Open Access Article
Jannis Fidelius†
a,
Clemens Taube†a,
Kai Schwedtmann
a,
Felix Hennersdorf
a,
Rosa M. Gomila
c,
Antonio Frontera
c,
Robert Wolf
*b and
Jan J. Weigand
*a
aFaculty of Chemistry and Food Chemistry, Technische Universität Dresden, 01062 Dresden, Germany. E-mail: jan.weigand@tu-dresden.de
bInstitute of Inorganic Chemistry, Universität Regensburg, 93040 Regensburg, Germany
cDepartment of Chemistry, Universitat de Illes Balears, 07122 Palma de Mallorca, Spain
First published on 28th May 2026
Monocationic imidazoliumyl-substituted phosphanes, LCP(R)Cl+ (LC = 1,3-diisopropyl-4,5-dimethylimidazol-2-yl), were synthesized as their respective triflate salts 2a–c[OTf] (a: R = Cy; b: R = Ph; c: R = Py). These serve as versatile building blocks for the formation of the corresponding imidazoliumyl-substituted diphosphanes ((LCPR)2 5a–c[OTf]2) and iso-tetraphosphanes ((LCPR)3P[OTf]3 6a,b[OTf]3). The introduction of a cationic (onio) substituent substantially alters the preferred reaction pathways of the P-scaffolds compared to their neutral congeners and electronically predisposes selected P–P bonds toward fragmentation. DFT calculations reveal a strong localization of the LUMO orbitals on the P–P bond, indicating susceptibility to nucleophilic attack. Both 5a,b[OTf]2 and 6a[OTf]3 undergo metal-mediated fragmentation reactions. Reactions of 5a,b[OTf]2 with Pd(PPh3)4 afford two distinct dinuclear complexes, while reactions of 6a[OTf]3 with metal chlorides yield triphosphanide complexes (LCPCy)2PM[OTf]2 9[OTf]2: M = Pd(allyl), 10[OTf]2: M = Au(PPh3), accompanied by the formation of 2a[OTf]. Treatment of 6a[OTf]3 with the NHC IPr (1,3-diisopropyl-4,5-dimethylimidazol-2-ylidene) provides the free triphosphanide ligand (LCPCy)2P[OTf] (11[OTf]).
As a result, there is a notable lack of detailed studies on the reactivity of these systems towards transition metals. To the best of our knowledge, only one iron carbonyl complex has been structurally characterized (Fig. 1-III).11
Beyond neutral oligophosphanes, the coordination chemistry of phosphorus-centered cations has garnered considerable interest over the last decade.12 Recently, we reported the synthesis of various cationic polyphosphanes that exhibit metal-dependent coordination and insertion reactions.13,14 Key to the formation of stable cationic oligophosphanes is the introduction of imidazoliumyl substituents, which enables precise electronic tuning of the attached phosphorus atoms,2,15 allowing for the stabilization of a wide range of phosphorus bonding motifs.16,17 Our access to imidazoliumyl-substituted chlorophosphane salts of the type LCP(R)Cl[OTf]17 motivated us to explore their potential in constructing imidazoliumyl-substituted oligophosphanes. Building on this platform, we now report the synthesis of cationic diphosphanes and iso-tetraphosphanes via controlled coupling of LCP(R)Cl+ precursors. Using these chlorophosphanes as a starting point, we highlight in this contribution the generation of the symmetric diphosphanes ((LCPR)2[OTf]2, Fig. 1-IV) and iso-tetraphosphanes ((LCPR)3P[OTf]3, Fig. 1-V). Notably, this is the first report of a successful synthesis of branched oligophosphanes featuring cationic substituents. These substituents substantially alter the preferred reaction pathways of these phosphanes and electronically predispose selected P–P bonds toward fragmentation, leading to distinct products upon reaction with transition metal compounds or nucleophiles. In contrast to literature reports on di- and iso-tetraphosphanes, the synthesized compounds do not exhibit classical coordination to transition metals via the free electron pairs on the phosphorus atoms (cf. Fig. 1-I and III), but rather engage in selective P–P bond cleavage reactions.
