Open Access Article
Anyie P.
Atencio
a,
Alba
Sevillano
a,
Ariadna
Lázaro
ab,
Zoraida
Freixa
cd,
David
Aguilà
ab,
Inmaculada
Angurell
ab and
Laura
Rodríguez
*ab
aDepartament de Química Inorgànica i Orgànica, Secció de Química Inorgànica, Universitat de Barcelona, Martí i Franquès 1-11, E-08028 Barcelona, Spain. E-mail: laurarodriguezr@ub.edu
bInstitut de Nanociència i Nanotecnologia (IN2UB), Universitat de Barcelona, 08028 Barcelona, Spain
cFacultad de Química, Universidad del País Vasco (UPV/EHU), San Sebastián, 20018, Spain
dIKERBASQUE, Basque Fundation for Science, Bilbao, 48013, Spain
First published on 8th October 2025
Two series of mono- or dinuclear gold(I) complexes incorporating an ethynyltriphenylene chromophore and various mono- and diphosphanes have been synthesized and characterized to explore the interplay between the ligand structure, aurophilic interactions, and photophysical properties. The complexes display dual emission behaviour, with fluorescence dominating under air-equilibrated conditions and phosphorescence emerging under oxygen-free environments. Dinuclear compounds bearing diphosphane linkers show enhanced phosphorescence, attributed to shorter Au(I)⋯Au(I) distances that facilitate intersystem crossing (ISC). Upon immobilization in PMMA matrices, all selected compounds exhibit efficient room-temperature phosphorescence even in the presence of oxygen, with emission quantum yields up to 33% and lifetimes extending to nearly one millisecond. These findings highlight the potential of structural design and matrix confinement to engineer metal-based luminophores for applications in time-gated imaging, security inks, and light-emitting devices.
At the same time, playing with nuclearity (mono- vs. dinuclear), flexibility/rigidity and conformation of the bridging ligands is key for the resulting photophysical properties. These factors will ultimately govern the resulting supramolecular assemblies generated, including the establishment of both intra- and intermolecular contacts, and the emissions present as a result (fluorescence, phosphorescence or dual emission).26–32
The insertion of a gold(I) centre into a π-conjugated backbone (alkynylated aromatics) can represent a solid foundation on which to build emissive structures, with a tuneable electronic structure and molecular arrangement.3,6,10,33 Triphenylene, a fully planar, rigid polycyclic aromatic hydrocarbon, is an interesting and easily accessible skeleton to be used as a luminophore, and its ethynyl-functionalization makes it capable of being coordinated directly to gold(I) through a conjugated system.
Additionally, phosphine ligands, and in particular mono and diphosphines, provide further modularity through their electronic properties, steric demand and conformational flexibility. A variety of mono- and dinuclear gold(I) complexes were synthesized, structurally characterized, and their photophysical properties were investigated.6,10,11,14,15,18,31–34 The aim of this study is to determine if and how the nature of the phosphine (basicity, bulkiness, and rigidity) tunes the emission properties of these complexes. Moreover, the effect of immobilization in a PMMA matrix was also investigated, as a means to quench non-radiative decay channels and access room-temperature phosphorescence.
The complexes were successfully characterized by 1H and 31P{1H} NMR, and IR spectroscopy and mass spectrometry. The 31P{1H} NMR spectra display, in all cases, a sharp singlet approximately 50–60 ppm downfield-shifted relative to the free phosphine, which is consistent with that previously reported for similar complexes.13–15,18,20 The presence of only one singlet also in the case of derivatives 2 confirms the binuclear structure of these compounds and the equivalence of their phosphorus atoms in solution. In the 1H NMR spectra, the signals corresponding to both the chromophore and the phosphine moieties were clearly observed with the expected integration and were perfectly assigned thanks to 13C and HSQC NMR spectra. These spectra also reflect the symmetry of the diphosphine ligands within the complex in solution. Additionally, ESI(+) mass spectrometry confirmed the formation of the desired complexes through the detection of the corresponding [M + H]+ or [M + Na]+ molecular ions.
