Open Access Article
Laura H.
Davies
,
Ross W.
Harrington
,
William
Clegg
and
Lee J.
Higham
*
School of Chemistry, Bedson Building, Newcastle University, Newcastle upon Tyne, NE1 7RU, UK. E-mail: lee.higham@ncl.ac.uk; Tel: +44 (0)191 208 5542
First published on 23rd June 2014
The syntheses of highly fluorescent analogues of PPh3 and PhPCy2 based on the Bodipy chromophore are described. The ligands have been incorporated into two- to four-coordinate group 11 metal complexes. The synthesis, characterisation and photophysical properties of the novel ligands and their metal complexes are reported; many of these compounds have also been characterised by single-crystal X-ray diffraction. Incorporation of the phosphino group and complexation to the group 11 metal centre has little effect on the absorption and emission profiles; high molar extinction coefficients and fluorescence quantum yields were still obtained. In particular, incorporation of the dicyclohexylphosphino substituent significantly increases the quantum yields relative to the parent dyes.
F-Bodipy has desirable photophysical properties which include a high fluorescence quantum yield, strong UV-absorption, chemical robustness and good solubility (Fig. 1).6 A common site of modification is at the meso position due to its easy synthetic incorporation.6 Over the last few years new synthetic procedures have been developed for the substitution of the fluorides with aryl/alkyl (C-Bodipy) or ethynyl (E-Bodipy) groups; this development has allowed more sophisticated functions to be introduced on the Bodipy backbone.6 Given the desirable properties of Bodipy and the extensive synthetic routes to derivatives,6 we aimed to create fluorescent tertiary phosphines based on this versatile fluorophore, coordinate the new ligands to transition metals and study their behaviour.
Group 11 metal phosphine complexes are sought after, in part, due to their known medicinal applications.7 Gold(I),8 silver(I)9 and copper(I)10 phosphine complexes have all shown cytotoxic activity, with significant anti-tumour properties – current complexes are based on monodentate and bidentate phosphines. One breakthrough was the discovery of auranofin (Fig. 1) in the early 1980s by Sutton,11 a gold(I) phosphine complex, that was approved for clinical use in 1985 to treat rheumatoid arthritis, but which has also been shown to exhibit anticancer properties,12 and led to the development of several two-coordinate gold(I) phosphine analogues.8
To further develop the possibility of using gold-based drugs, a greater knowledge of their subcellular distribution and mechanism of action is desirable – a fluorescent gold phosphine complex could help to understand the biodistribution of such compounds at high resolution and precision.1,3 Both gold and silver also have potential in therapeutic nuclear medicine due to the beta-emitting radioisotopes 199Au and 111Ag, which have long half-lives of 3.15 and 7.5 days respectively.13 Copper has a range of radionuclides, but the most commonly investigated is 64Cu – a positron emitter – and thus can be used for diagnostic nuclear medicine purposes in Positron Emission Tomography (PET) imaging; its relatively long half-life of 762 minutes is considered attractive.14 For the aforementioned reasons it would therefore be interesting to investigate the coordination chemistry of novel fluorescent monodentate phosphines with the group 11 metals and measure the photophysical properties of any complexes so synthesised, to ascertain if they are suitable for study in the applications already discussed above.
The 31P{1H} NMR spectra of the triarylphosphines in d-chloroform showed 2a/2b at δ −5.5 ppm; aryldialkylphosphines 3a and 3b are shifted downfield to δ 2.7 and 2.8 ppm respectively, due to the electron-donating cyclohexyl rings.
Crystals of 2a were analysed by X-ray crystallography and its molecular structure is depicted in Fig. 2; similar atom numbering schemes are used for all the crystal structures. The P–C bond lengths of 1.8302(19), 1.834(2) and 1.827(2) Å and C–P–C bond angles of 104.03(9), 101.66(9) and 102.40(9)° are typical for tertiary phosphines and compare well to triphenylphosphine.16
The Cu–P bond lengths of 2.2384(11) and 2.2273(11) Å are typical for copper(I) complexes.18,19 The complex has a distorted trigonal planar geometry for copper, shown by the P1–Cu–P2, P1–Cu–O5 and P2–Cu–O5 bond angles of 130.49(4)°, 113.61(9)° and 115.43(9)° respectively; both the phosphorus atoms are slightly tilted towards the ethanol molecule. The anion⋯Cu(I) interaction is weak as signified by the closest Cu⋯F distance of 3.156 Å. The analogous reaction of a 2
:
1 ratio of triphenylphosphine and [Cu(CH3CN)4][PF6] resulted in the distorted four-coordinate tetrahedral complex [Cu(PPh3)2(CH3CN)2].17,20 Ligand 2b is sterically more bulky than triphenylphosphine, and therefore the four-coordinate structure may be too crowded for the first-row d10 transition metal in this case.