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| Scheme 1 Synthesis of imidazoliumyl-substituted chlorophosphanes 2a–c[OTf] and the molecular structure of 2b[OTf]·C6H5F (hydrogen atoms, solvate molecule, and anion are omitted for clarity, and ellipsoids are displayed at 50% probability). Selected bond lengths [Å] and angles [°]: C1–P1 1.827(3), P1–C2 1.822(2), P1–Cl1 2.0638(8), C1–P1–C2 100.78(9), C1–P1–Cl1 98.86(7), C2–P1 Cl1 102.83(7). (i) 2a[OTf] (R = Cy): C6H5F, 70 °C, 3 d, 74%; 2b[OTf] (R = Ph): C6H5F, 90 °C, 16 h, 74%; 2c[OTf] (R = Py): C6H5F, 70 °C, 3 h, 99% (ref. 18). | ||
The 31P{1H} NMR spectra of 2a–c[OTf] each show a single, broad resonance (2a[OTf]: δ(P) = 55.6 ppm; 2b[OTf]: δ(P) = 48.8 ppm; 2c[OTf]: δ(P) = 24.0 ppm), which are significantly upfield-shifted compared to 3a–c. The resonance of 2c[OTf] is downfield-shifted compared to 2b[OTf] due to the mesomeric effect of the pyridyl substituent. Upon cooling to 250 K, the resonances of 2a–c[OTf] each resolve into two singlet resonances. This is attributed to the presence of two rotamers, which originate from hindered rotation of the iPr-groups at the imidazoliumyl substituent. This assumption is supported by the observation of a splitting of the resonances of the iPr-groups in the 1H-NMR spectra at low temperatures and by a disordered iPr-group in the molecular structure of 2b[OTf] (see SI, Section 2.1.2).
To better understand this behaviour, a conformer search for 2b+ was conducted using the Conformer-Rotamer Ensemble Sampling Tool (CREST; see Fig. 2).19 After geometry optimization (BP86-D4/def2-TZVP), two isoenergetic isomers were identified. The calculated rotational barrier in CH2Cl2 was 10.4 kcal mol−1, which agrees well with the NMR-derived barrier (12.3 kcal mol−1) at the coalescence temperature. The calculated chemical shift difference Δδ(P) is 3.0 ppm, which is also consistent with the experimental data (Δδ(Pexp) = 3.1 ppm).
Both computationally disclosed conformers were also observed in the molecular structure of 2b+ in the form of a disordered isopropyl group (see Scheme 1 and Fig. S6). As expected, the molecular structures (2a,c[OTf]: see SI) show the pyramidal bonding environment at the phosphorus atom, with typical P–Cl bond lengths ranging from 2.064(8) Å to 2.0770(13) Å, and P–C bonds which are comparable to those in known imidazoliumyl-substituted phosphanes.17
With larger quantities of 2a–c[OTf] in hand, we explored the reduction reactions using 1,4-bis(trimethylsilyl)-1,4-dihydropyrazine (4), a reagent previously shown to be effective for reductive P–P bond formation.14,20 The 2:1 reaction of 2a–c[OTf] in C6H5F produced colourless or yellow precipitates over 16 h. After filtration and subsequent drying under vacuum, diphosphane salts 5a–c[OTf]2 were isolated in good yields (5a[OTf]2: 63%; 5b[OTf]2: 78%; 5c[OTf]2: 87%; Scheme 2).
At ambient temperature, the 31P{1H}-NMR spectra show a single broad resonance in each case (5a[OTf]2: δ(P) = −50.0 to −38.4 ppm; 5b[OTf]: δ(P) = −47.9 ppm; 5c[OTf]: δ(P) = −43.0 ppm). The signals are upfield-shifted compared to related neutral diphosphanes (e.g. Cy2P–PCy2: δ(P) = −21.0 ppm; Ph2P–PPh2: δ(P) = −14.6 ppm).21 Upon cooling to 250 K, the broad resonances resolve into singlet resonances (5b[OTf]2: δ(P) = −57.1 ppm, δ(P) = −50.5 ppm, δ(P) = −41.0 ppm) and an AB spin system (5b[OTf]2: δ(PA) = −46.4 ppm δ(PB) = −43.3 ppm, 1J(PP) = −146 Hz; Fig. 3e). This is attributed to the presence of three conformers, arising from hindered rotation around the N–C bond of the iPr groups.
