a 5-ring chelate, means that there is one OH oscillator in the Eu coordination environment. A quenching effect that is half of that created by a coordinated water occurs, assuming that the Ln–O distances are about the same. Earlier work substantiates this view, and X-ray studies of chelated lactate and citrate adducts show a Ln–O bond distance that is within 0.05 Å of the corresponding hydrated complexes.29,32 The rate data obtained (Table 3), shows that the lactate adduct for [Eu·L1]+ has no coordinated OH group, implying carboxylate binding only, whereas there is a bound hydroxyl group for complexes of L2 and L3.
| [Eu·L1]+ | [Eu·L1 lactate] | [Eu·L2]3+ | [Eu·L2 lactate]2+ | [Eu·L3]+ | [Eu·L3 lactate] | |
|---|---|---|---|---|---|---|
| k (H2O)/(ms−1) | 2.97 | 2.33 | 3.85 | 2.86 | 3.70 | 2.63 |
| k (D2O)/(ms−1) | 2.00 | 2.00 | 2.33 | 1.89 | 2.63 | 2.00 |
| q | 0.8 | 0.08 | 1.3 | 0.6 | 0.9 | 0.4 |
![]() | ||
| Fig. 4 CPL spectra of [Eu·L4]+ following addition of R-phenylpropionic acid (green) and R-cyclohexylhydroxyacetic acid (red). (λexc 348 nm, 2 mM anion, 5 μM complex, MeOH, pH 5.5, 295 K). | ||
![]() | ||
| Fig. 6 Partial CPL spectra for Eu(III) complexes of L1–4, compared to Δ-[Eu·L6]3+ (top), showing the similar ΔJ = 4 manifold in the presence of excess R-cyclohexylhydroxyacetic acid (295 K, H2O, 10 μM complex, 50 μM acid), correlating with selective formation of a Δ-complex in each case. Mirror image profiles were obtained adding S-acid (see ESI† for total emission and full CPL spectra of each system). | ||
| g em | [Eu·L1]+ | [Eu·L2]3+ | [Eu·L3]+ | [Eu·L4]+ | |
|---|---|---|---|---|---|
| R-Lactate | |||||
| ΔJ = 1 | (592 nm) | +0.01 | −0.03 | +0.02 | +0.05 |
| ΔJ = 4 | (683 nm) | +0.005 | +0.01 | +0.01 | +0.01 |
| (692 nm) | +0.02 | +0.02 | +0.01 | +0.02 | |
| (702 nm) | −0.02 | −0.01 | −0.01 | −0.02 | |
| (708 nm) | −0.04 | −0.04 | −0.03 | −0.06 | |
| R-Mandelate | |||||
| ΔJ = 1 | (592 nm) | +0.01 | −0.05 | +0.04 | +0.05 |
| ΔJ = 4 | (683 nm) | +0.01 | +0.01 | +0.01 | +0.01 |
| (692 nm) | +0.02 | +0.02 | +0.03 | +0.03 | |
| (702 nm) | −0.03 | −0.01 | −0.03 | −0.02 | |
| (708 nm) | −0.09 | −0.05 | −0.06 | −0.09 | |
| R-Cyclohexylhydroxyacetate | |||||
| ΔJ = 1 | (592 nm) | +0.02 | −0.05 | +0.07 | +0.06 |
| ΔJ = 4 | (683 nm) | +0.01 | +0.01 | +0.02 | +0.02 |
| (692 nm) | +0.02 | +0.03 | +0.04 | +0.04 | |
| (702 nm) | −0.02 | −0.01 | −0.07 | −0.03 | |
| (708 nm) | −0.09 | −0.08 | −0.09 | −0.11 | |
Investigation of the binding of one water molecule to each of the four complexes reveals binding energies of increasing strength in the order: [Y·L4]+ < [Y·L1]+ < [Y·L3]+ < [Y·L2]3+ (Fig. 7, ESI Table S4†). This sequence is consistent with the trend of observed radiative rate constants of decay of Eu(III) emission (Table 1). The relative energies of free and water bound conformers of [Y·L4]+ suggested an expected value of q = 1 rather than the observed q = 0 value derived from the emission rate constants of decay in water and D2O for [Eu·L4]. The steric demand imposed by the benzyl group does not appear to prevent water binding, on the basis of the calculated geometry using Y instead of Eu (Fig. 6). The discrepancy in the q values may be accounted for by a different argument. The metal-bound water complex may be of higher energy when the rotation of the benzyl group hinders formation of a stabilising hydrogen bond network between the coordinated water and its hydrogen-bonded (i.e. second-sphere) waters.