Crystals suitable for single crystal X-ray diffraction were obtained by slow diffusion of Et2O or hexane, respectively, into dichloromethane solutions of 1c or 2i. The compounds crystallize in the P
(1c) and P21/c (2i) space groups of the triclinic and monoclinic crystal systems, respectively, and confirm the structure and nuclearity of each series. The corresponding molecular structures are presented in Fig. 1 and selected bond lengths and angles are summarized in Table 1.
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| Fig. 1 X-ray crystal structures of 1c (a) and 2i (c). Solvates and hydrogen atoms were omitted for clarity. Colour key: yellow = Au; orange = P; grey = C. | ||
| Distance | [Å] | Angle | [°] |
|---|---|---|---|
| 1c | |||
| Au(1)–C(1) | 2.005(6) | P(1)–Au(1)–C(1) | 176.9(2) |
| Au(2)–C(39) | 2.016(8) | P(2)–Au(2)–C(51) | 172.7(2) |
| P(1)–Au(1) | 2.2737(18) | Au(1)–P(1)–C(21) | 113.6(2) |
| P(2)–Au(2) | 2.278(2) | Au(2)–P(2)–C(71) | 117.5(3) |
| P(1)–C(21) | 1.802(7) | C(1)–C(2)–C(3) | 175.5(8) |
| P(2)–C(71) | 1.829(8) | C(39)–C(40)–C(41) | 176.5(9) |
| C(1)–C(2) | 1.189(9) | ||
| C(39)–C(40) | 1.183(11) | ||
| 2i | |||
| Au(1)–Au(2) | 3.0998(5) | P1–Au1–C56 | 172.8(2) |
| P1–Au1 | 2.284(2) | P2–Au2–C1 | 175.4(2) |
| Au1–C56 | 2.031(9) | C1–C2–C3 | 178.4(9) |
| Au2–P2 | 2.287(2) | C58–C57–C56 | 174.8(9) |
| Au2–C1 | 2.023(9) | Au1–Au2–P2 | 103.58(6) |
| C1–C2 | 1.19(1) | Au2–Au1–P1 | 107.93(6) |
| C57–C56 | 1.16(1) | Au2–C1–C2 | 178.2(8) |
| Au1–C56–C57 | 174.7(8) | ||
Compound 1c exhibits two mononuclear molecules in the asymmetric unit, each of them showing the bonding between the PPh3 phosphine and the gold precursor. A near linear geometry around the gold atom is observed, with P–Au–C angles of 176.9(2) and 172.7(2)°, respectively. Compound 2i demonstrates the dinuclear nature of series 2, with the diphosphine connecting the two AuL units and promoting a short intermolecular Au(I)⋯Au(I) interaction between both gold cations (3.0998(5) Å). The values of the corresponding P–Au–C angles (172.8(2) and 175.4(2)°) are similar to 1c, showing again a slight departure from a linear arrangement. For both compounds, the Au–C and C
C distances and P–Au–C and Au–C
C angles (Table 1) are in the usual ranges for Au(I) alkynyl complexes.10,34
The 3D packing of the mononuclear complexes exhibits a conformation driven by the establishment of π–π and C–H⋯π interactions. In complex 1c, the intermolecular interactions occur in two ways: (1) between the alkyl/aryl substituents of the phosphine and the triphenylene unit, and (2) between the C–H groups of the triphenylene and the C
C group of a neighbouring molecule, as shown in Fig. S44. As a result, the molecules arrange themselves into alternating dimers relative to each other, although they are not entirely parallel. In the case of the bimetallic complex 2i, the molecular structure reflects the spiral structure of the chiral ligand. As the ligand has been used as a racemate, the compound crystallizes in a centrosymmetric group containing both enantiomers. The unit cell could be described as containing the centroid of four molecules (two pairs of enantiomers), in addition to 4 solvent molecules. Each pair of enantiomers is related by a glide plane and both pairs relate one each other through an inversion centre located in the middle point of the unit cell (see Fig. S44). The ligand used, SPANphos, is a highly flexible ligand originally designed as a trans-chelator.35 In 2i the spirobichromane backbone of the ligand adopts an extended conformation with the spiro rings in what has been described as a boat–boat conformation, similar to that encountered in other dinuclear SPANphos complexes.36 Accordingly, in this conformation, the two phosphorus atoms are at a rather large distance, and coordinate to two different gold(I) centres, in a bridging manner (5.791(3) Å). Eventually, the final conformation is stabilized by the intramolecular Au(I)⋯Au(I) interaction, forcing the disposition of the two triphenylene moieties in a cross-like spatial arrangement. No intermolecular aurophilic interactions are present in 2i.