Complex 5a was crystallised by slow solvent diffusion (chloroform–diethyl ether); two types of crystals were produced and their molecular structures are shown in Fig. 4. Structure A is a three-coordinate copper(I) complex with two phosphines and one acetonitrile ligand coordinated to the copper centre, and a non-coordinating anion, PF6−. The Cu–P bond lengths of 2.2273(11) and 2.2564(10) Å are typical of copper(I) phosphine complexes.18,19 The complex has a distorted trigonal planar geometry as shown by the P1–Cu–P2, P1–Cu–N5 and P2–Cu–N5 bond angles of 136.11(4)°, 120.68(10)° and 102.36(10)° respectively; the P1–Cu–P2 angle is larger than in complex 4b due to the steric bulk of the cyclohexyl groups. The anion⋯Cu(I) interaction is again weak, as signified by the closest Cu⋯F distance of 3.228 Å. Structure B is a distorted trigonal-planar copper(I) complex with two phosphines coordinated and no bound acetonitrile ligands, but the PF6− anion (modelled with disorder) is weakly coordinated to the copper centre as shown by a stronger anion⋯Cu(I) interaction than in structure A; the alternative closest Cu⋯F distances are 2.741(7) Å to F6A as shown in Fig. 4, and 2.964(11) Å to F6B (not shown); F6A is disordered over two symmetry-related positions in the trigonal plane with the copper centre (on a twofold rotation axis) and two P atoms. All other Cu⋯F distances are >4 Å and are thus non-bonded. A search of the Cambridge Structural Database21 reveals 11 structures recorded with weakly coordinated PF6− and BF4− anions having Cu⋯F > 2.7 Å.22 The P–Cu–P bond angle of 149.98(9)° is large for a three-coordinate structure but is consistent with the steric bulk of the cyclohexyl groups and is similar to that in the three-coordinate complex [Cu(PCy3)2(ClO4)], which has a P–Cu–P angle of 144.46(6)°.23 The symmetry-equivalent Cu–P bonds lengths of 2.2280(15) Å are typical and compare well with [Cu(PCy3)2][PF6], which was prepared by Che et al.18 In that complex the crystal structure reveals a two-coordinate linear copper(I) structure, with Cu–P bond lengths of 2.213(1) and 2.313(1) Å, and a much larger P–Cu–P angle of 179.47(3)°, consistent with a linear geometry and ionic PF6−.18 However, when the counter-ions tetrafluoroborate and perchlorate were employed, three-coordinate structures were obtained (similar to 5a, structure B) with copper–fluorine and copper–oxygen distances of 2.420(6) and 2.220(7) Å and P–Cu–P angles of 159.98(8)° and 144.46(6)° respectively.23,24 Willet et al. showed that dicyclohexylphenylphosphine (which is the closest analogue to 3a and 3b) produced [Cu(PCy2Ph)2][ClO4] with the perchlorate anion, but with tetrafluoroborate a different copper(I) complex formed, [Cu(PCy2Ph)2(F–BF3)]. Currently the crystal structures are not known to confirm whether the counter-ions have any significant coordinating interaction.25
Phosphine coordination resulted in a downfield shift of the 31P{1H} NMR signal at room temperature from δ −5.5 ppm for the free phosphines 2a/2b to broad peaks at δ 10.2 and 6.6 ppm for the complexes 6a and 6b respectively (Fig. 5 and ESI†); the signal was a broad singlet at elevated temperatures in both cases, which likely results from rapid phosphine exchange.26 This lability is reduced at low temperatures and the Ag–P coupling can be observed.26
At low temperature (−40 °C) two doublets appeared; 1J107AgP = 444 Hz and 1J109AgP = 511 Hz, and 1J107AgP = 446 Hz and 1J109AgP = 507 Hz coupling constants were observed for 6a and 6b respectively; these values are typical for silver(I) complexes with two phosphines bound26,27 and compare well to [Ag(PEt3)2(hfa)] (1J107AgP = 468 Hz).28 For both 6a and 6b a second set of two low-intensity doublets was observed at −40 °C and indicates that a second silver species was present in solution. For these signals the following Ag–P couplings were measured: 1J107AgP = 696 Hz and 1J109AgP = 803 Hz, and 1J107AgP = 590 Hz and 1J109AgP = 677 Hz for 6a and 6b respectively. The increase in Ag–P coupling constants indicates a change in the hybridisation state of the silver(I) complex26,27 and is attributed to [Ag(2a/2b)(hfa)] with only one phosphine ligand bound. The coupling constants are similar to the reported values for [Ag(PR3)(hfa)] (R = Ph, Me, Et): 1J107AgP = 700–760 Hz.28,29
Puddephatt et al. reported that an equilibrium is established on the addition of excess phosphine to [Ag(PR3)(hfa)] complexes and showed that the Ag–hfa bonding is more ionic when extra phosphines are present.28,30 Mass spectrometry confirmed the [Ag(2a/2b)2]+ product, giving peaks at m/z of 1469.6056 (6a) and 1217.5443 (6b), with loss of the hfa ligand. Low-intensity peaks at 786.2561 and 663.2251 were also observed, which correspond to [Ag(2a/2b)]+, in addition to peaks at 2148.9477 and 1777.8560 for the tris-cations [Ag(113a/113b)3]+, but these latter species were not detected by NMR spectroscopy.
On coordination of the dicyclohexyl phosphines 3a and 3b the 31P{1H} NMR signals at room temperature were also shifted downfield for the complexes 7a and 7b; however, instead of a broad singlet, two broadened doublets were observed at δ 23.7 ppm and δ 23.9 ppm for 7a and 7b respectively (Fig. 6 and ESI†). The following Ag–P coupling constants were observed for 7a and 7b respectively: 1J107AgP = 453 Hz and 1J109AgP = 517 Hz, and 1J107AgP = 453 Hz and 1J109AgP = 519 Hz. At higher temperatures (120 °C) 7a and 7b gave a broad singlet.
