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Redox activation of halogen-bonding catalysts for organic synthesis

Sihem Groni a, Sercan Akbabab, Uchral Otgonbayara, Jérémy Fortéa, Stefan M. Huberc, Sitthichok Kasemthaveechok*a, Bernd Schöllhorn*d and Claire Fave*a
aSorbonne Université, CNRS, Institut Parisien de Chimie Moléculaire, IPCM, F-75005 Paris, France. E-mail: claire.fave@sorbonne-universite.fr; sitthichok.kasemthaveechok@sorbonne-universite.fr
bUniversité Paris Cité, CNRS, 75013 Paris, France
cFakultät für Chemie und Biochemie, Ruhr-Universität Bochum Universitätsstraβe 150, 44801 Bochum, Germany
dITODYS UMR 7086, Université Paris Cité, CNRS, 75013 Paris, France. E-mail: bernd.schollhorn@u-paris.fr

Received 7th April 2026 , Accepted 5th June 2026

First published on 8th June 2026


Abstract

Among non-covalent interactions, halogen bonding (XB) has emerged as a sophisticated tool for molecular assembly and catalysis, distinguished from its hydrogen bonding (HB) analogues by its superior directionality and the high polarizability of the halogen atom. These characteristics offer unique opportunities for fine-tuning the strength and the geometry of this interaction to achieve targeted functionalities. Furthermore, the use of a redox-active moiety enables a controlled increase in the XB donor strength upon oxidation, effectively activating the XB donor catalyst. Herein, we report the rational design and the synthesis of ferrocene-based XB donors. Characterization of the fundamental XB interactions in the system was performed through a synergistic approach involving single-crystal X-ray diffraction and solution-phase binding studies. Density Functional Theory (DFT) analysis reveals a significant amplification of the ‘σ-hole’ intensity upon oxidation, a feature we exploit to drive catalytic turnover. Notably, these redox-switchable iodoferrocene derivatives serve as potent catalysts for XB-mediated Friedel–Crafts alkylation reactions, even in competitive polar solvents—a challenging environment for traditional XB catalysis. This work demonstrates the efficacy of charge modulation by redox activation in fine-tuning XB strength for organic transformation.


Introduction

Organocatalysis has transformed synthesis by facilitating molecular transformation under mild and metal-free conditions.1–4 Enhancing catalytic activity in solution through the combination of external stimuli and supramolecular chemistry remains an exciting challenge.5–7 Among supramolecular interactions, halogen bonding has emerged as a particularly promising approach. Noncovalent halogen bonding (XB) has attracted considerable interest across chemistry and biochemistry owing to its distinctive features, particularly its pronounced directionality. Beyond its well-established conceptual foundations in crystal engineering, molecular recognition, and biomolecular interactions, XB has recently emerged as a powerful tool in organic synthesis even if it remains a weak interaction.8–12 This renewed attention stems from the presence of a partially electron-deficient region—known as the “σ-hole”—on halogen atoms.13 Acting as a Lewis acid, the σ-hole enables XB donors to engage in specific attractive interactions with Lewis bases. In the context of organic synthesis, the Lewis bases involved are typically weaker than those employed in other applications of halogen bonding.14,15 Consequently, strategies to enhance halogen-bond strength are crucial for expanding its utility and effectiveness in promoting organic reactivity.

For decades, efforts to enhance the strength of the halogen bond donors, predominantly iodine-containing derivatives, have focused on two concept strategies.16–19 The first involves chemical modification of the molecular scaffold by introducing electron-withdrawing groups (EWGs) and/or permanently charged moieties to electronically increase the strength of the XB (Fig. 1a). This approach provides great flexibility, enabling various molecular backbones in a manner that enhances the binding capacity of halogen bond donors. A second strategy consists of combining two or more XB donors to amplify and promote the halogen bond interaction. The main limitations arise from the strict geometric requirements inherent in the halogen bond, the intrinsic stability of the donor moieties, and solubility issues which complicate the rational design and synthesis of new XB donors.


image file: d6sc02883g-f1.tif
Fig. 1 (a) Halogen bond strength modification strategies. (b) Redox activation of halogen bonding.

