Open Access Article
Mariia
Beliaeva
a,
Andrey
Belyaev
a,
Henna
Korhonen
a,
Ondrej
Mrózek
b,
Janne
Jänis
a,
Andreas
Steffen
*b and
Igor O.
Koshevoy
*a
aDepartment of Chemistry and Sustainable Technology, University of Eastern Finland, Yliopistokatu 7, Joensuu, 80101, Finland. E-mail: igor.koshevoy@uef.fi
bDepartment of Chemistry and Chemical Biology, TU Dortmund University, Otto-Hahn-Str. 6, 44227 Dortmund, Germany. E-mail: andreas.steffen@tu-dortmund.de
First published on 4th November 2025
Hybrid phosphines with anionic hard donor functions can be used to create an adaptable ligand environment for soft late transition metals. Herein, we show that the change of coordination of a diphosphine–phosphinic acid (P3OOH) in response to acid–base interactions or hydrogen bonding results in structural transformations of a disilver complex [Ag2(P3OO)2] (1) to give solvated and protonated derivatives [Ag2(P3OOH)2]2+ (2) and [Ag3(P3OO)3H]+ (3), accompanied by the alteration of the quantum yield of the solid-state photoluminescence from 0.06 up to 0.69. The related diphosphine–phosphide oxide complexes [M2(P3O)2] (M = Ag, Au) are oxidized to phosphinate compounds 2 and non-luminescent [Au2(P3OO)2H]+ (5) in the presence of triflic acid. Alternatively, [Au2(P3O)2] readily accommodates an additional gold(I) ion to yield a trinuclear cluster [Au3(P3O)2]+ (6), which is brightly sky-blue phosphorescent in the crystalline state (Φem = 0.76). The phosphide oxide group −P
O in 6 is stable towards oxidation under acidic conditions in solution but undergoes protonation that results in two orders of magnitude (>170-fold) increase of the emission intensity. Complex 6 acts as a guest in the crystalline matrix of 5 due to their structural similarity and affords solid solutions with bright luminescence at a doping content of 1–2%.
A similar strategy has been applied to photoemissive transition metal complexes by utilizing the ligands decorated with donor/acceptor functions (hydroxyl, carboxyl, amines/N-heterocycles etc.) capable of reversible interaction with protic acids and bases. The involvement of the metal and ligand orbitals into electronic transitions offers a selection of excited states (ligand or metal centered (LC/MC), intraligand (IL)/metal to ligand (ML)/ligand to metal (LM)/ligand to ligand (LL) charge transfers). Their energies, mixing, population, and deactivation are defined by the nature of the metal ion and acid–base reactivity. A diversity of possible scenarios can be illustrated by tetrazolate d6 complexes of Re(I), Ru(II) and Ir(III), which demonstrate hypsochromic shift/enhanced intensity (Re), bathochromic shift/change of the excited state (Ir), and quenching of the emission (Ru) upon protonation.10 Such characteristics allow the use of luminescent transition metal complexes as sensors for pH,11–17 acid–base vapors,18–20 and metal ions,21 receptors for anions,22,23 and photodynamic therapy agents.24
Interactions with acids and bases can influence the physical properties of metal complexes not only by electronic means of reactive functions tailored to the metal-coordinated ligands, but also through the modulation of non-covalent interactions, for instance hydrogen or metal⋯metal bonding. Interesting cases of pH-responsive supramolecular aggregates were described for square planar platinum(II) complexes. Their luminescence behavior strongly depends on the intermolecular arrangement, governed by Pt⋯Pt and π–π stacking interactions. These can be amended upon acid–base treatment of compounds containing ligands with hydrogen bond active sites.25–28 In a broader view, incorporation of H-bonding groups into complexes, which have a tendency for metallophilicity-driven assembly (i.e. primarily those of Pt(II), Au(I)), leads to the competition or interplay of weak forces and offers rich opportunities for the design of luminescent systems with dynamic or chromic behavior.29–36
Furthermore, a change in optical properties might arise from external perturbation of intramolecular ligand to metal coordination or reorganization of the ligand sphere. Flexible binding can be achieved for hybrid hemilabile ligands, i.e. those simultaneously possessing electronically different donor groups bound to the metal center with different strengths. This type of ligands showing variable coordination has found applications in catalysis and sensing.37–39 Notably, an adaptable ligand environment, which is regulated by acid–base interactions or hydrogen bonding and producing detectable photophysical changes, remains virtually unexplored among transition metal complexes.40,41 Nevertheless, a change in coordination mode of a loosely binding function upon interactions with protic and Lewis acids and particularly the related structural transformations are likely to have a substantial influence on the composition of frontier molecular orbitals, energies of electronic transitions, and the excited state properties.