The binding energies of the anions R-lactate, R-mandelate and R-cyclohexyl-α-hydroxyacetate with a water molecule were calculated in order to assess the relative hydrophobicity of these anions. The order of increased binding energies (ESI, Table S6†) is cyclohexyl-α-hydroxyacetate < mandelate < lactate, corresponding to the sequence of binding affinities to the europium complexes that was observed experimentally (Table 2).
The binding energies of R-lactate with [Y·L1–4] also reveal a trend that is consistent with the association constants calculated by emission spectroscopy (Table 2), where R-lactate binds with increasing strength in the order: [Y·L1]+ < [Y·L4]+ ∼ [Y·L3]+ < [Y·L2]3+ (ESI Table S5†). Investigation of the geometries of R-lactate bound to [Y·L1]+ shows that the hydroxyl group of the coordinated lactate does not bind as strongly as in [Y·L2–4], with a longer Y–O distance of 2.7 Å compared to corresponding distances of 2.4–2.5 Å for complexes [Y·L2–4]. Close inspection of the optimised geometries of the R-lactate [Y·L1–4] adducts, reveals that the phosphinate groups in [Y·L1]+ are more sterically bulky than the corresponding amide or carboxylate donors in [Y·L2–4]. The increased steric demand results in less space being available for lactate binding via chelation (Fig. S7†). This interpretation lends support to the hypothesis that lactate coordinates to [Y·L1]+via the carboxylate group, either in a monodentate manner or via a 4-membered chelate. Such a hypothesis is corroborated by the differences in the observed radiative decay rate constants (Table 3).
The constitution and relative stereochemistry of the isomeric adducts with a given Eu complex are difficult to determine in solution, without a crystallographic analysis. In principle, chelation of an α-hydroxy-acid for example, may give rise to four isomeric species: according to the orientation of the α-hydroxy chelate and the Δ/Λ complex configuration (Scheme 3). 1H NMR analysis (CD3OD) of the solvent and complex adducts were compromised by considerable line-broadening and the relatively small dipolar shifts that characterise these types of complex, associated with their relatively small ligand field splitting.12 Nevertheless, addition of R-lactate to [Eu·L3]+ led to a general sharpening of the observed resonances and the most shifted axial ring proton resonance (by analogy with the analysis of [Eu·L7]), was observed to shift to lower frequency (ΔδH = −1.5 ppm) compared to the solvate species; four species were observed in relative ratio 3
:
1
:
0.8
:
0.7 (295 K, 11.7 T).
Calculations were performed to assess the relative energies of the four isomeric adducts depicted as Y(III) complexes, in an attempt to reveal whether the presence of non-bonding steric interactions could rationalise the preferred formation of a particular isomer. For each yttrium complex, the preferred constitution of the lactate chelate placed the 2-pyridyl nitrogen atoms in the same plane as the lactate carboxylate oxygen (ESI Table S7†). Thus, the lowest energy isomer (Scheme 3, bottom right) possesses a Δ configuration for the R-lactate adduct, consistent with the assignment of configuration using the CPL data. The energy difference between the two low energy isomers increases in the order [Y·L2]3+ < [Y·L3]+ < [Y·L1]+ < [Y·L4]+. Such a sequence accords with the observation that the N-benzyl complex [Eu·L4]+ has the highest gem values for 70% of the induced CPL transitions in the complexes studied here. Inspection of the calculated geometries shows that in the R-lactate adduct, the Me group points away from a coordinated carboxylate oxygen lone pair (Fig. 8); i.e. such an interaction destabilises the S-lactate-Δ adduct formation.
:
1 ratio in this case).34 These two recent examples, describing covalent modification of the ligand structure suggest a degree of cooperativity or chiral amplification in formation of the preferred complex helicity, as defined by the sign of the three NCCNpy torsion angles.