A conformational analysis using CREST was performed on compound 5b2+. The analysis identified three isomers with comparable energies. Fig. 3a–c presents the optimized geometries and relative energies, alongside the predicted 31P{1H}-NMR spectra for these isomers. Two of the isomers are centrosymmetric, leading to an anticipated singlet resonance in the 31P{1H}-NMR spectrum (labelled as 5b2+(b) and 5b2+(c); in Fig. 3b and c). The third isomer, denoted as 5b2+(a), lacks symmetry and is expected to display an AB spin system in 31P{1H}-NMR (Fig. 3d and e). These three isomers arise from rotation of the iPr groups marked in yellow in Fig. 3a–c. In contrast, the rotation of the green-marked groups leads to significantly higher-energy rotamers, resulting in diminished population. The predicted 31P{1H}-NMR spectrum for this isomer mixture is shown in Fig. 3d. The calculated spectrum aligns with the experimental spectra. The close match of the expected coupling constant for 5b2+(a; −144 Hz) and the experimental value (−146 Hz) strongly supports the presence of this non-symmetric rotamer in solution. The molecular structure of 5c[OTf]2 evidenced disordered isopropyl groups, confirming the presence of the computationally predicted conformers (see Fig. S24). The crystal structures of 5a–c[OTf]2 show an anti-conformation along the P–P bond (5b[OTf]2: Fig. 4; 5a,c[OTf]2: see SI, Sections 2.2.1 and 2.2.3). The P–P bond lengths range from 2.2315(17) Å to 2.2581(7) Å, in line with P–P single bonds in neutral diphosphanes (Cy2P–PCy2 2.21 Å; Ph2P–PPh2 2.22 Å).21,22
Aiming at the construction of larger oligophosphorus scaffolds, we treated the chlorophosphanes 2a–c[OTf] with an excess of P(SiMe3)3 in C6H5F. The reaction leads to the formation of colourless precipitates over the course of 1 to 3 days, which, after filtration, could be identified as the desired tricationic iso-tetraphosphane salts 6a,b[OTf]3 (see Scheme 2). 6a,b[OTf]3 were isolated in 76% and 81%, respectively. In contrast, the pyridyl-substituted derivative 6c[OTf]3 was found to decompose in solution, preventing its isolation. 6a,b[OTf]3 show AX3-type spin systems in the 31P{1H}-NMR spectra (AX3 spin system: 6a[OTf]3 δ(PA) = −87.4 ppm, δ(PX) = −57.7 ppm, 1J(PP) = −271 Hz; 6b[OTf]3 δ(PA) = −47.9 ppm, δ(PX) = −41.8 ppm, 1J(PP) = −130 Hz). 6a3+ additionally shows dynamic behaviour at ambient temperature. The observed additional broad resonances resolve into an AX3 pattern at 240 K (δ(PA) = −84.0 ppm, δ(PX) = −41.5 ppm, 1J(PP) = −296 Hz), which is attributed to a similar rotational behaviour of its isopropyl groups, as described above for 2a–c[OTf]. Additional resonances at ca. −23 ppm are assigned to an unknown isomer formed by an exchange process, which could be monitored via 31P–31P EXSY NMR spectroscopy (see SI, Section 2.3.4). The resonances of 6b[OTf]3 exhibit second-order effects, as documented for related systems.7,11 Compared to the neutral iso-tetraphosphane (Cy2P)3P (AX3: δ(PA) = −108.9 ppm, δ(PX) = −5.2 ppm; 1J(PP) = −361.9 Hz), the cationic analogues 6a,b[OTf]3 exhibit upfield shifted PX resonances. Additionally, significantly smaller |1J(PP)| values are observed for the phenyl-substituted species 6b3+ compared to the cyclohexyl-substituted derivative 6a3+. This is attributed to the smaller steric volume of the phenyl substituent. Less steric congestion results in a diminished spatial overlap of the lone pairs on the outer phosphorus atoms, thereby reducing the electronic coupling between the central and terminal phosphorus atoms in 6b3+.23