| Compound | Absorption λmax, nm (ε × 104 M−1 cm−1) | Fluorescence emission air-eq., λmax (nm) | Phosphorescence emission N2-sat, λmax (nm) | I Ph /I Fl |
|---|---|---|---|---|
| L | 268 (9.79), 290 (1.17) | 375 | — | — |
| 1a | 278 (8.44), 310 (3.50), 324 (4.52) | 380 | 520 | 0.44 |
| 1b | 278 (5.82), 310 (2.73), 324 (3.51) | 380 | 520 | 2.67 |
| 1c | 279 (4.83), 309 (2.46), 328 (3.39) | 379 | 520 | 3.87 |
| 1d | 278 (5.72), 310 (3.10), 328 (4.06) | 367 | 520 | 8.02 |
| 1e | 277 (6.46), 310 (4.43), 327 (4.42) | 380 | 520 | 11.72 |
| 2f | 277 (10.7), 310 (5.58), 327 (7.36) | 380 | 520 | 0.95 |
| 2g | 279 (8.03), 315 (4.08), 331 (3.70) | 382 | 522 | 8.78 |
| 2h | 277 (3.64), 315 (1.66), 332 (1.73) | 382 | 524 | 4.52 |
| 2i | 278 (12.4), 315 (6.18), 329 (7.42) | 382 | 524 | 5.19 |
The absorption spectra of all the compounds display characteristic bands between 250 and 350 nm, attributed to π–π* intraligand transitions associated with the triphenylene ligand (Fig. 2). These bands are ca. 10–20 nm red-shifted for the gold(I) complexes with respect to L. The lowest-energy absorption bands are attributed to π → π* charge transfer nature transitions while the following prominent band is assigned to a combined character of intra-ligand charge transfer (ILCT) and ligand-to-metal charge transfer (LMCT), in agreement with previous theoretical calculations.31 Lower absorption intensities and broad bands were recorded for dppm (2g) and xantphos (2h) derivatives due to lower solubility and formation of small aggregates under these conditions.
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| Fig. 2 Absorption spectra of 4.0 × 10−6 M dichloromethane solutions of (a) series 1 and (b) series 2 complexes. | ||
The emission spectra of the gold(I) complexes show a vibronically structured fluorescence band as the dominant emission under air-equilibrated conditions, while phosphorescence becomes the most intense emissive band upon oxygen removal (N2-saturated samples, Fig. 3). The emergence of phosphorescence is attributed to the heavy atom effect of the Au(I) centre, as evidenced by the purely fluorescence emission observed for the organic precursor ligand. Among the mononuclear complexes, compounds 1d and 1e (featuring PTA and DAPTA ligands, respectively) exhibited lower solubility in organic solvents and displayed a greater contribution from phosphorescence.37 Analysis of the emission spectra of the dinuclear complexes reveals an increased phosphorescence-to-fluorescence intensity ratio for compounds 2g, 2h, and 2i (see Table 2). Notably, compound 2g shows significant band broadening (also detected in the NMR spectrum, see the SI), which, along with the reduced solubility observed in its absorption spectrum, suggests close proximity between the gold(I) centres, as in the case of 2i.28 This spatial arrangement, likely maintained in solution due to the structural disposition of the two Au(I) atoms, facilitates intersystem crossing and enhances the phosphorescence emission. As expected, these aurophilic interactions are less important for 2f, that contains the more flexible dppe diphosphane as the bridging ligand. The effect of the gold(I) atom in the intersystem crossing is also reflected in the resulting fluorescence and phosphorescence quantum yields (see Table 3) that are one order of magnitude smaller for the gold(I) complexes with respect to L.