In the new work discussed here, there are only two such NCCNpy torsion angles; non-covalent formation of a ternary complex with enantiopure anions has been examined. A common pattern emerged: an R acid configuration favours formation of a Δ complex and leads to a strong induced CPL signal. The NMR and DFT studies provide some supporting evidence for this analysis: a preferred major isomer was observed in which the anion carboxylate lies in the same plane as the pyridyl nitrogens. The induced CPL gem values are significant albeit lacking the very high stereoselectivity and larger gem values that characterise the behaviour of the more conformationally rigid, trisubstituted 9-coordinate systems.
The substitution of the third N position plays a key role. The N-benzyl complex gave the highest gem values for 70% of the induced CPL transitions, consistent with the tentative hypothesis that the N-benzyl may align helically in the same sense as the two coordinated pyridylmethyl groups to create a slightly more rigidified local chiral structure.
Finally, this work provides a starting point for developing enhanced selectivity in the association of the chiral analyte. For example, based on the N-benzyl system, introduction of charged groups or directed hydrogen bonding or chelating moieties, e.g. NH2Me+ or a boronic acid group, into the benzyl ring may allow additional stabilising interactions to occur that will enhance affinity and stereoselectivity. The outcome of such work will be reported subsequently.
2Ph); 13C NMR (295 K, 100 MHz, CDCl3) δC 162.9 (
ONH), 159.7 (py–C6), 149.2 (py–C2), 138.0 (Ph–Ci), 132.6 (py–C5), 130.8 (py–C3), 128.9 (Ph–Cm), 128.0 (Ph–Cp), 127.8 (Ph–Co), 107.9 (py–C4), 64.3 (py–
H2), 43.7 (
H2Ph); m/z (HRMS+) 390.9893 [M + Na]+ (C14H13N2O2NaI127 requires 390.9919).
), 8.21 (1H, s, py–H3), 7.53 (1H, s, py–H5), 7.50 (2H, dt, 4J 2, 3J 8, Ar–H3/3′), 7.37–7.34 (4H, m, Ph–Ho, Ph–Hm), 7.29 (1H, m, Ph–Hp), 6.91 (2H, dt, 4J 2, 3J 8, Ar–H2/2′), 4.77 (2H, s, py–CH2), 4.68 (2H, d, 3J 6, CH2Ph), 3.85 (3H, s, OCH3); 13C NMR (295 K, 100 MHz, CDCl3) δC 163.7 (
ONH), 160.7 (Ar–C1), 158.7 (py–C6), 149.2 (py–C2), 138.2 (Ci), 134.6 (Ar–C4), 133.8 (Ar–C3,3′), 128.9 (Ph–C), 128.0 (Ph–C), 127.8 (Ph–C), 124.7 (py–C5), 123.5 (py–C3), 114.4 (Ar–C2,2′), 114.0 (py–C4), 96.1 (C5), 85.6 (C6), 64.6 (py–
H2), 55.5 (O
H3), 43.7 (
H2Ph); m/z (HRMS+) 373.1561 [M + H]+ (C23H21N2O3 requires 373.1552).
), 7.63 (1H, d, 3J 1.5, py–H3), 7.51 (2H, dt, 4J 2.5, 3J 9, Ar–H3/3′), 7.37–7.29 (5H, m, Ph–H), 6.92 (2H, dt, 4J 2.5, 3J 9, Ar–H2/2′), 5.30 (2H, s, py–C
2), 4.68 (2H, d, 3J 6, C
2Ph), 3.85 (3H, s, OC
3), 3.07 (3H, s, SO2C
3); m/z (HRMS+) 451.1320 [M + H]+ (C24H23N2O5S requires 451.1328).