In our previous results on phosphine–phosphine oxide derivatives, we have shown that the neutral P
O moiety interacts with coinage metals at a moderate strength (Cu(I) > Ag(I) > Au(I)),42 while the deprotonated secondary oxide motif (−P
O) of bis(2-(diphenylphosphaneyl)phenyl)phosphine oxide (HP3O) forms H-bonds with a clear impact on the photophysical characteristics of disilver(I) and digold(I) complexes [M2(P3O)2].43,44 In this work, we have selected a chelating phosphine comprising phosphinic acid as a concept of an adaptable ligand (Fig. 1), with an aim to investigate its coordination chemistry towards d10 coinage metal ions and the photophysical behavior of the corresponding compounds. This choice was dictated by the following reasons: (i) numerous phosphine complexes of Cu(I), Ag(I) and Au(I) show rich luminescence behavior;45–49 (ii) phosphinate/phosphonate (R2PO2−/RPO32−) groups are prone to protonation and hydrogen bonding50,51 and as hard O-donors are expected to have weaker affinity to d10 coinage metal ions in comparison to phosphines; (iii) the variable coordination number of coinage metals can adjust to the ligand environment;52 (iv) there have been only a few reports on mixed phosphine–phosphinic/phosphonic acids (or salts)53–55 and their coordination complexes (Fig. 1).56–59
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Fig. 1 Examples of (A) phosphine–phosphinic/phosphonic acid ligands;53–55 (B) chelating diphosphines with P O functions used in our works.42–44,60 | ||
We now demonstrate that using a novel diphosphine–phosphinate ligand, bis(2-(diphenylphosphaneyl)phenyl)phosphinic acid (P3OOH), allows for the preparation of structurally flexible silver(I) and gold(I) complexes, the molecular arrangement and photoluminescent behavior of which are affected by the anionic R2POO− part acting as a proton acceptor.
Simultaneously, we further studied the reactivity of compounds [M2(P3O)2] (M = Ag(I), Au(I))43,44 towards acids. Thus, a strong protic acid promotes a facile transformation of a phosphinite (phosphide–oxide) group −P(O)R2 into a phosphinate function R2POO−. On the other hand, [Au2(P3O)2] readily adds the Au(I) ion (Lewis acid), resulting in the expansion of the cluster framework that stabilizes the phosphide oxide motif −P
O and makes it sensitive to the protonation with a distinct optical response.
The reaction of silver(I) acetylide (AgC2Ph)n
62 with P3OOH under ambient conditions results in substitution of the hydrocarbon ligand and produces colorless neutral dimetallic complex [Ag2(P3OO)2] (1), which can be conveniently isolated as a methanol solvate. The use of silver triflate AgCF3SO3 instead of (AgC2Ph)n yields pale yellowish bis-protonated cationic derivative [Ag2(P3OOH)2](CF3SO3)2 (2, Scheme 1). Alternatively, 2 can be generated from 1 by adding a slight excess of triflic acid. In attempt to prepare the monoprotonated congener, a trimetallic cluster [Ag3(P3OO)3H](CF3SO3) (3) was identified as the only new product, which can be obtained by reacting the phosphine P3OOH with (AgC2Ph)n and AgCF3SO3 in 3
:
2
:
1 molar ratio.43 Analogous gold(I) compounds, however, are not formed in the reaction of the corresponding (AuC2Ph)n acetylide with P3OOH, which yields poorly soluble products probably having a polymeric nature.
The easy protonation of a coordinated phosphinate group POO− in 1 prompted us to probe the behavior of the congener phosphine–phosphide oxide complexes [M2(P3O)2], which are derived from the (o-Ph2PC6H4)2P(O)H (HP3O) ligand (M = Ag,43 Au44), under acidic conditions. We have shown previously that the [Ag2(P3O)2] adds an equimolar amount of HCl to give [Ag2(P3O)2H(μ-Cl)] as a result of hydrohalogenation.43 The digold relative [Au2(P3O)2] reacts with two equivalents of HCl yielding yellow-orange doubly protonated species [Au2(HP3O)]Cl2 (4), which also can be obtained from the HP3O phosphine and [Au(tht)Cl] (tht = tetrahydrothiophene) in 82% yield, Scheme 2 and the SI. Interestingly, applying stronger triflic acid in aerated solution quickly oxidizes the phosphide-oxide groups to the phosphinates, converting [M2(P3O)2] into the aforementioned bis-protonated complex 2 and monoprotonated [Au2(P3OO)2H]CF3SO3 (5) for M = Ag and Au, respectively (Scheme 2). This transformation of the metal-bound phosphine, i.e. HP3O + ½O2 → P3OOH, occurs if HP3O is reacted with silver triflate, or when the chloride is replaced by the triflate in 4 in an aerated solution. Both pathways leading to complexes 2 and 5 (Scheme 2) can be considered as the protonation of the oxygen atom in the M–PR2
O fragment (λ5σ4-P configuration) by a strong acid that likely increases the contribution of the resonance form M+–PR2–OH (λ4σ4-P) having phosphinous acid ligand. This, in turn, enhances the nucleophilicity of the central phosphorus atom and makes it more reactive towards molecular oxygen.