Emission lifetimes of the fluorescence bands are in the order of 10 ns, supporting the fluorescence assignment as 1IL emission (see Table 3).31,38,39 The vibronically structured shape of the red-shifted emission and comparison with the literature,14,30,31 together with the recorded emission lifetimes in the order of microseconds, supports an 3IL assignment. Phosphorescence emission lifetimes are around 100–145 μs for the mononuclear compounds while they are smaller for the dinuclear ones. Compounds 2f and 2i are those with the larger phosphorescence quantum yields and lifetimes within the dinuclear series, probably due to the lower possibility of intramolecular aurophilic contacts for the compounds containing the more flexible conformations. The smaller phosphorescence efficiency of the dinuclear compounds
with respect to the mononuclear ones can be ascribed to more favoured deactivation processes, in agreement with the larger values of knr, that are expected to be more favoured in the presence of intramolecular aurophilic contacts (see Table S3).
The results indicate a global decrease in the fluorescence emission in all cases, having recorded almost pure room temperature phosphorescence in all cases under these conditions, even in the presence of oxygen, in air-equilibrated solutions (see Fig. 4). The residual fluorescence emission in compound 1a disappears after oxygen removal.
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| Fig. 4 Emission spectra of the selected compounds immobilized in PMMA matrixes under air equilibrated conditions (a) and (b) and nitrogen saturated samples (c) and (d). | ||
The phosphorescence quantum yields and lifetimes were also recorded achieving very interesting results with about 20–33% emission efficiency (Table 4). The large values of the emission lifetimes previously recorded under N2-saturated conditions in solution are now achieved in air-equilibrated solid samples and increase to 400–925 μs when oxygen is removed, giving rise to emissive materials with quite interesting emission efficiencies and very long lifetimes, being half and one millisecond, respectively. This is mainly due to the reduction of the non-radiative deactivation pathways (restricted internal rotations around P–C bonds, among others) within the immobilized PMMA material (Table S4). These interesting photophysical properties would be relevant for the development of emissive materials with potential applications such as PhOLEDs,42 Time-Gated Bioimaging & Sensing43,44 and security and anti-counterfeiting.45–48
Immobilization in PMMA matrices efficiently suppresses non-radiative decay pathways, yielding materials with high phosphorescence quantum yields and extended lifetimes even under ambient conditions. These results showcase the promise of gold(I)-based systems as tunable, long-lived emissive materials suitable for technological applications in optoelectronics and luminescence sensing.
Infrared spectra have been recorded on an FT-IR Nicolet™ iS™ 5 spectrophotometer. 1H NMR (δ(TMS) = 0.0 ppm), 31P{1H} NMR (δ(85% H3PO4) = 0.0 ppm) and 13C{1H} NMR spectra were recorded at 400 or 500 MHz using Varian and Bruker spectrometers at 25 °C. ESI mass spectra have been recorded on a Fisons VG Quatro spectrometer. Absorption spectra have been recorded on a Varian Cary 100 Bio UV spectrophotometer, and emission spectra on a Horiba-Jobin-Ybon SPEX Nanolog spectrofluorimeter. Quantum yields have been recorded on a Hamamatsu Absolute PL Quantum Yield Spectrometer C11347. Luminescence lifetimes were measured on a JYF-DELTAPRO-NL equipment upon excitation of the samples with a 280 nm NanoLED and collecting the decays through a bandpass filter of 400 nm.
Single crystal data for compounds 1c and 2i were collected at BL13-XALOC beamline49 of the ALBA synchrotron (λ = 0.72931) at 100 K. Crystals were mounted with Paratone N grease on a MiTegen kapton loop and placed in the N2 stream of an Oxford Cryosystems Cryostream. Both structures were solved by intrinsic phasing (SHELXT)50 and refined by full-matrix least squares on F2 using Olex251 utilising the SHELXL module.52 Anisotropic displacement parameters were assigned to non-H atoms and isotropic displacement parameters for all H atoms were constrained to multiples of the equivalent displacement parameters of their parent atoms with Uiso(H) = 1.2Ueq.(CH) or 1.5Ueq.(CH2, CH3) of their respective parent atoms. CCDC 2481588 and 2482223 contain the supporting crystallographic data for the two structures.