The observation of Ag–P coupling at room temperature was unusual since the rapid exchange of the phosphine ligands usually causes this coupling to be averaged to zero; this ligand exchange is normally slowed down by cooling the solution to low temperatures (as is the case for 6a and 6b).27 However, the observation of Ag–P coupling at room temperature has been reported previously, where the phosphine is sterically hindered or chelating.27,31 Phosphines 3a and 3b are also bulky which may explain the lower rate of phosphine exchange and the observation of Ag–P coupling. The electrospray mass spectra gave peaks for [M − (hfa)]+ at m/z of 1489.7998 for 7a, and 1242.7354 for 7b. Complexes 6a and 7b were also characterised by X-ray crystallography (Fig. 7). The complexes have neutral silver(I) tetrahedral four-coordinate geometries with two phosphines and one hfa ligand bound to the metal. The Ag–P bond lengths of 2.4255(10) Å and 2.4028(13) Å are typical for silver(I) phosphine complexes.25,30,32 The complexes are somewhat distorted, shown by the P–Ag–P, P–Ag–O and O–Ag–O bond angles (Fig. 7 caption). The synthesis of a related four-coordinate silver(I) complex [Ag(PPh3)2(hfa)] has been reported in a similar fashion, but currently no crystal structure is known.33
However, the three-coordinate complex [Ag(PPh3)(hfa)] has had its solid state structure determined – shorter bond lengths are observed: 2.346(3) for Ag–P, and 2.341(5) and 2.218(5) Å for Ag–O.29 For 7b the Ag–O bond distances of 2.337(6) Å (Ag–O1) and 2.718(8) Å (Ag–O2) are significantly different, and the latter is longer than the normal covalent silver(I)–oxygen bond length of ca. 2.3 Å, which indicates that the second oxygen is only weakly bonded to the silver;28 the hfa ligand is disordered over two positions related by the twofold rotation axis passing through Ag. The bite angle of the phosphines is larger than in 6a, due to the increased steric bulk of the phosphine 3b. No β-diketonate silver complexes with dicyclohexylphenylphosphine or tricyclohexylphosphine have been reported, however cationic two- and three-coordinate silver(I) complexes do form with dicyclohexylphenylphosphine and the non-coordinating perchlorate, tetrafluoroborate, hexafluorophosphate and hexafluoroantimonate anions.25,32,33
Coordination of the phosphines resulted in a downfield shift of the 31P{1H} NMR signal of the free phosphines 2a/2b and 3a/3b to δ 33.2/33.3 and 51.4/51.6 ppm for the complexes 8a/8b and 9a/9b respectively. Complexes 8a, 9a and 9b were also characterised by X-ray crystallography (Fig. 8 and ESI†). The solid-state structures show them to be gold(I) two-coordinate linear complexes, as expected.
The Au–P and Au–Cl bond lengths are typical for gold(I) compounds (Fig. 8 caption).34 The P–Au–Cl bond angles of 177.24(14)°, 178.27(5)° and 177.55(3)° for 8a, 9a and 9b respectively are close to the ideal 180° for a linear complex. The analogous complex to 8a/8b, [AuCl(PPh3)], prepared from triphenylphosphine and chloroauric acid, has a slightly longer P–Au bond length (2.235(3) Å), and a slightly larger Au–P–Cl bond angle than 8a (179.68(8)°).34a The analogous dicyclohexylphenylphosphine complex, [AuCl(PCy2Ph)], made from the ligand and a reaction mixture of tetrachloroauric acid and 2,2′-thiodiethanol, has P–Au and P–Cl bond lengths of 2.234(2) and 2.281(3) Å respectively and an Au–P–Cl bond angle of 178.3(1)°, very similar to 9a/9b.34b
| Compound | λ abs (nm) | λ em (nm) | ε (M−1 cm−1) | Φ F |
|---|---|---|---|---|
| a Measured in dry degassed tetrahydrofuran at room temperature. Fluorescence quantum yields were measured with respect to 4,4-difluoro-8-phenyl-1,3,5,7-tetramethyl-2,6-diethyl-4-bora-3a,4a-diaza-s-indacene.36 | ||||
| 2a | 517 | 534 | 77 000 |
0.042 |
| 4a (Cu) | 518 | 535 | 133 000 |
0.038 |
| 6a (Ag) | 518 | 535 | 151 000 |
0.036 |
| 8a (Au) | 519 | 538 | 76 000 |
0.034 |
| 2b | 513 | 527 | 92 000 |
0.29 |
| 4b (Cu) | 513 | 528 | 167 000 |
0.29 |
| 6b (Ag) | 513 | 528 | 155 000 |
0.26 |
| 8b (Au) | 514 | 529 | 74 000 |
0.20 |
| 3a | 518 | 533 | 77 000 |
0.073 |
| 5a (Cu) | 518 | 534 | 143 000 |
0.069 |
| 7a (Ag) | 518 | 534 | 141 000 |
0.070 |
| 9a (Au) | 519 | 536 | 78 000 |
0.058 |
| 3b | 512 | 526 | 82 000 |
0.44 |
| 5b (Cu) | 512 | 527 | 171 000 |
0.42 |
| 7b (Ag) | 513 | 527 | 157 000 |
0.43 |
| 9b (Au) | 514 | 529 | 85 000 |
0.39 |
The four phosphine ligands 2a/2b and 3a/3b all show a typical Bodipy profile6 with absorption maxima at either 517/513 nm or 518/512 nm depending on the groups at the boron centre; changing from diphenyl to dimethyl causes a hypsochromic shift of the absorption maxima (4–6 nm). The lowest energy maximum is assigned to the S0–S1 (π–π*) transition for the Bodipy core. All the ligands have typically high molar absorption coefficients, ranging from 77
000 to 92
000 M−1 cm−1.6 Secondly, a lower intensity, broader absorption band can be seen between 370 and 385 nm (ε = 3000–10
000 M−1 cm−1), which is attributed to the S0–S2 (π–π*) transition of the Bodipy core. There are also low-intensity, high-energy peaks centred between 250–300 nm for the dicyclohexyl derivatives 3a/3b. The absorption spectra for phosphines 2b/3b and their complexes are given in Fig. 9; the corresponding spectra for 2a/3a and their complexes is given in the ESI.†
![]() | ||
| Fig. 9 Top: absorption spectra of triarylphosphine 2b and its complexes [Cu(2b)2(CH3CN)][PF6] 4b, [Ag(2b)2(hfa)] 6b and [AuCl(2b)] 8b. Bottom: absorption spectra of aryldialkylphosphine 3b and its complexes [Cu(3b)2(CH3CN)][PF6] 5b, [Ag(3b)2(hfa)] 7b and [AuCl(3b)] 9b. All measured in dry degassed tetrahydrofuran at room temperature (concentrations range from 3.0 × 10−6 to 1.1 × 10−5 M, see ESI†). | ||
Room-temperature fluorescence of the phosphine ligands was readily detected, with maxima of 534/527 nm or 533/526 nm, again depending on the boron substituents (Fig. 10). The Stokes shifts of 14–17 nm are small, which is common for the Bodipy fluorophore, and suggests that only small structural changes occur on excitation.6 The fluorescence quantum yields of 2b (0.29) and 3b (0.44) are typically high for Bodipy molecules and compare well to the parent Bodipy 10b (0.35, ESI†), which shows the phosphorus donor does not quench the fluorescence.