In recent years, redox activation has emerged as a powerful and innovative strategy for enhancing halogen bond donor strength (Fig. 1b). In this approach, oxidation of the XB donor bearing redox-active moieties, such as tetrathiafulvalenes and ferrocene, increases the electrophilicity character of the halogen atom, thereby amplifying the value of its σ-hole.20–26 This strategy opens new opportunities for deploying XB in organic synthesis. Several iodinated redox-active compounds, particularly those incorporating ferrocene units, have been reported and demonstrated to function as strong halogen bond donors in both anion sensing27–30 and catalysis.31,32 Despite these promising results, the broader use of redox activation to modulate halogen-bond strength remains relatively underexplored. The use of such reversible redox entities allows for a dynamic control of the halogen-bond interaction in solution. The ultimate goal of the present work is to trigger a catalytic reaction via the electrochemical switching of a tailored redox-active XB-donor catalyst as recently reported in C–N bond formation using anthracene derivatives.33,34 Herein, we reported a novel molecular design strategy for iodoferrocene-derived XB donors. By leveraging the redox-active ferrocene core, we demonstrate a tunable ‘σ-hole’ strength that facilitates halogen-bond-mediated Friedel–Crafts alkylation. Our findings highlight the role of charge induction by redox activation in stabilizing XB interactions within polar media, providing a versatile platform for redox-switchable catalysis.

Results and discussion

Synthesis of the catalysts

Fc-1 was designed as a bidentate redox active XB-donor catalyst based on a 3,5 disubstituted pyridine. The two ferrocenyl groups are directly linked to the iodotriazole moieties thus providing an efficient electronic communication with the halogen atoms via the π-conjugated system. However, the arrangement of these ferrocenyl–iodotriazol units at the 3 and 5 position of the pyridine core prevents the direct electronic coupling between the redox active groups. The synthesis of Fc-1 was accomplished in a single step via a modified Cu(I)-catalyzed azide–alkyne 1,3-dipolar cycloaddition between 3,5-diiodoethynylpyridine and azidoferrocene in 56% yield (Scheme 1). The use of 3,5-diethynylpyridine instead afforded the halogen free analogue Fc-3 in 71% yield. Subsequent regioselective alkylation of Fc-1 and Fc-3 at the pyridine core with methyl trifluoromethanesulfonate afforded the cationic species (Fc-2)OTf and (Fc-4)OTf in 92 and 89% yield, respectively.
image file: d6sc02883g-s1.tif
Scheme 1 Synthesis of ferrocene-based XB donors and non-XB donor analogues. Reaction conditions: (i) Cu(MeCN)4BF4, azidoferrocene, tris-(benzyltriazolylmethyl)amine, diisopropylethylamine, CH2Cl2, 4 h, rt, 56 and 71% yield for Fc-1 and Fc-3, respectively; (ii) MeOTf, CH2Cl2, 1 h, Ar, rt, 92 and 89% yield for (Fc-2)OTf and (Fc-4)OTf, respectively.

Photophysical and electrochemical characterization of the catalysts in the neutral state

To probe the electronic communication between the redox-active ferrocene scaffold and the halogen bond (XB) donor site, we performed UV-vis spectroscopic studies in 1[thin space (1/6-em)]:[thin space (1/6-em)]1 dichloromethane/acetonitrile (Table 1). The fundamental d–d transition of the ferrocene core, observed at 427 nm, undergoes a subtle bathochromic shift to 437 nm in both Fc-1 and Fc-3, upon conjugation with the triazole moiety. This shift is further intensified to 441 nm following N-methylation to the pyridinium core in (Fc-4)OTf, a result of the lowered LUMO energy induced by the potent electron-withdrawing nature of the quaternary heterocycle. In contrast, the presence of iodine in (Fc-2)OTf results in a weak hypsochromic shift to 436 nm. The σ-hole of the iodine donor effectively modulates the electron-deficiency of the pyridinium ring, thereby widening the HOMO–LUMO gap. However, the ability of the iodine donor to modulate the electronic environment of ferrocene, even in the presence of a permanent positive charge, underscores the robustness of the charge-induction effect.
Table 1 Electrochemical and photophysical data for ferrocene derivatives and their respective oxidized species in 1[thin space (1/6-em)]:[thin space (1/6-em)]1 ACN/CH2Cl2 solution. (Electrochemical cond.: 0.25 mM Fc derivatives with 0.1 M n-Bu4NBF4. UV-vis cond: ∼0.5–1.0 × 10−5 M Fc-derivatives, optical path 1 cm)
Compound Epc1a (C–I) Epc2a (py+) E°′b (Fc/Fc+) λmaxc (εd) (reduced state) λmaxc (εd) (oxidized state) t1/2e (oxidized state)
a Reductive potential peak in V vs. SCE.b Formal standard potential in V vs. SCE.c Wavelength maximum of absorption in nm.d Molecular extinction coefficient in M cm−1.e Half-life time in min.
Fc 0.53 427 (170) 617 (641) >24 h
Fc-1 −1.40 0.70 437 (718) 642 (1341) 15
(Fc-2)OTf −1.64 −1.05 0.78 436 (1157) 642 (1421) 200
Fc-3 0.68 437 (635) 690 (851) 8
(Fc-4)OTf −1.07 0.72 441 (900) 688 (984) 6