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| Scheme 2 Preparation of phosphinate complexes 2 and 5via acid-mediated oxidation of the −P3O phosphine–phosphide oxide ligand. | ||
A more efficient synthesis of colorless complex 5 involves the reaction of P3OOH ligand with [Au(tht)Cl] and subsequent removal of the chloride with AgCF3SO3 (Scheme 3).
Notably, an acid-mediated oxidation of [Au2(P3O)2] produces 5 as a yellowish crystalline material 5*, which contains 5 as a main component accompanied by a very minor (ca. 1–2%) but systematically reproduced admixture of a trigold cluster [Au3(P3O)2]CF3SO3 (6), see the discussions of the X-ray data and solid-state photophysical properties below. The ability of the digold complex to accept an additional metal ion likely stems from coordinative saturation of one of the gold centers being in a pseudotetrahedral environment of four P-donors.
Curiously, the trigold species 6 initially evaded detection: none of the conventional characterization techniques (XRD, NMR and mass-spectrometry, elemental analysis) gave a clear indication of its presence. It was only when two separate reactions leading to 5* and 5 (Schemes 2 and 3) yielded crystals of distinctly different colors and luminescence behavior that required an explanation. This anomaly was not resolved by repeated crystallizations, but column chromatography performed on 5* (silica gel, dichloromethane–methanol, 95
:
5 v/v) led to a substantial enrichment of the mixture with elusive trigold complex 6, increasing its content to nearly 30% (vide infra).
Yellow-greenish cluster 6 is readily obtained in 77% yield from [Au2(P3O)2] and labile species [Au(tht)n]CF3SO3 generated in situ (Scheme 3 and the SI). In contrast to the parent [Au2(P3O)2] compound, complex 6 is stable in the presence of a strong acid, showing no visible signs of oxidation of the phosphide oxide moiety.
No silver analogue of 6 was formed in the reaction of [Ag2(P3O)2] with silver triflate, which proceeds non-stoichiometrically, giving a mixture of products.
Structurally different modifications, 1(X/H2O) (X stands for unresolved disordered solvent) and solvent-free 1, were obtained from dichloromethane/diethyl ether mixture (Fig. 2 and S2). The latter species requires the use of dry solvents and is difficult to reproduce in a phase-pure form. In both 1(X/H2O) and 1, the phosphinate anion bridges the metal centers in a μ2:O1,O2 fashion, utilizing two oxygen atoms, resulting in an 8-membered metallacycle with chair-like conformation. The silver ions exhibit a heavily distorted tetrahedral coordination geometry, similar to that in 1(MeOH), including the Ag–O and Ag–P bond lengths (Table S4 and S5). 1(X/H2O) contains a fraction of water molecule (ca. 0.3) bound to each metal that induces a disorder of the {C6H4–POO−} fragment and affects the Ag–O connectivity (Fig. S2).
All three forms 1, 1(MeOH) and 1(X/H2O) crystallize in the same type of space group (P
) with unit cells of comparable size (Table S1), which points to a possibility of accessible phase transitions. Thus, drying pristine methanol solvate 1(MeOH) under ambient conditions leads to rapid loss of ca. 50% of crystallization solvent (4 out of 8 molecules found in the unit cell according to elemental analysis), apparently which is not involved in hydrogen bonding and occupies the space voids around the molecules of the complex (Fig. S3). This transition gives intermediate phase 1′(MeOH) with distinct photophysical properties (see discussion below). Further vacuum drying at 473 K transforms 1′(MeOH) into solvent-free material 1 as confirmed by powder X-ray diffraction patterns (Fig. S4). Semi-solvated compound 1′(MeOH) can be restored by exposing powder sample 1 to methanol vapors.
The molecular configuration of doubly protonated 2 resembles that of 1(MeOH) and features a nearly flat {Ag2O2} fragment possessing tetracoordinate silver ions (Fig. 3, Table S6). The short separations between the oxygen atoms of the phosphinate and triflate anions (d(O⋯O) = 2.565(7) Å) evidence for efficient PO–H⋯OS interactions engaging the acidic residues. Comparable geometry and structural parameters of the {Ag2O2} core in 2 and 1(MeOH) manifest that protonation of the phosphinate groups and POO⋯H–OMe hydrogen bonding have a similar effect on the coordination mode of the R2POO groups, both causing the formation of four-membered metallocycles.