![]() | ||
| Fig. 10 Top: emission spectra of triarylphosphine 2b and its complexes [Cu(2b)2(CH3CN)][PF6] 4b, [Ag(2b)2(hfa)] 6b and [AuCl(2b)] 8b. Bottom: emission spectra of aryldialkylphosphine 3b and its complexes [Cu(3b)2(CH3CN)][PF6] 5b, [Ag(3b)2(hfa)] 7b and [AuCl(3b)] 9b. All measured in dry degassed tetrahydrofuran at room temperature, excitation wavelength = 485 nm, concentrations range from 1.9 × 10−6 to 4.0 × 10−6 M, see ESI†). | ||
This is unusual and, as with our previously reported Bodipy primary phosphines,15 contradicts several phosphine examples.4 However, it is perhaps to be expected, given that the DFT calculations (see Fig. 11 and ESI†) show there is no phosphorus character in the HOMO, HOMO−1 or HOMO−2 for 2a and 3a, nor in the HOMO or HOMO−1 for 2b and 3b, and that the energy difference between the HOMO and the first phosphorus-containing orbital is 0.9 eV for all the phosphine ligands (Fig. 11 and ESI†). The quantum yield for 3b is, perhaps surprisingly, also higher than that of the parent Bodipy which has no substituents on the meso phenyl ring (3b = 0.44 and 10b = 0.35). More detailed investigations into a Bodipy phosphine series could reveal how the quantum yield is affected by both the electronic and steric nature of the substituents on the phosphorus. Changing the methyl groups at the boron atom for phenyl groups severely quenches the fluorescence (compare 2b: ΦF = 0.29 to 2a: ΦF = 0.042), which is consistent with our previous findings.15 The absorption spectra of the complexes are very similar to those of the uncoordinated ligands (Fig. 9); wavelengths of the low energy transition fall in the range 519–512 nm. The corresponding molar extinction coefficients are large for the copper (4–5) and silver (6–7) complexes (ε = 133
000–171
000 M−1 cm−1), due to the presence of two Bodipy ligands; the monodentate gold complexes (8–9) retain similar values to the free ligands (ε = 74
000–85
000 M−1 cm−1).
![]() | ||
| Fig. 11 Calculated molecular orbital surfaces of the triarylphosphine 2a (top two rows) and the aryldialkylphosphine 3a (bottom two rows) from LUMO+1 to HOMO−5. | ||
The fluorescence spectra of the complexes 4b–9b are displayed in Fig. 10. On complexation, the fluorescence quantum yields are generally retained, with only a slight decrease observed on descending the group (for instance 2b: ΦF = 0.29, 8b: ΦF = 0.20). The gold species (8–9) have the lowest relative quantum yields, likely due to the heavy atom effect. Quenching is less pronounced for the aryldialkylphosphine complexes of 3b compared to those of the triarylphosphine 2b (Table 1, Fig. 10) and all three metal complexes of 3b have higher quantum yields than the parent Bodipy 10b (ΦF = 0.35). It is noteworthy that Gray et al. reported group 11 complexes which contained separated azadipyrromethene and triphenylphosphine ligands; however, the molar extinction coefficient and fluorescence quantum yields are significantly lower in those cases, 30
000–65
000 M−1 cm−1 and 0.0024–0.0039 respectively.37
Flash chromatography was performed on silica gel from Fluorochem (silica gel, 40–63 μ, 60 Å, LC301). Thin-layer chromatography was performed on Fisher aluminium-based plates with silica gel and fluorescent indicator (254 nm). Infrared spectra were recorded on a Varian 800 FT-IR spectrometer and mass spectrometry was carried out by the EPSRC National Mass Spectrometry Service Centre, Swansea. 1H, 13C{1H}, 31P{1H}, 19F{1H} and 11B{1H} NMR spectra were recorded on a JEOL Lambda 500 (1H 500.16 MHz) or JEOL ECS-400 (1H 399.78 MHz) spectrometer at room temperature (21 °C) using the indicated solvent as internal reference, unless specified otherwise; 1H and 13C shifts were relative to tetramethylsilane, 31P relative to 80% H3PO4, 11B relative to BF3·Et2O and 19F relative to CFCl3. It is worth noting that, as for dicyclohexylphenylphosphine,39 six unique cyclohexyl carbon signals are seen in the 13C{1H} NMR spectra for phosphines 3a and 3b and their respective complexes. The six signals arise as the two cyclohexyl rings are equivalent but the carbon atoms that are symmetrically equivalent are diastereotopic; these diastereotopic carbon atoms are also non-equivalent with respect to P–C coupling constants.