Suitable crystals for X-ray diffraction analysis could be obtained by diffusion of Et2O into a saturated CH3CN (6a[OTf]3) or CH2Cl2 (6b[OTf]3) solution at −30 °C. The crystal structure of 6b[OTf]3 (Fig. 4) confirms the expected pyramidal coordination geometry at the central phosphorus atom. Due to the presence of two different substituents at the terminal phosphorus atoms, the cations 6a3+ and 6b3+ are chiral. The rac-diastereomer is observed in the single-crystal X-ray structure, with both enantiomers present in the unit cell. The P–P bond lengths (2.2315(17) Å to 2.2596(7) Å) are slightly elongated compared to neutral iso-tetraphosphanes.10,11 In 6a3+, the imidazoliumyl-substituent and the lone pair of electron pair at the central phosphorus atom adopt an eclipsed arrangement. In contrast, cation 6b3+ exhibits a staggered conformation along the same axis, wherein the lone pairs on P1 and P2 are arranged in an antiperiplanar fashion.
The Pd atoms in 7a,b[OTf]2 are in the formal oxidation state +I. The structural data indicate a Pd–Pd interaction (7b2+: Pd–Pd 2.584(19) Å). In the 31P{1H}-NMR spectra, the complexes show two sets of A2X2 spin systems (7b[OTf]2: δ(PA) = 24.5 ppm, δ(PX) = 105.33 ppm, 2J(AX) = 44 Hz; δ(PA) = 25.9 ppm, δ(PX) = 111.5 ppm, 2J(AX) = 41 Hz; for 7a[OTf]2, see SI Section 2.4), attributed to the rac and meso stereoisomers resulting from the different orientation of the imidazoliumyl-substituents. The PA resonances show the typical chemical shift of PPh3 ligands at palladium. The PX resonances of the bridging phosphanide moieties show a substantial downfield shift compared to chemical shifts of related imidazoliumyl-substituted phosphanides,15 including bridging phosphanides in three-membered metallacycles.24 In the case of 7b[OTf]2, the isomer with the more downfield-shifted PX resonances is the major isomer (84/16), whereas 7a[OTf]2 shows an inverted ratio (10/90). Interestingly, in both cases, no interconversion between isomers was observed, even at elevated temperatures or in highly polar solvents. Although these conditions typically promote isomerization in phosphorus–metal complexes, this does not seem to occur with 7a[OTf]2.25
Suitable crystals for X-ray diffraction analysis could be obtained by diffusion of n-pentane into a saturated CH2Cl2 solution at −30 °C. The molecular structure of the meso isomer of 7b[OTf]2 is depicted in Fig. 5. In the bicyclic P2Pd2 core, the two imidazoliumyl-substituted phosphanide units bridge the palladium atoms, which are connected through a short Pd–Pd contact (2.584(19) Å), indicating metal–metal interaction as known from related compounds.26 Additionally, one remaining PPh3 ligand is coordinated each of the Pd-atoms.
Although the Pd–Pd bond length is comparably short,27 the calculated Wiberg Bond Index (WBI) is fairly low (0.24), indicating only a weak interaction of the two palladium atoms (see SI Section 3.2).
During our attempts to isolate pure 7b[OTf]2, we observed the formation of a side-product at elevated temperatures. 31P-NMR investigations of the reaction mixture of 5a[OTf]2 with Pd(PPh3)4 stirred at 80 °C indicate the formation of dinuclear µ2(η2:η2)-diphosphene complex 8[OTf]2.