Monocationic complex 3 is constructed of three nonequivalent phosphine ligands and three silver ions, all found in different four-coordination environments {AgPxO4−x}, x = 1–3, Fig. 3. The assembly of 3 is evidently driven by favorable hydrogen bonding O(4)⋯H⋯O(6) (d(O⋯O) = 2.445(7) Å, Table S7) between two phosphinate groups due to partial protonation. Variable coordination of silver ions and dynamic metal–P/O interactions are other necessary factors, which allow redistribution of the ligand sphere occurring upon formation of 3.
In a CD2Cl2 solution, the 31P{1H} spectrum of 1 at 293 K displays two broad resonances (Fig. S4), which indicate substantial structural non-rigidity at room temperature. The unresolved singlet at 26.2 ppm is assigned to acidic phosphorus atom, the high field signal of twice larger integral intensity can be interpreted as two doublets (5.0 and 3.7 ppm, 1JPAgca. 230 Hz). This pattern arises from nonequivalent phosphine motifs in the absence of significant phosphorus–phosphorus coupling that might occur due to intramolecular dynamics and/or dissociation of a dimeric structure into mononuclear fragments. Addition of methanol to a dichloromethane solution of 1 visibly sharpens the signals and slightly shifts them to low field region that is tentatively attributed to the formation of hydrogen bonding with protic solvent (Fig. S5).
The protonated derivative 2 undergoes dissociation in a CD2Cl2/MeOD-d3 mixture under ambient conditions and has to be stabilized by adding some triflic acid (Fig. S5). The set of sharp signals consisting of a singlet at 43.4 ppm (POOH) and doublets at 14.3 ppm (–PPh2; two isotopomers 1JPAg = 339 and 392 Hz for 107Ag and 109Ag) can be assigned to a symmetrical mononuclear species [Ag(P3OOH)]+. The broad dominating resonances form the pattern, similar to that of complex 1 but shifted to a low field region that presumably corresponds to binuclear compound being in dynamic equilibrium with triflic acid. The ESI+ mass spectrum of 2 displays the main signal of [Ag(P3OOH)]+ ion (Fig. S6) that confirms easy fragmentation of the dimeric structure.
Cluster 3 is rigid in solution in the NMR timescale at ambient conditions. Its phosphorus spectrum exhibits three narrow resonances of equal intensities in the range 31.5–28.8 ppm (Fig. S5), which belong to three different POO− groups found in crystallographically characterized molecule. The multiplets spanning from 6.1 to −5.7 ppm originate from six different –PPh2 fragments connected to three silver atoms that gives a complicated spin system producing multiple P–107,109Ag and P–P couplings. The presence of the molecular ion of 3 in solution is corroborated by the dominating signal of a doubly charged cation at m/z = 1060.0 corresponding to the adduct [3 + K]2+ (Fig. S6).
The structure of the intermediate gold complex 4 (Fig. 4 and Table S8) implies the protonation of the phosphide oxide groups, which seemingly form the O–H⋯Cl− hydrogen bonds with chloride anions (d(O⋯Cl) = 2.880(9)–2.926(7) Å). Both P(OH) functions of phosphine ligands in 4 are bound to the same gold center. Contrarily, the phosphines in the non-protonated parent compound [Au2(P3O)2] have a head-to-tail orientation.44 The gold atoms in 4 are found in two- and four-coordination environments completed by the P-donor groups. These are supplemented by a short Au–Au contact (2.8615(6) and 2.8226(6) Å for two independent molecules), despite high coordination number of one of the metal ions. Complex 4 represents one of a few cases of effective aurophilic interactions with the participation of a four-coordinated Au(I) center.44,69,70 The P–O bonds in 4 (1.593(8)–1.597(8) Å) are visibly elongated in comparison to those in [Ag(P3O)] (1.5170(4) and 1.5180(4) Å) that testifies in favor of the Au+–PR2–OH configuration.
The metal centers in the digold phosphinate complex 5 adopt close to linear two-coordinate geometry furnished by the P atoms of phosphine functions (Fig. 4 and Table S9), the P–Au–P motifs being nearly orthogonal to each other. Hard phosphinate donors do not participate in binding to gold(I) ions, the shortest Au⋯O distances are 2.935 and 2.771 Å (acetonitrile solvate) might suggest only weak interactions slightly distorting the P–Au–P angles (172.48(3) and 176.32(3)°). Instead, the O(1) and O(3) atoms (d(O⋯O) = 2.396(4) Å) trap the proton to form the O⋯H⋯O motif, which occupies the space between the gold centers and is sterically protected by phenyl rings.