:
1) was reacted with sodium acetate (37 mg, 0.46 mmol) for 1 h at room temperature. Then, [AuCl(tht)] (72 mg, 0.22 mmol) was added, and a yellow precipitate was instantly generated. The mixture was stirred for 1 h at room temperature. Finally, the solid was filtered and dried under vacuum. IR (
, cm−1): 3079 (Csp2-H st.), 1983 (C
C st.) 1605 + 1488 (C
C st.), 748 (Csp2-H be).
, cm−1): 3081 (Csp2-H st.), 2966 (Csp3-H st.), 2107 (C
C st.), 1655 + 1487 (C
C st.), 753 (Csp2-H be.). 1H NMR (500 MHz, CDCl3, 298 K): δ: 8.79 (d, 4J = 1.6 Hz, 1H, H1), 8.65–8.57 (m, 4H, H4–H7), 8.52 (d, 3J = 8.6 Hz, 1H, H3), 7.74 (dd, 3J = 8.5 Hz, 4J = 1.6 Hz, 1H, H2), 7.69–7.57 (m, 4H, H8–H11), 1.62 (d, 9H, P-CH3). 31P{1H} NMR (202 MHz, CDCl3, 298 K): δ:1.2 (s). HR ESI-MS(+) m/z: 797.105 ([2M − L]+, calcd 797.107); 547.088 ([M + Na]+, calcd 547.087), 349.055 ([Au(PMe3)2]+, calcd 349.055).
, cm−1): 3069 (Csp2-H st.), 2966 + 2929 (Csp3-H st.), 2116 (C
C st.), 1605 + 1488 (C
C Ar st.), 1449 (CH2 be.), 1379 (CH3 be.), 759 (Csp2-H be.). 1H NMR (CD2Cl2, 400 MHz) δ: 8.70 (d, 4J = 1.6 Hz, 1H, H1), 8.67–8.60 (m, 4H, H4–7), 8.53 (d, 3J = 8.4 Hz, 1H, H3), 7.68–7.64 (m, 5H, H2,8–H11), 1.86 (dq, 2JHP = 9.6 Hz, 3JHH = 7.6 Hz, 6H, P-CH2-CH3), 1.24 (dt, 3JHP = 18 Hz, 3JHH = 7.6 Hz, 9H, P-CH2-CH3). 31P{1H} NMR (CD2Cl2, 161.9 MHz) δ: 38.3. ESI-MS(+) m/z: 567.15 ([M + H]+, calcd 567.15), 589.14 ([M + Na]+, calcd 589.13), 881.20 ([2M − L]+, calcd 881.20), 1155.28 ([2M + Na]+, calcd 1155.28).
, cm−1): 3051 (Csp2-H st.), 2961 (C–H st.), 2112 (C
C st.), 1604 + 1481 (C
C st.), 752 (Csp2-H be.). 1H NMR (400 MHz, CDCl3, 298 K): δ: 8.84 (d, 1H, 4J = 1.6 Hz, H1), 8.66–8.58 (m, 4H, Hd), 8.54 (d, 1H, 3J = 8.6 Hz, H3), 7.79 (dd, 1H, 3J = 8.5 Hz, 4J = 1.6 Hz, H2), 7.66–7.45 (m, 19H, PPh3 + H4–11). 31P{1H} NMR (161.9 MHz, CDCl3, 298 K): δ: 42.3. HR ESI-MS(+) m/z: 1169.201 ([2M − L]+, calcd 1169.201), 721.148 ([Au(PPh3)2]+, calcd 721.149).