The complex is a structural isomer of 7b[OTf]2 and is formed by oxidative addition of the P–C bond of the imidazoliumyl substituent to Pd, rather than the P–P bond. Such P–C activation is rare and typically occurs only as a side reaction with phosphane ligands in organometallic chemistry.28
A selective synthesis of 8[OTf]2 was achieved by stirring the reaction mixture of 5a[OTf]2 with two equivalents of Pd(PPh3)4 at 40 °C for 14 days in ortho-C6H4F2. The 31P-NMR spectrum 8[OTf]2 shows broad resonances at δ(PA) = −11.7 ppm and δ(PX) = 18.2 ppm, which resolve at higher temperatures to an AA‘XX’ spin system (fitted iteratively; see SI, Section 2.4.3). The resonance of the diphosphene moiety (PA) is shifted downfield compared to the related molybdenum complex [(Cp)2Mo2(CO)4(PPh2)2] (δ(P) = −94 ppm)29,30 and the large 1J(PP) coupling constant of −489 Hz is typical for diphosphene complexes.31 In the 31P-NMR spectrum, a minor isomer is observed, which is presumed to be the corresponding meso isomer.
Single crystals of 8[OTf]2 suitable for X-ray analysis were obtained by slow diffusion of Et2O into a saturated ortho-C6H4F2 solution at −30 °C (see Fig. 5). The molecular structure revealed the rac isomer, with a central cis-substituted diphosphene coordinated to two palladium atoms in η2 mode. The palladium atoms are additionally coordinated by one LC ligand and one PPh3 ligand. The P–P bond length of 2.1160(12) Å is in the expected range for diphosphene complexes.31 The central four-membered Pd2P2 ring is puckered, adopting a “butterfly” conformation (fold angle between the P–Pd–P planes = 129.95(4)°; Fig. 5). The Pd–C bond (2.061(2) Å) aligns well with those in known N-heterocyclic carbene palladium complexes.32 Only a few related complexes have been reported, which feature a similar diphosphene ligand bridging two transition-metal atoms, such as Fe, Mo and Ta.29,30,33,34 The Pd–Pd distance of 3.8007(8) Å is significantly larger than the sum of the van der Waals radii (3.26 Å),35 indicating that there is no significant Pd⋯Pd interaction in 82+.
It is noteworthy that the formation of 8[OTf]2 from 5b[OTf]2 is highly selective. The mechanism likely involves a nucleophilic attack by a Pd atom on 5b2+, which ultimately results in the cleavage of two P–P bonds. The DFT-calculated frontier molecular orbitals of 5b2+ (RI-BP86-D4/def2-TZVP level, Fig. 6) show that the P–P bonds exhibit strong antibonding behaviour in the LUMO, indicating pronounced electrophilic character. The detailed mechanism presently remains unknown. However, it is noteworthy that 8[OTf]2 could not be generated from the isomeric complex 7b[OTf]2, which remained stable in solution at elevated temperatures for days. This indicates that 8[OTf]2 does not form via isomerization from 7b[OTf]2.
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| Fig. 7 Frontier molecular orbitals of 6a3+, resembling the high antibonding character of the LUMO and LUMO+1/+2. | ||
Following solvent removal and toluene extraction of 2a[OTf], complex 9[OTf]2 was obtained as a pure orange solid in 59% yield. The two A2X spin systems are observed in the 31P-NMR spectrum of the isolated compound in a 44
:
56 ratio. These correspond to the rac and meso diastereomers, which originate from different configurations of the P atoms in the triphosphanide ligand present in 9[OTf]2.37
The susceptibility of iso-tetraphosphane 6a[OTf]3 towards chloride-induced P–P cleavage motivated further reactions with transition metal chlorides. To this end, we treated 6a[OTf]3 with AuCl(PPh3), assuming that a similar fragmentation process might occur (Scheme 4). As expected, the reaction of 6a[OTf]3 with AuCl·PPh3 (1 equiv.) leads to the formation of 2a[OTf] and gold complex 10[OTf]2. 10[OTf]2 was isolated as an analytically pure, colourless powder (88% yield) after removal of all volatiles and repeated washing with toluene.