Cluster 6 possesses a bent trigold core (∠Au(2)–Au(1)–Au(3) = 142.205(17)/144.772(8)° for diethyl ether/acetonitrile solvates) with short interatomic distances between 2.8414(5) and 2.8695(2) Å (Table S10), which are significantly below the sum of van der Waals radii (3.32 Å). Each of the lateral metal ions is decorated with two phosphine groups forming the ∠P–Au–P angle close to 170° (171.34(8)–173.23(8)°), while the central gold atom is connected to phosphide oxide anionic donors with a larger deviation from linearity (∠P(1)–Au(1)–P(4) = 168.47(8)/167.69(4)°).
As was mentioned above, cluster 6 readily co-crystallizes with complex 5. Despite pure 5 and 6 being found in different space groups (monoclinic P21/c and orthorhombic Pbca, respectively, Table S1), the similarity of structural motifs makes these cations fungible in a crystalline matrix. The formation of a solid solution of 6 in 5 was confirmed for their mixture, obtained in the course of chromatographic separation, the structure of which was satisfactorily refined as a composite containing two components with 33.3% and 66.7% occupancies (Fig. S7).
Yellowish crystals of 5*, i.e.5 containing a small additive of 6, was characterized in acetonitrile and acetone solvated forms, which are crystallographically indistinguishable from those of pure colorless 5 synthesized according to Scheme 3 (Tables S1 and S9). The powder XRD analysis also proves the crystallographic identity of bulk phases of 5 and 5* obtained via two different pathways (Fig. S8), pointing to a low content of 6 embedded in the matrix of 5 (1–2% according to the NMR data, Fig. 5 and S10). Such a reproducible co-crystallization with a resolved composition of low-abundant species is rarely encountered in coordination chemistry. It reminds of the co-crystallization of dopants in organic hosts that induces room temperature phosphorescence and could lead to misinterpretation of the photophysical properties.71,72
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| Fig. 5 162 MHz 31P{1H} NMR spectra of complex 5* before (top, showing a minor admixture of 6) and after (bottom) addition of triflic acid (acetonitrile-d3, 233 K). | ||
In solution at room temperature, a low field signal at 18.2 ppm in the 1H NMR spectrum of 5 (Fig. S9) matches the reported data for hydrogen-bonded homoconjugated phosphinate ions {R2POO⋯H⋯OOPR2}−
73 and is consistent with this structural assignment. The phosphorus NMR spectrum of 5 shows two signals of 1
:
2 intensities ratio, assigned to POO− (22.9 ppm) and –PPh2 groups (45.7 ppm), Fig. S10. This profile purports intramolecular motion, resulting in symmetrization of the digold-diphosphine core. Below 240 K, the broad low-field singlet splits into the AB spin system P–Au–P′ (2JPP = 365 Hz). The addition of an excess of triflic acid to an acetonitrile solution of 5 shifts the POO− resonance to 38.7 ppm (3JPP = 5.5 Hz at 233 K, Fig. 5) that confirms the protonation of both phosphinates. Simultaneously, it decreases the coupling within the AB system and enhances the rigidity of the complex, that is corroborated by variable temperature spectra (Fig. S10).
The ESI+ mass spectra of 5 and 5 + H+ display the signals of singly and doubly charged molecular cations at m/z = 1565.2 and 783.1 (Fig. S6), indicating that these species exist in dynamic equilibrium and that the dimetallic structure is retained in acidic medium. However, crystallization of 5 even in the presence of CF3SO3H yields only the monoprotonated form shown in Fig. 4.
The well-resolved 31P{1H} NMR spectrum of 6 at ambient temperature and the ESI+-MS showing the peak of molecular ion at m/z = 1729.3 (Fig. S6) approve high structural rigidity and stability of this compound. The NMR pattern can be adequately simulated as an X2AA′BB′ spin system (Fig. 6). Adding the triflic acid (3 eq.) shifts the resonance assigned to the phosphide oxide groups (δ = 82.6 ppm) to the low field region (δ = 100.4 ppm). This observation suggests the formation of phosphinous acid functions P(OH) in 6 + H+ analogously to those in the protonated complex 4 bearing the same −P3O ligand, which demonstrates a broad resonance of the P(OH) groups at δ around 101 ppm (Fig. S5). The mass spectrum of 6 in the presence of CF3COOH shows a minor signal of dicationic species at m/z 865.1, which corresponds to the monoprotonated [6 + H+]2+ cluster. The loss of large coupling JAB = 324 Hz in the form 6 + H+ might arise from structural reorganization that nearly equivalizes phosphorus nuclei in the positions A (A′) and B′ (B).