All calculations were carried out using Spartan 10 software.40 Full geometry optimizations of the studied compounds were performed using density functional theory with a B3LYP/6-31G* basis set. A vibrational analysis was performed at the same level to characterize calculated structures as minima.
Absorption spectra were recorded with a Hitachi Model U-3310 spectrophotometer while fluorescence studies were recorded with a Hitachi F-4500 fluorescence spectrophotometer. Solvents used for spectroscopic experiments were spectrophotometric grade. Absorption and emission spectra were recorded in dry degassed tetrahydrofuran solution at room temperature. Fluorescence quantum yields were measured with respect to 4,4-difluoro-8-phenyl-1,3,5,7-tetramethyl-2,6-diethyl-4-bora-3a,4a-diaza-s-indacene (ΦF = 0.76, λabs = 524 nm, λem = 537 nm, ε = 86
000 M−1 cm−1, tetrahydrofuran).36 Dyes were excited at 485 nm and excitation slits set to 5 nm.
:
3, Rf = 0.4) and gave an orange solid (0.50 g, 84%). A sample suitable for X-ray crystallographic analysis was obtained from chloroform–pentane. 1H NMR (400 MHz, CDCl3) δ 7.45–7.41 (m, 7H), 7.40–7.35 (m, 11H), 7.29–7.24 (m, 4H), 7.22–7.19 (m, 2H), 2.26 (q, 3JHH = 7.3 Hz, 4H), 1.82 (s, 6H), 1.44 (s, 6H), 0.94 (t, 3JHH = 7.3 Hz, 6H) ppm; 13C{1H} NMR (100 MHz, CDCl3) δ 153.0, 150.8 (br), 140.0, 137.9 (d, JCP = 11.5 Hz), 137.3, 136.7 (d, JCP = 10.5 Hz), 135.0, 133.8, 133.6, 133.4, 132.8, 130.6, 129.0, 128.9, 128.6 (d, JCP = 6.7 Hz), 127.1, 125.4, 17.3, 14.7, 14.5, 12.1 ppm; 31P{1H} NMR (162 MHz, CDCl3) δ −5.5 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −1.0 ppm; IR (neat):
= 2958 (w), 1542 (s), 1472 (s), 1396 (s), 1308 (m), 1170 (m), 1143 (m), 1061 (m), 971 (s), 775 (s) cm−1; HRMS (ESI+) exact mass calcd for C47H47N2B1P1 [M + H]+ requires m/z 681.3544, found m/z 681.3570 (2.6 ppm).
:
5, Rf = 0.3) to yield an orange solid (0.37 g, 60%). 1H NMR (400 MHz, CDCl3) δ 7.45–7.42 (m, 2H), 7.41–7.35 (m, 10H), 7.34–7.30 (m, 2H), 2.47 (s, 6H), 2.35 (q, 3JHH = 7.3 Hz, 4H), 1.36 (s, 6H), 1.01 (t, 3JHH = 7.3 Hz, 6H), 0.30 (s, 6H) ppm; 13C{1H} NMR (100 MHz, CDCl3) δ 150.6, 139.8, 137.9, 137.8, 136.7 (d, JCP = 11.5 Hz), 133.8, 133.6, 133.5, 132.4, 132.1, 132.0, 128.8, 128.5 (d, JCP = 6.7 Hz), 17.4, 14.7, 14.5, 11.9, 10.4 (br) ppm; 31P{1H} NMR (162 MHz, CDCl3) δ −5.5 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −1.9 ppm; IR (neat):
= 2924 (w), 2863 (w), 1552 (s), 1455 (m), 1372 (w), 1314 (s), 1170 (s), 1144 (s), 1064 (m), 977 (s) cm−1; HRMS (EI+) exact mass calcd for C37H43N2B1P1 [M + H]+ requires m/z 556.3288, found m/z 556.3294 (1.1 ppm).
:
4, Rf = 0.3) to yield an orange solid (0.42 g, 69%). 1H NMR (500 MHz, CDCl3) δ 7.59–7.56 (m, 2H), 7.41–7.33 (m, 6H), 7.23–7.17 (m, 6H), 2.22 (q, 3JHH = 7.8 Hz, 4H), 1.99–1.66 (m, 12H), 1.77 (s, 6H), 1.36–1.02 (m, 10H), 1.33 (s, 6H), 0.90 (t, 3JHH = 7.8 Hz, 6H) ppm, 13C{1H} NMR (126 MHz, CDCl3) δ 153.1, 150.8 (br), 140.5, 137.6, 135.2, 135.1, 135.0, 134.0, 133.0, 130.8, 128.4 (d, JCP = 7.6 Hz), 127.2, 125.6, 32.2 (d, 1JCP = 11.5 Hz), 30.1 (d, 2JCP = 16.3 Hz), 28.7 (d, 2JCP = 6.7 Hz), 27.3 (d, 3JCP = 12.5 Hz), 27.1 (d, 3JCP = 7.7 Hz), 26.7, 17.5, 14.8, 14.7, 12.1 ppm; 31P{1H} NMR (202 MHz, CDCl3) δ 2.7 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −0.7 ppm; IR (neat):
= 2925 (m), 2850 (m), 1548 (s), 1474 (m), 1384 (m), 1307 (s), 1168 (s), 1110 (m), 973 (s) cm−1; HRMS (AP+) calcd for C47H59B1N2P1 [M + H]+ requires m/z 692.4540, found m/z 692.4560 (2.9 ppm).