), 8.39 (1H, t, 3J 6.5, CON
′), 8.17 (1H, s, py–H5), 8.16 (1H, s, py–H5′), 7.64 (1H, s, py–H3), 7.57 (1H, s, py–H3′), 7.48 (4H, d, 3J 9, Ar–H3/3′), 7.35–7.24 (10H, m, Ph–H), 6.89 (4H, d, 3J 9, Ar–H2/2′), 4.65 (4H, d, 3J 6.5, C
2Ph), 3.83 (6H, s, OC
3), 3.82 (4H, s, py–C
2), 3.31–3.26 (4H, m, ring Hs), 3.05–2.96 (4H, m, ring Hs), 2.68–2.62 (4H, m, ring Hs), 1.45 (9H, s, O(C
3)3); 13C NMR (295 K, 175 MHz, CDCl3) δC 164.1 (CONH), 164.0 (CONH), 160.6 (Ar–C1), 160.5 (py–C2), 159.3 (py–C2′), 149.5 (py–C6), 149.3 (py–C6′), 138.4 (Ci), 138.3 (Ci), 138.4 (Ar–C4), 138.3 (Ar–C3/3′), 133.8 (Ph–C), 133.7 (Ph–C), 128.8 (Ph–C), 128.7 (Ph–C), 128.0 (py–C3), 127.9 (py–C3′), 122.8 (py–C5), 122.7 (py–C5′), 114.3 (Ar–C2/2′), 114.1 (py–C4), 114.0 (py–C4′), 95.4 (C5), 95.1 (C5′), 85.9 (C6), 85.8 (C6′), 62.9 (py–
H2), 56.3 (ring C), 55.4 (O
H3), 54.9 (ring C), 54.5 (ring C), 53.9 (ring C), 50.1 (ring C), 49.6 (ring C), 43.6 (
H2Ph), 43.5 (
H2Ph), 28.7 (O(
H3)3); m/z (HRMS+) 938.4594 [M + H]+ (C57H60N7O6 requires 938.4605).
2Ph), 3.95 (4H, s, py–C
2), 3.78 (6H, s, OC
3), 3.06 (4H, m, ring Hs), 2.93 (4H, m, ring Hs), 2.74 (4H, m, ring Hs); 13C NMR (295 K, 175 MHz, CDCl3) δC 116.0 (
ONH), 162.3 (Ar–C1), 159.9 (py–C6), 151.1 (py–C2), 139.7 (Ci), 135.4 (Ar–C4), 134.6 (Ar–C3/3′), 129.7 (Ph–C), 128.7 (Ph–C), 128.5 (Ph–C), 128.0 (py–C5), 123.8 (py–C3), 115.4 (Ar–C2/2′), 114.7 (py–C4), 96.8 (C5), 86.0 (C6), 61.5 (py–
H2), 55.9 (O
H3), 51.6 (ring C), 45.1 (ring C), 44.3 (
H2Ph); m/z (HRMS+) 838.4083 [M + H]+ (C52H52N7O4 requires 838.4081).
:
H2O (0.1% formic acid)). The solvent was removed under reduced pressure to give a white solid that was used directly without any further purification. LRMS (ESI MeCN) m/z 1285 [M + 2(CF3SO3)]+, 569 [M + (CF3SO3)]2+. λexc (MeOH) = 348 nm; ϕ (MeOH) 0.02, ε (MeOH) 40
000 M−1 cm−1; τ (H2O) = 0.26 ms, τ (D2O) = 0.43 ms, q = 1.3.
3), 2.41 (6H, s, C
3), 0.25 (9H, s, Si(C
3)3); 13C NMR (295 K, 100 MHz, CDCl3) δC 159.2 (Ar–C1), 142.6 (Ar–C), 113.1 (Ar–C), 112.5 (Ar–C), 103.1 (alkyne C), 101.0 (alkyne C), 55.3 (O
H3), 21.4 (
H3), 0.40 (Si(
H3)3); GC-EI, tR = 4.47, m/z 232 (M+), 217 (M+ − CH3).
23
3), 3.43 (1H, s, ArCC
), 2.44 (6H, s, 2C
3); 13C NMR (295 K, 100 MHz, CDCl3) δC 159.3 (Ar–C1), 142.8 (Ar–C), 144.4 (Ar–C), 112.5 (Ar–C), 83.9 (alkyne C), 81.4 (alkyne C), 55.3 (O
H3), 21.4 (2
H3); GC-EI t = 3.75, m/z 160 (M+), 145 (M+ − CH3).
23
2), 4.01 (3H, s, CO2C
3), 3.80 (3H, s, OC
3), 2.49 (6H, s, C
3); 13C NMR (295 K, 175 MHz, CDCl3) δC 165.5 (
O2CH3), 160.6 (Ar–C1), 160.2 (py–C6), 147.3 (Ar–C4), 143.1 (py–C2), 134.4 (Ar–C3,3′), 125.5 (py–C3), 125.2 (py–C5), 114.0 (py–C4), 112.8 (Ar–C2,2′), 94.0 (alkyne C5), 93.3 (alkyne C6), 64.7 (py–
H2), 55.3 (O
H3), 53.1 (CO2
H3), 21.5 (
H3); m/z (HRMS+) 326.1378 [M + H]+ (C19H20NO4 requires 326.1392).