Compounds 4 and 6 with aurophilic interactions extend absorption tails to longer wavelengths above 450 nm. In particular, trigold cluster 6 demonstrates a strong band peaking at 384 nm, which matches the predicted lowest energy singlet–singlet transition S0 → S1 (λ = 388.7 nm, f = 0.5088, Table S14).
The S1 state primarily involves the metal core, i.e. the cluster-centered (CC) configuration, supplemented with some metal-to-metal-to-ligand charge transfer, MMLCT. In addition, a weaker band is found around 440 nm (εmax = 2.6 × 103 M−1 cm−1) that can be assigned to direct S0 → T1 absorption (calculated λ = 444.7 nm, Table S14 and Fig. S11) due to strong spin–orbit coupling mediated by the three gold atoms. Protonation of 6 slightly red shifts the prominent band from 384 to 390 nm (Fig. 8 and Table S15).
Among the titled complexes 1–6, only cluster 6 shows detectable photoemission in solution. In dichloromethane, 6 exhibits weak blue-green luminescence with a broad band maximized at λem = 500 nm (Fig. 8 and Table S15), the low quantum yield of which Φem ∼ 0.004 did not allow for accurate determination of the excited state lifetime. Remarkably, in the presence of excess CF3SO3H, the emission of 6 + H+ is only slightly bathochromically shifted (λem = 512 nm), but Φem is drastically enhanced (>170-fold), reaching 0.71 under oxygen-free conditions. The observed lifetime of τ = 4.0 μs and associated radiative decay rate kr = 1.77 × 105 s−1 indicate that triplet excited states are involved either via phosphorescence or thermally delayed activated fluorescence (TADF). The predicted electronic configuration of the T1 state of 6 resembles that of the S1 (Fig. S12) and has the 3CC character of the 3[5dσ*6pσ1] type, which has been recognized as an origin of phosphorescence among di- and trinuclear gold-phosphine compounds with metal–metal bonds.74–77 While linear chain Au3 compounds can be intensely emissive in solution,75,77 the very weak luminescence of 6 might arise from vibrational degrees of freedom of the bent trigold core.
The increase of the intensity induced by the protonation of the −PO motifs (cf. NMR results vide supra) can be ascribed to the structural and electronic changes related to the −PO → POH transformation, which seem to primarily suppress nonradiative relaxation that is also suggested by comparable kr values for non-protonated 6 in crystals (see the Discussion below). Nevertheless, some acceleration of the radiative rate cannot be ruled out as evidenced by the solid-state characteristics.
| λ em, nm | Φ em |
τ
av
a, μs |
k
r × 104 b, s−1 |
k
nr × 104 c, s−1 |
λ em, nm | Φ em |
τ
av
a, ms |
k
r
× 102 b, s−1 |
k
nr × 102 c, s−1 |
|
|---|---|---|---|---|---|---|---|---|---|---|
| 297 K | 77 K | |||||||||
| a Amplitude-weighted average emission lifetime determined by the equation τav = ∑Aiτi, Ai = weight of the i-th component. b k r = Φem/τav. c k nr = (1 − Φem)/τav. | ||||||||||
| P 3 OO H | 490 | 0.06 | 1.5 ns | 4370 | 63 900 |
547 | 0.59 | 12.57 | 0.47 | 0.33 |
| 1′(MeOH) | 510 | 0.69 | 19.16 | 3.61 | 1.61 | 511 | 0.99 | 1.58 | 6.25 | 0.06 |
| 1 | 555 | 0.06 | 1.15 | 4.87 | 82.1 | 508 | — | 0.49 | — | — |
| 2 | 514 | 0.44 | 28.61 | 1.54 | 1.96 | 529 | 0.56 | 2.25 | 2.49 | 1.96 |
| 3 | 521 | 0.32 | 6.16 | 5.26 | 11.0 | 522 | 0.74 | 1.28 | 5.78 | 2.04 |
| 6 | 488 | 0.76 | 2.53 | 30.0 | 9.49 | 483 | — | 3.21 μs | — | — |
| 5* (5 + ∼2% 6) | 498 | 0.32 | 2.82 | 11.3 | 24.1 | 498 | 0.58 | 4.61 μs | 1250 | 919 |
Crystalline solvent-free 1 is a weak yellow luminophore (λem = 555 nm, Φem = 0.06). The low quantum yield of this material is caused by a high non-radiative rate (knr = 8.21 × 105 s−1), which is nearly 17 times faster than the radiative process (kr = 4.87 × 104 s−1). The neat methanol solvate 1(MeOH), which contains 8 crystallization solvent molecules, is non-emissive, while intense green luminescence (λem = 510 nm, Φem = 0.69; Fig. 9) was observed for partially solvated 1′(MeOH) (vide supra) that is readily obtained by drying 1(MeOH) at room temperature. Intermolecular rearrangement, which occurs upon the removal of the least H-bound crystallization solvent, corresponds to the transition to another crystalline phase as evidenced by the PXRD data (Fig. S4). The elimination of the solvent-free void space likely leads to denser packing, inhibiting non-radiative relaxation, which evidently dominates for 1(MeOH). A drastic increase of the quantum efficiency for 1′(MeOH) vs.1, having comparable kr values, is a manifestation of ca. 50-fold decelerated non-radiative rate for the former solvate (knr = 1.61 × 104 s−1). This physical behavior can be tentatively explained in terms of intramolecular structural alterations within di-(silver–phosphinate) moiety. 1′(MeOH) presumably adopts compact and therefore stiff {Ag2O2} core analogously to that in 1(MeOH), which constrains excited state geometry changes and non-radiative pathways.