:
4, Rf = 0.4) to yield an orange solid (0.39 g, 62%). 1H NMR (400 MHz, CDCl3) δ 7.47 (m, 2H), 7.21 (d, 3JHH = 8.2 Hz, 2H), 2.37 (s, 6H), 2.23 (q, 3JHH = 7.3 Hz, 4H), 1.90–1.56 (m, 12H), 1.90 (s, 6H), 1.30–0.78 (m, 10H), 0.90 (t, 3JHH = 7.3 Hz, 6H), 0.21 (s, 6H) ppm; 13C{1H} NMR (100 MHz, CDCl3) δ 150.6, 140.2, 137.9, 135.0 (d, JCP = 19.2 Hz), 134.7 (d, JCP = 19.2 Hz), 133.8, 132.5, 129.1, 128.3 (d, JCP = 7.7 Hz), 32.1 (d, 1JCP = 12.5 Hz), 29.9 (d, 2JCP = 16.3 Hz), 28.7 (d, 2JCP = 6.7 Hz), 27.4 (d, 3JCP = 12.5 Hz), 27.1 (d, 3JCP = 6.7 Hz), 26.7, 17.6, 14.8, 14.4, 11.9, 10.5 (br) ppm; 31P{1H} NMR (162 MHz, CDCl3) δ 2.8 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −2.1 ppm; IR (neat):
= 2927 (w), 2856 (w), 1551 (s), 1448 (m), 1321 (m), 1171 (s), 1145 (s), 946 (s) cm−1; HRMS (AP+) calcd for C37H55B1N2P1 [M + H]+ requires m/z 568.4227, found m/z 568.4226 (0.1 ppm).
= 2960 (w), 2925 (w), 2869 (w), 1548 (s), 1473 (m), 1435 (m), 1397 (m), 1362 (m), 1305 (m), 1263 (w), 1173 (s), 1144 (m), 974 (s) cm−1; HRMS (ESI+) calcd for C94H92B2N4P2Cu1 [M − C2H3N1]+ requires m/z 1421.6346, found m/z 1421.6335 (0.8 ppm).
= 2959 (w), 2925 (w), 2869 (w), 1551 (s), 1471 (m), 1435 (m), 1360 (m), 1320 (s), 1264 (w), 1173 (s), 1145 (s), 1112 (m), 1026 (w), 981 (m), 945 (s) cm−1; HRMS (ESI+) calcd for C74H84B2N4P2Cu1 [M − C2H3N1]+ requires m/z 1173.5720, found m/z 1173.5927 (0.9 ppm).
= 2960 (w), 2929 (w), 2854 (w), 1549 (s), 1475 (m), 1449 (w), 1397 (w), 1362 (w), 1304 (m), 1263 (w), 1173 (s), 1145 (m), 1112 (m), 974 (s) cm−1; HRMS (ESI+) calcd for C94H116B2N4P2Cu1 [M − C2H3N1]+ requires m/z 1445.8224, found m/z 1445.8197 (1.9 ppm).
= 2959 (w), 2929 (w), 2854 (w), 1552 (s), 1448 (m), 1360 (m), 1320 (s), 1261 (m), 1173 (s), 1146 (s), 1112 (m), 1021 (w), 982 (m), 945 (s) cm−1; HRMS (ESI+) calcd for C74H108B2N4P2Cu1 [M − C2H3N1]+ requires m/z 1197.7598, found m/z 1197.7583 (1.3 ppm).
= 2966 (w), 2928 (w), 2870 (w), 1662 (m), 1520 (s), 1472 (m), 1434 (m), 1302 (m), 1171 (s), 972 (s) cm−1; HRMS (ESI+) calcd for C94H92B2N4P2Ag1 [M − (C5H1F6O2)]+ requires m/z 1469.6068, found m/z 1469.6056 (1.6 ppm).
= 2963 (w), 2932 (w), 2871 (w), 1660 (m), 1552 (s), 1538 (s), 1436 (m), 1321 (s), 1253 (s), 1172 (s), 1143 (s), 945 (s), 800 (s) cm−1; HRMS (ESI+) calcd for C74H84B2N4P2Ag1 [M − (C5H1F6O2)]+ requires m/z 1217.5475, found m/z 1217.5443 (2.5 ppm).
= 2928 (w), 2853 (w), 1661 (s), 1548 (s), 1522 (s), 1474 (m), 1303 (m), 1250 (m), 1172 (s), 1133 (s), 973 (s) cm−1; HRMS (ESI+) calcd for C94H116B2N4P2Ag1 [M − (C5H1F6O2)]+ requires m/z 1489.7979, found m/z 1489.7998 (1.3 ppm).
= 2930 (m), 2857 (w), 1663 (m), 1545 (s), 1525 (m), 1448 (m), 1361 (m), 1321 (s), 1251 (m), 1173 (s), 1146 (s), 944 (s) cm−1; HRMS (ESI+) calcd for C74H108B2N4P2Ag1 [M − (C5H1F6O2)]+ requires m/z 1242.7329, found m/z 1242.7354 (2.0 ppm).