, cm−1): 2930 (Csp3-H st.), 2116 (C
C st.), 1603 + 1491 (C
C st.), 1451 (CH2 be.), 757 (Csp2-H be.). 1H NMR (400 MHz, DMSO-d6, 298 K) δ: 8.84–8.72 (m, 4H, H4–7), 8.69 (d, 3J = 8.7 Hz, 1H, H3), 8.63 (d, 4J = 1.4 Hz, 1H, H1), 7.77–7.67 (m, 4H, H8–11), 7.56 (dd, 1H, 3J = 8.4Hz, 4J = 1.5 Hz, H2), 4.55 (d, 2J = 12 Hz, 3H, P-CH2-N), 4.38 (d, 2J = 16 Hz, 3H, P-CH2-N), 4.32 (s, 6H, N-CH2-N). 31P{1H} NMR (161.9 MHz, DMSO-d6, 298 K) δ: −48.6; HR ESI-MS(+) m/z: 606.134 ([M + H]+, calcd 606.137), m/z: 511.12 ([Au(PTA)2]+, calcd 511.120), m/z: 158.084 ([PTA + H]+, calcd 158.084).
, cm−1): 3051 (Csp2-H st.), 2923 (Csp3-H st.), 2109 (C
C st.), 1637 (C
O st.), 1370 (CH3 be.), 755 (Csp2-H be. op.). 1H NMR (CDCl3, 400 MHz) δ: 8.79 (s, 1H, H1), 8.64–8.57 (m, 4H, H4–11), 8.54 (d, 3J = 8.6 Hz, 1H, H3), 7.73 (d, 4J = 8.3 Hz, 1H, H2), 7.67–7.62 (m, 4H, H4–11), 5.78 (d, 2J = 14.4 Hz, 1H, N-CH2-N, Hb), 5.67 (dbr, 2J = 15.9 Hz, 3J = 7.2 Hz, 1H, P-CH2-N, Hd), 4.93 (d, 2J = 14.0 Hz, 1H, N-CH2-N, Hc), 4.69 (dbr, 1H, P-CH2-N, Ha), 4.63 (d, 2J = 14.5 Hz, 1H, N-CH2-N, Hc′), 4.18 (dbr, 2J = 15.5 Hz, 1H, P-CH2-N, Ha′), 4.05 (d, 2J = 14.4 Hz, 1H, N-CH2-N, Hb′), 3.9 (s, 2H, P-CH2-N, He), 3.62 (dd, 2J = 13.1 Hz, 1H, P-CH2-N, Hd′), 2.11–2.10 (s + s, 6H, CH3). 13C{1H} NMR (CDCl3, 100 MHz) δ: 170.2 (C
O), 170.0 (C′
O), 130.9 (C2), 130.1–129.4 (C4d), 127.6–127.4 (C1, C4–C11), 123.6–123.4 (C3, C4-C11), 67.5 (N-CH2-N, Cc), 62.3 (N-CH2-N, Cb), 49.6 (d, J = 25.9 Hz, P-CH2-N, Ce), 45.0 (d, J = 26.2 Hz, P-CH2-N, Ca), 39.8 (d, J = 27.2 Hz, P-CH2-N, Cd), 21.7 (CH3), 21.4 (CH3). 31P{1H} NMR (CDCl3, 202 MHz) δ: −22.1. ESI-MS(+) m/z: 230.11 ([DAPTA + H]+, calcd 230.11), 252.09 ([DAPTA + Na]+, calcd 252.09).
, cm−1): 3050 (Csp2-H st.), 2947 (Csp3-H st.), 2110 (C
C st.) 1610 + 1487 (C
C st.), 1451 (CH2 be.), 753 (Csp2-H br). 1H NMR (500 MHz, CD2Cl2, 298 K): δ: 8.76 (d, 4J = 1.2 Hz, 2H, H1), 8.60–8.68 (m, 8H, H4–11), 8.56 (d, 3J = 8.5 Hz, 2H, H3), 7.74–7.85 (m, 8H, H4–11), 7.72 (dd, 3J = 8.5 Hz, 4J = 1.5 Hz, 2H, H2), 7.64–7.70 (m, 8H, PPh2), 7.52–7.60 (m, 12H, PPh2), 2.80 (s, 4H, PPh2-CH2-CH2-PPh2). 31P{1H} NMR (202 MHz, CD2Cl2, 298 K): δ: 39.4 (s). HR ESI-MS(+) m/z: 2612.469 ([2M + Na]+, calcd 2612.474); 2337.387 ([2M − L]+, calcd 2337.394); 1889.341 ([2M − AuL2]+, calcd 1889.342); 1441.285 ([2M − Au2L3]+, calcd 1441.289); 1317.229 ([M + Na]+, calcd 1317.230); 1043.152 ([M − L1]+, calcd 1043.155); 993.237 ([Au(dppe)2]+, calcd 993.237); 819.127 ([2M − AuL3]2+, calcd 819.128); 595.101 ([Au2(dppe)2]2+, calcd 595.102).