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| Fig. 9 Normalized excitation (dashed lines) and emission (solid lines) spectra of complexes 1–3, 6 and 5* (5 doped with ca. 2% of 6) in the solid state at 297 K. | ||
While the emission onsets for 1′(MeOH) and 1 are nearly the same (Fig. 9), more severely shifted emission maximum and offset for 1 argue for pronounced structural reorganization occurring in the excited state. This feature likely reflects higher flexibility of the {Ag2(OPO)2} metallacyle in 1vs. {Ag2O2} in 1′(MeOH), which also permits more efficient non-radiative relaxation. The influence of intermolecular interactions also cannot be ruled out. The packing of 1 reveals non-negligible contacts between silver atoms and adjacent phenyl rings (Fig. S3), which can coordinate to the metals in the excited state and contribute to geometry distortions being detrimental for luminescence. A similar reason can be tentatively applied to non-emissive 1(MeOH), which contains methanol molecules forming weak Ag⋯O contacts (3.311(3) Å, Fig. S3) and offering excessive coordination environment with additional degrees of freedom.
The photophysical characteristics of the protonated dicationic complex 2 are close to those of 1′(MeOH). Accordingly, 2 shows green moderately intense emission (λem = 514 nm, Φem = 0.44) with a somewhat longer lifetime of 28.6 μs cf. 19.61 μs for 1′(MeOH). The similar effects of protonation and hydrogen bonding on the luminescence of 1 thus primarily correlate with the structural changes of the silver-phosphinate core and its impact on the magnitude of knr, whereas the energies and localization of the electronic transitions along with the rates of ISC/radiative decay are only slightly sensitive to the degree of perturbation of the POO− groups. It is worth mentioning that packing arrangement of 2 (Fig. S3) shields the central {Ag2O2} core from intermolecular interactions, in contrast to the weakly and non-emissive congeners 1 and 1(MeOH).
Trinuclear compound 3 luminesces at a longer wavelength (λem = 521 nm) and attains the fastest radiative decay among silver complexes 1–3. However, its quantum yield of 0.32 stems from enhanced radiationless deactivation compared to dimetallic congeners 1′(MeOH) and 2 probably due to a larger and less rigid molecular emitting core, favoring additional vibrational modes to quench the emission.
Cooling to 77 K does not change structureless emission profiles of 1–3 and induces a slight red shift of the band maxima except for solvent-free 1 (Fig. S17, Table 1). In parallel, the observed lifetimes for 1′(MeOH), 2 and 3 are found between 1.3 and 2.2 ms, which correspond to kr ranging from 2.49 to 6.25 × 102 s−1. Such a decrease in rate constants of several orders of magnitude argues for a temperature-dependent change of the nature of the excited state and for a different emission mechanism at low temperatures, which is typically found for TADF with a Boltzmann equilibrium between, e.g., 1/3MLCT states. Considering relatively high quantum yields and their moderate growth under cryogenic conditions, which cannot account for the orders of magnitude change of radiative rates, monitoring of the observed lifetimes for 1′(MeOH), 2 and 3 in the range 297–77 K was carried out in the first approximation. The obtained S-shaped temperature dependences of τav are typical of TADF materials and were satisfactorily fitted using a two-state model (Fig. S18 and eqn S1). Thus, 1–3 likely realize this kind of emission process.80 Indeed, our TD-DFT calculations of complex 1 and the dication 22+ indicate energy gaps ΔES1T1 at the ground state geometry of 144 and 210 meV, respectively, and 190 meV for 1 at the T1 geometry (Tables S11 and S12). These energy barriers correlate well with the experiment and appear to be small enough to be overcome at room temperature and bypass the spin-forbidden phosphorescence from the T1 state, albeit resulting in relatively small kr of the order of 104 s−1 in comparison to many other efficient d10 coinage metal TADF emitters exhibiting smaller ΔES1T1 and, consequently, higher values for kr of up to 106 s−1.81–83