:
1, Rf = 0.4) to yield an orange solid (0.101 g, 75%). A sample suitable for X-ray crystallographic analysis was obtained from chloroform–hexane. 1H NMR (400 MHz, CDCl3) δ 7.68–7.61 (m, 2H), 7.60–7.45 (m, 12H), 7.30–7.28 (m, 4H), 7.18–7.10 (m, 6H), 2.16 (q, 3JHH = 7.3 Hz, 4H), 1.69 (s, 6H), 1.26 (s, 6H), 0.82 (t, 3JHH = 7.3 Hz, 6H) ppm; 13C{1H} NMR (100 MHz, CDCl3) δ 153.7, 149.9 (br), 141.7, 138.2, 134.5, 134.3 (d, JCP = 13.4 Hz), 134.0 (d, JCP = 13.4 Hz), 133.7, 133.3, 132.1 (d, JCP = 2.9 Hz), 130.2, 130.0 (d, JCP = 11.5 Hz), 129.3 (d, JCP = 11.5 Hz), 128.6, 127.9, 127.1, 125.5, 17.3, 14.7, 14.6, 12.2 ppm; 31P{1H} NMR (202 MHz, CDCl3) δ 33.2 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −1.1 ppm; IR (neat):
= 2962 (w), 1544 (s), 1472 (m), 1435 (s), 1142 (m), 1101 (m), 972 (s) cm−1; HRMS (ESI+) calcd for C47H46B1N2P1Cl1Au1 [M]+ requires m/z 912.2960, found m/z 911.2989 (3.2 ppm).
:
1, Rf = 0.4). Yield 0.129 g (91%). 1H NMR (400 MHz, CDCl3) δ 7.66–7.58 (m, 2H), 7.57–7.52 (m, 4H), 7.52–7.44 (m, 8H), 2.44 (s, 6H), 2.30 (q, 3JHH = 7.3 Hz, 4H), 1.28 (s, 6H), 0.99 (t, 3JHH = 7.3 Hz, 6H), 0.27 (s, 6H) ppm; 13C{1H} NMR (100 MHz, CDCl3) δ 151.2, 141.6, 137.9, 134.3 (d, JCP = 13.4 Hz), 134.0 (d, JCP = 13.4 Hz), 133.1, 132.9, 132.1 (d, JCP = 1.9 Hz), 129.9 (d, JCP = 12.4 Hz), 129.3 (d, JCP = 11.5 Hz), 128.6, 128.5, 128.0, 17.4, 14.6, 14.3, 12.0, 10.3 (br) ppm; 31P{1H} NMR (162 MHz, CDCl3) δ 33.3 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −2.0 ppm; IR (neat):
= 2962 (w), 2926 (w), 2866 (w), 1552 (s), 1436 (m), 1314 (m), 1170 (s), 1101(s), 946 (s) cm−1; HRMS (AP+) calcd for C37H43B1N2P1Cl1Au1 [M + H]+ requires m/z 788.2642, found m/z 788.2627 (1.9 ppm).
:
1, Rf = 0.5). Yield 0.116 g (87%). A sample suitable for X-ray crystallographic analysis was obtained from chloroform–diethyl ether. 1H NMR (500 MHz, CDCl3) δ 7.89–7.78 (m, 2H), 7.52–7.49 (m, 2H), 7.37–7.30 (m, 4H), 7.25–7.16 (m, 6H), 2.32 (m, 2H), 2.21 (q, 3JHH = 7.3 Hz, 4H), 2.11–2.09 (m, 2H), 1.89–1.63 (m, 8H), 1.77 (s, 6H), 1.43–1.10 (m, 10H), 1.27 (s, 6H), 0.89 (t, 3JHH = 7.3 Hz, 6H) ppm; 13C{1H} NMR (126 MHz, CDCl3) δ 153.9, 150.3 (br), 141.3 (d, JCP = 2.9 Hz), 138.5, 135.3 (d, JCP = 11.6 Hz), 134.7, 133.9, 133.5, 130.4, 129.7 (d, JCP = 10.6 Hz), 127.3, 125.7, 125.2, 33.5 (d, 1JCP = 34.7 Hz), 29.7 (d, 2JCP = 1.9 Hz), 28.4, 26.5 (d, 3JCP = 5.7 Hz), 26.4 (d, 3JCP = 2.9 Hz), 25.9, 17.4, 14.8, 14.7, 12.2 ppm; 31P{1H} NMR (202 MHz, CDCl3) δ 51.4 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −1.0 ppm; IR (neat):
= 2926 (w), 2854 (w), 1545 (s), 1473 (m), 1304 (m), 1263 (m), 1172 (s), 1143 (m), 972 (s) cm−1; HRMS (AP+) calcd for C47H59B1N2P1Au1Cl1 [M + H]+ requires m/z 924.3897, found m/z 924.3904 (1.1 ppm).
:
1, Rf = 0.4). Yield 0.121 g (86%). A sample suitable for X-ray crystallographic analysis was obtained from chloroform–pentane. 1H NMR (500 MHz, CDCl3) δ 7.78 (m, 2H), 7.47 (m, 2H), 2.44 (s, 6H), 2.30 (q, 3JHH = 7.5 Hz, 4H), 2.09–1.70 (m, 10H), 1.39–0.85 (m, 12H), 1.21 (s, 6H), 0.98 (t, 3JHH = 7.5 Hz, 6H), 0.27 (s, 6H) ppm; 13C{1H} NMR (126 MHz, CDCl3) δ 151.3, 141.6 (d, JCP = 2.8 Hz), 138.2, 135.4 (d, JCP = 11.6 Hz), 133.1 (d, JCP = 17.3 Hz), 129.6 (d, JCP = 10.6 Hz), 128.6, 125.4, 125.0, 33.5 (d, 1JCP = 34.7 Hz), 29.6 (d, 2JCP = 2.9 Hz), 28.4, 26.5 (d, 3JCP = 6.7 Hz), 26.4 (d, 3JCP = 3.9 Hz), 25.9, 17.5, 14.8, 14.4, 11.9, 10.5 (br) ppm; 31P{1H} NMR (202 MHz, CDCl3) δ 51.6 ppm; 11B{1H} NMR (128 MHz, CDCl3) δ −2.1 ppm; IR (neat):
= 2924 (m), 2851 (w), 1552 (s), 1447 (m), 1359 (m), 1324 (s), 1263 (w), 1173 (s), 1147 (s), 945 (s) cm−1; HRMS (EI+) calcd for C37H53B1N2P1Au1Cl1 [M − H]+ requires m/z 798.3424, found m/z 798.3426 (0.2 ppm).