23
2OSO2), 3.97 (3H, s, CO2C
3), 3.75 (3H, s, OC
3), 3.14 (3H, s, SO2C
3), 2.44 (6H, s, C
3); m/z (HRMS+) 404.1170 [M + H]+ (C20H22NO6S requires 404.1168).
3), 4.02 (4H, s, py–C
2), 3.74 (6H, s, OC
3), 3.48 (4H, br s, ring Hs), 3.06 (4H, br s, ring Hs), 2.81 (4H, s, ring Hs), 2.42 (12H, s, C
3); 13C NMR (295 K, 175 MHz, CDCl3) δC 165.2 (
O2CH3), 160.2 (Ar–C1), 159.4 (py–C6), 147.6 (Ar–C4), 134.5 (Ar–C3,3′), 126.9 (py–C5), 125.7 (py–C3), 113.8 (py–C4), 112.8 (Ar–C2,2′), 94.2 (alkyne C5), 92.8 (alkyne C6), 60.3 (py–
H2), 55.3 (O
H3), 53.9 (ring Cs), 53.6 (CO2
H3), 50.5 (ring Cs), 46.2 (ring Cs), 21.4 (
H3); m/z (HRMS+) 744.3765 [M + H]+ (C44H50N5O6 requires 744.3761).
:
1, 1 mL). The mixture was stirred at 65 °C for 4 h. The reaction was monitored by LCMS. Upon completion, aqueous hydrochloric acid (0.1 M) was added until pH 6.5 was achieved. Europium chloride hexahydrate (5.4 mg, 14.7 μmol) was added and the pH was readjusted to 6.5 by addition of aqueous sodium hydroxide (0.1 M). The reaction was stirred at 65 °C for 24 h. The solvent was removed under reduced pressure to give a white solid (5 mg, 43%); m/z (HRMS+) 864.2371 M+ (C42H43N5O6151Eu requires 864.2412); λexc (MeOH) = 352 nm; ϕ (MeOH) 0.2, ε (MeOH) 35
000 M−1 cm−1; τ (H2O) = 0.27 ms, τ (D2O) = 0.38 ms, q = 0.9.
2), 3.92 (6H, s, CO2C
3), 3.78 (6H, s, OC
3), 3.66 (4H, br s, ring Hs), 3.05 (8H, br s, ring Hs), 2.91 (2H, s, C
2Ph), 2.42 (12H, s, C
3); 13C NMR (295 K, 175 MHz, CDCl3) δC 165.7 (
O2CH3), 160.2 (Ar–C1), 147.6 (py–C6), 143.0 (Ar–C4), 133.9 (Ar–C3/3′), 129.1 (Ph–C), 128.4 (Ph–C), 127.8 (Ph–C), 126.9 (py–C5), 125.1 (py–C3), 114.1 (py–C4), 112.8 (Ar–C2/2′), 93.6 (alkyne C), 64.7 (py–
H2), 56.3 (Ph–
H2), 55.4 (O
H3), 53.1 (CO2
H3), 51.8 (ring Cs), 29.8 (ring Cs), 21.5 (
H3); m/z (HRMS+) 834.4246 [M + H]+ (C51H56N5O6 requires 834.4231).
:
1, 1 mL). The mixture was stirred at 65 °C for 4 h. The reaction was monitored by LCMS. Upon completion, aqueous hydrochloric acid (0.1 M) was added until pH 6.5 was achieved. Europium chloride hexahydrate (5.3 mg, 14.5 μmol) was added and the pH was readjusted to 6.5 by addition of aqueous sodium hydroxide (0.1 M). The reaction was stirred at 65 °C for 24 h. The solvent was removed under reduced pressure and the solid was purified by flash column chromatography (silica, gradient elution starting from 5% CH3OH to 15% CH3OH in CH2Cl2 in 0.5% increments) to give a white solid (10 mg, 80%). m/z (HRMS+) 954.2896 M+ (C49H49N5O6151Eu requires 954.2881); λexc (MeOH) = 352 nm; ϕ (MeOH) 0.18, ε (MeOH) 36
000 M−1 cm−1; τ (MeOH) = 0.83 ms; τ (H2O) = 0.53 ms, τ (D2O) = 0.50 ms, q = 0.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c5dt02358k |
| This journal is © The Royal Society of Chemistry 2015 |