While colorless phosphinate digold complex 5 synthesized according to Scheme 3 is not luminescent at room temperature, the phosphide oxide relative [Au2(P3O)2]44 and its trinuclear derivative 6 are intensely emissive in the solid state. Sky-blue luminescence of trigold cluster 6 (λem = 488 nm, Φem = 0.76) occurs at substantially higher energy than that of a yellow luminophore [Au2(P3O)2] (λem = 585 nm, Φem = 0.34). In contrast to broad emission profiles of [Au2(P3O)2] and 1–3, 6 unveils a considerably narrower band (FWHM = 34 nm, 1412 cm−1 at 297 K, Fig. 9). The narrowband luminescence has been previously encountered for a few homo-74,75,77,84 and heterometallic85,86 gold complexes but remains rather uncommon for transition metal emitters, particularly of a multinuclear nature. The observed average lifetime for 6 exhibit a linear increase in the temperature range 297–77 K from 2.53 to 3.21 μs (Fig. S19, Table 1). Assuming that at 77 K the emission quantum yield approaches unity, kr values are almost identical at 297 and 77 K (3.0 and 3.1 × 105 s−1, respectively). This does not agree with the typical TADF behavior but rather suggests phosphorescence as the dominant process both at room and low temperatures. The behavior of 6 correlates with that of chain Au3 clusters stabilized by tridentate phosphine75,76 and phosphino-carbene ligands,77 which luminesce in a blue region with quantum yields up to 0.8 and kr reaching 3.0 × 105 s−1 in the solid state.
According to theoretical studies, the ΔES1T1 at the ground state geometry of the cation 6+ of 401 meV is too high to allow for TADF (Table S14). As the lowest energy triplet state T1 is dominated by cluster-centered transitions, it is reasonable to assume that the strong SOC is mediated cooperatively by the three Au atoms and gives rise to the high phosphorescence rate constants, whereas rigid crystalline matrix diminishes nonradiative relaxation.
Unlike non-emissive pure 5, pale-yellow crystals of 5* (prepared as in Scheme 2) are appreciably photoluminescent. The crystallographic identity of bulk materials 5 and 5* suggests that a minor dopant admixture is responsible for luminescence. Indeed, the crystallization of colorless 5 in the presence of 2% of 6 produces a uniform pale-yellow material with blue-greenish luminescence. This photophysical behavior is retained after several cycles of dissolving-crystallization. The emission of 6 embedded in crystals of 5 (λem = 498 nm, Table 1 and Fig. 9) is bathochromically shifted with respect to neat 6 (λem = 488 nm) and resembles that in solution (λem = 500 nm, Table S15). A dramatic enhancement of the quantum yield in the solid vs. liquid medium (Φem = 0.32 and 0.004, respectively) is associated with minimizing radiativeless deactivations of the excited state. On the other hand, a nearly 3-fold decrease of the radiative rate for 6 in 5vs. neat 6 (kr = 1.1 × 105 and 3.0 × 105 s−1, respectively) suggests non-negligible roles of intermolecular interactions and intramolecular geometry alterations (e.g. the angle and distances within the Au3 core) imposed by different matrices in affecting the SOC and the probabilities of spin-forbidden transitions.
We have also investigated the behavior of congener disilver(I) and digold(I) complexes comprising phosphine–phosphide oxide ligand −P3O towards acids, which are capable of promoting oxidation of the coordinated −P
O group to the phosphinic acid to generate compounds 2 and 5 from [M2(P3O)2] precursors. Notably, it was shown that the synthesis of 5via acid-mediated protocol affords a minor co-product, a trigold complex 6, which co-crystallizes very efficiently with 5 due to their structural similarity to form a solid solution of 6 in 5 (5*) with bright luminescence even at low doping concentrations of 1–2%. Compound 6 can be selectively derived from [Au2(P3O)2] in a reaction of cluster expansion. The phosphide oxide function in 6 is stabilized by the additional gold center towards the oxidation and endures protonation with a dramatic enhancement of the intensity of the phosphorescence in solution. In the solid state, cluster 6 is the brightest emitter among studied complexes with the quantum yield of 0.76.
The difficulty in evaluating a minor admixture underscores surprising formal interchangeability O⋯H⋯O ↔ Au that occurs within these ligand environments and simultaneously illustrates new possibilities for the design of new light emitting molecular materials of coinage metal complexes.
Supplementary information (SI): experimental procedures and computational studies. See DOI: https://doi.org/10.1039/d5qi01622c.
CCDC 2475264–2475275 (1–6 and P3OOH) contain the supplementary crystallographic data for this paper.87a–l
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