| Compound | 2a | 4a | 4b | 5a (structure A) | 5a (structure B) |
|---|---|---|---|---|---|
| Chemical formula | C47H46BN2P | C98H102B2CuN4O2P2 | C76H90B2CuN4OP2+·PF6− | C96H119B2CuN5P2+·PF6−·C4H10O·2CHCl3 | C94H116B2CuN4P2+·PF6−·2CHCl3 |
| Formula mass | 680.6 | 1514.9 | 1367.6 | 1947.9 | 1832.7 |
| Crystal system | Monoclinic | Monoclinic | Triclinic | Triclinic | Monoclinic |
| a/Å | 29.596(7) | 22.626(2) | 10.7978(6) | 11.2490(2) | 13.7756(6) |
| b/Å | 8.231(2) | 10.2574(8) | 12.4349(7) | 17.1875(4) | 10.2495(5) |
| c/Å | 31.073(12) | 20.8126(19) | 28.2720(15) | 26.6167(6) | 33.6122(17) |
| α/° | 80.643(4) | 93.8881(19) | |||
| β/° | 102.186(2) | 111.403(10) | 86.405(4) | 93.6056(17) | 91.672(4) |
| γ/° | 72.103(5) | 92.9238(19) | |||
| Unit cell volume/Å3 | 7399(4) | 4497.2(7) | 3564.0(4) | 5116.22(19) | 4743.8(4) |
| Space group | I2/a | P2/c |
P![]() |
P![]() |
P2/c |
| Z | 8 | 2 | 2 | 2 | 2 |
| μ/mm−1 | 0.075 | 0.327 | 1.575 | 0.476 | 0.508 |
| No. of reflections measured | 28 804 |
32 492 |
21 401 |
83 501 |
30 847 |
| No. of independent reflections | 6727 | 7915 | 11 052 |
20 525 |
9235 |
| R int | 0.0601 | 0.1080 | 0.0392 | 0.0496 | 0.0394 |
| R (F, F2 > 2σ) | 0.0457 | 0.0803 | 0.0617 | 0.0728 | 0.0827 |
| R w (F2, all data) | 0.1133 | 0.2213 | 0.1729 | 0.2236 | 0.2228 |
| Goodness of fit on F2 | 1.065 | 1.033 | 1.035 | 1.023 | 1.072 |
| Difference map extremes/e Å−3 | 0.32, −0.27 | 0.39, −0.41 | 0.72, −0.38 | 1.69, −1.32 | 1.28, −0.64 |
| Compound | 6a | 7b | 8a | 9a | 9b |
|---|---|---|---|---|---|
| Chemical formula | C99H93AgB2F6N4O2P2 | C79H109AgB2F6N4O2P2 | C47H46AuBClN2P2·CHCl3 | C47H58AuBClN2P·0.5C4H10O | C37H54AuBClN2P·CHCl3 |
| Formula mass | 1676.2 | 1452.1 | 1032.4 | 962.2 | 920.4 |
| Crystal system | Monoclinic | Monoclinic | Orthorhombic | Triclinic | Monoclinic |
| a/Å | 17.8281(6) | 34.386(6) | 9.5273(7) | 8.9183(14) | 18.2559(8) |
| b/Å | 16.4975(4) | 10.3299(19) | 15.9516(10) | 15.431(3) | 9.4353(4) |
| c/Å | 28.2893(12) | 24.444(5) | 28.6394(14) | 17.126(3) | 23.1349(10) |
| α/° | 106.221(2) | ||||
| β/° | 93.976(5) | 107.786(2) | 91.812(2) | 93.337(4) | |
| γ/° | 97.007(2) | ||||
| Unit cell volume/Å3 | 8300.4(5) | 8268(3) | 4352.5(5) | 2240.8(7) | 3978.2(3) |
| Space group | I2/a | C2/c | P212121 |
P![]() |
P21/c |
| Z | 4 | 4 | 4 | 2 | 4 |
| μ/mm−1 | 2.857 | 0.285 | 9.234 | 3.110 | 4.036 |
| No. of reflections measured | 13 509 |
35 858 |
11 804 |
23 163 |
40 350 |
| No. of independent reflections | 6411 | 9121 | 6623 | 10 658 |
9004 |
| R int | 0.0417 | 0.1189 | 0.0477 | 0.0431 | 0.0409 |
| R (F, F2 > 2σ) | 0.0476 | 0.0839 | 0.0544 | 0.0432 | 0.0307 |
| R w (F2, all data) | 0.1272 | 0.2293 | 0.1495 | 0.0964 | 0.0668 |
| Goodness of fit on F2 | 0.958 | 1.019 | 1.002 | 1.098 | 1.059 |
| Difference map extremes/e Å−3 | 0.59, −0.54 | 0.82, −0.85 | 3.13, −1.66 | 1.49, −1.09 | 1.35, −1.10 |
Footnote |
| † Electronic supplementary information (ESI) available: Experimental methods, spectroscopic and crystallographic characterisation, photophysical measurements and molecular modelling details. CCDC 987389, 987388, 987387, 987386, 987385, 987390, 987384, 987391, 987383 and 987382. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c4dt00704b |
| This journal is © The Royal Society of Chemistry 2014 |