At room temperature, the 31P NMR spectrum of 10[OTf]2 shows broad signals. Upon cooling to 190 K, four distinct spin systems are resolved, corresponding to four isomers: rac, meso, and the rotamers rac′ and meso′ (see SI, Fig. S69). Both rac isomers exhibit AMNX spin systems with comparable features, while the symmetric meso isomer displays an AM2X spin system. The meso isomer also exhibits an AM2X spin system, with only slight differences in chemical shift between the PM and PN atoms (δ(PM) = −21.6 ppm, δ(PN) = −21.3 ppm). The central phosphorus atom shows a downfield-shifted resonance (δ(PA) = −78.9 to −84.5 ppm) compared to the anionic ligand [P(tBu2P)2]− (δ(PA) = −134 ppm),8 suggesting its coordination to the metal center. This assignment is corroborated by the crystal structure of 10[OTf]2 (see Fig. 8), which shows the rac isomer with gold coordinated linearly by the PPh3 ligand and the central P atom of the triphosphanide ligand (P2–Au–P4 angle of 172.38(5)°). The P–P bond lengths (2.210(2) Å and 2.207(2) Å) fall within the range expected for P–P single bonds.38 A slight elongation of the P–P bond is attributed to reduced negative hyperconjugation from the central phosphorus atom due to the lower electron density upon metal coordination.
Based on the successful synthesis of triphosphanide complexes 9[OTf]2 and 10[OTf]2, we explored the isolation of the free ligand. At first, we tested the reaction of 6a[OTf]3 with Ph4P[Cl] as a soluble chloride source. However, the reaction proved unselective, forming several products (see the SI, Section 2.5.5). Using the N-heterocyclic carbene IPr instead of chloride resulted in the clean formation of the desired triphosphanide salt 11[OTf] and bis(imidazoliumyl)phosphane salt 12[OTf]2 (Fig. 9). 12[OTf]2 is formed by nucleophilic attack of IPr on a LCPCy unit of 6a3+. The formation of 12[OTf]2 was confirmed by 31P-NMR spectroscopy, which showed an identical resonance δ(P) = −38.2 ppm as a sample independently synthesized via an alternative route (see SI, Section 2.5.4).39 Triphosphanide salt 11[OTf] was isolated as a yellow crystalline solid 65% yield after recrystallization from THF. The 31P-NMR spectrum of 11[OTf] at room temperature shows two broad AX2 spin systems, consistent with a rac, meso mixture (meso: δ(PA) = −135.2 ppm, δ(PX) = −3.2 ppm, 1J(PP) = −316 Hz; rac: δ(PA) = −130.6 ppm, δ(PX) = −6.9 ppm, 1J(PP) = −315 Hz). Upon cooling to 190 K, four spin systems emerge, corresponding to the rac and meso diastereomers as well as their inverted rotamers rac′ and meso′, analogous to the behaviour for 10[OTf]2.
Crystals of 11[OTf] suitable for X-ray diffraction analysis were obtained by slow diffusion of n-pentane into a saturated solution in CH2Cl2/C6H5F (v/v = 1
:
1) at −30 °C. The molecular structure is depicted in Fig. 9, confirming the presence of the meso diastereomer. The structure features the two nearly identical P–P bonds (2.1591(6) Å and 2.1606(6) Å) and a central P1–P2–P3 angle of 93.65(7)°, consistent with a flexible, uncoordinated triphosphanide framework.40
The use of transition metal chlorides in reactions with the readily accessible 6a[OTf]3 enabled the selective generation of cationic triphosphanide complexes. Two distinct coordination motifs were identified: a four-membered metallacycle in the case of palladium (9[OTf]2) and a linear coordination to the central phosphorus atom in the case of gold (10[OTf]2), showcasing the versatility of the triphosphanide framework. Motivated by these findings, we developed a direct route to the free, non-coordinated triphosphanide ligand 11[OTf], whose flexibility and structural integrity suggest a rich coordination chemistry yet to be explored.
CCDC 2524560–2524572 contain the supplementary crystallographic data for this paper.41a–m
Footnote |
| † These authors contributed equally to this work. |
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