, cm−1): 3049 (Csp2-H st.), 2957(Csp3-H st.), 2105 (C
C st.) 1607 + 148 (C
C st.), 1459 (CH2 be.), 752 (Csp2-H be.). 1H NMR (400 MHz, CD2Cl2, 298 K) δ: 8.53 (d, 4J = 1.1 Hz, 2H, H1), 8.39 (d, 2H, 3J = 8.0 Hz, H3), 8.34–7.97 (m, 8H, H4–11), 7.75–7.65 (m, 8H, H4–11), 7.58 (dd, 3J = 8.5 Hz, 4J = 1.5 Hz, 2H, H2), 7.55–7.27 (m, 20H, PPh2), 3.71 (t, 2J = 11.2 Hz, 2H, PPh2-CH2-PPh2). 31P{1H} NMR (161.9 MHz, CD2Cl2, 298 K) δ: 32.4 (s). HR ESI-MS(+) m/z: 1303.214 ([M + Na]+, calcd 1303.214), 1861.309 ([2M − AuL2]+, calcd 1861.309), 2309.362 ([2M − L]+, calcd 2309.363), 2583.433 ([2M + Na]+, calcd 2583.439).
, cm−1): 3066 (Csp2-H st.), 2962 (Csp3-H st.), 2107 (C
C st.), 1604 + 1480 (C
C st.), 1258 (C-O st.), 752 (Csp2-H be.). 1H NMR (400 MHz, CD2Cl2, 298 K) δ: 8.73–8.51 (m, 10H, CH Ar), 7.70–6.60 (m, 38H, CH Ar), 1.70 (s, 6H, CH3). 31P{1H} NMR (161.9 MHz, CD2Cl2, 298 K) δ: 31.8. HR ESI-MS(+) m/z: 1223.209 ([M − L]+, calcd 1223.211); 1353.351 ([2M − Au3L4]+, calcd 1353.352); 1801.404 ([2M − Au2L3]+, calcd 1801.404); 2249.449 ([2M − AuL2]+, calcd 2249.457).
, cm−1): 3047 (Csp2-H st.), 2958 (Csp3-H st.), 2109 (C
C st.) 1606 + 1428 (C
C st.), 1364 (CH3 be.), 1096 (C-O st.), 748 (Csp2-H be.). 1H NMR (500 MHz, CD2Cl2, 298 K) δ: 8.70–8.41 (m, 12 H, CH Ar), 7.93–7.16 (m, 32 H, CH Ar), 6.58 (dd, 3J = 12 Hz, 4J = 1.5 Hz, 2H, CH Ar, Ha), 2.06 (s, 6H, CH3-Ph, Hb), 1.82 (d, 2J = 14.5 Hz, 2H, R-CH2-R, Hc), 1.70 (d, 2J = 14.5 Hz, 2H, R-CH2-R, Hc′), 1.2 (s, 6H, CH3-R, Hd), 1.02 (s, 6H, CH3-R, Hd′). 31P{1H} NMR (202 MHz, CD2Cl2, 298 K) δ: 34.9. HR ESI-MS(+) m/z: 1349.313 ([M − L]+, calcd 1349.316), 901.263 ([M − AuL2]+, calcd 901.263).
000) was dissolved in chloroform at a concentration of 200 mg mL−1. Subsequently, 50 μL of polymer solution was added to the same volume a solution of the sample at a concentration of 2 mM. The films were drop cast onto a quartz substrate at room temperature to avoid any thermal annealing.
CCDC 2481588 (1c) and 2482223 (2i) contain the supplementary crystallographic data for this paper.53a,b
Footnote |
| † Dedicated to Professor Resnati, celebrating a career in fluorine and noncovalent chemistry on the occasion of his 70th birthday. |
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