Cyclic voltammetry (CV) of Fc-1, (Fc-2)OTf, Fc-3, and (Fc-4)OTf in a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 mixture of dichloromethane/acetonitrile and 0.1 M tetrabutylammonium tetrafluoroborate (n-Bu)4BF4 is shown in Fig. 2 and Table 1. All ferrocene derivatives exhibit a reversible oxidation wave at the same formal standard potential of +0.73 ± 0.05 V vs. SCE, which is about 200 mV more positive than that of ferrocene. This behaviour is similar to that reported by Molina and colleagues and is characteristic of the ferrocene attachment to the triazole rings at the N-1 position.29 Surprisingly, the formation of the pyridinium ion results in a slight anodic shift in both cases (Fc-1 relative to Fc-2+ or Fc-3 relative to Fc-4+), probably due to steric hindrance or reorganisation in solution. Similar diffusion coefficients have been determined for all investigated ferrocene derivatives (D ∼ 10−5 cm2 s−1) suggesting their similar solubility and mobility in solution. The plot of the peak current versus the square root of the scan rate shows a linear trend accounting for a reversible diffusion limited electrochemical process meaning that the species freely diffuse in solution (Fig. S7 to S10).35


image file: d6sc02883g-f2.tif
Fig. 2 Cyclic voltammograms of 0.25 Fc-1 (black), Fc-3 (red), (Fc-2)OTf (green), (Fc-4)OTf (blue), and ferrocene (grey) versus the saturated calomel electrode (SCE) as the reference and 0.1 M n-Bu4NBF4 in 1[thin space (1/6-em)]:[thin space (1/6-em)]1 acetonitrile/dichloromethane as the electrolyte on a GC working electrode and Pt counter electrode; scan rate 0.1 V s−1.

In reduction, two different redox processes can be observed. (Fc-4)OTf and (Fc-2)OTf both exhibit an irreversible reduction peak centered at −1.07 V and −1.05 V vs. SCE, respectively. This wave is attributed to the reduction of the pyridinium core and is only slightly affected by the chemical structures of the XB donors. A second irreversible wave appears for Fc-1 and (Fc-2)OTf at −1.40 V and −1.64 V, respectively, corresponding to C–I bond cleavage. The ∼240 mV shift in the C–I bond cleavage wave indicates that the C–I bond is either coordinated to the OTf anion or stabilized by the electron-deficient pyridinium ring. This observation confirms halogen bonding in solution and motivated us to explore further evidence in both solid and solution states before investigating its role in catalysis.

Evidence of halogen bonding in crystal and solution

Evidence of halogen bonding in the crystal structure. X-ray diffraction of single crystals obtained for each compound is presented and discussed here (see the SI for more details and for the crystallization conditions). The resulting structural analyses provide further insight into Fc-1 and Fc-3. Both compounds crystallize in the monoclinic system, space group P21/c, albeit with different unit cell parameters. The centroids of the triazole rings were defined in order to determine the dihedral angles between the two triazoles and the attached iodine or hydrogen atoms (Table 2). Thus, the molecular arrangements of the two analogues differ significantly. In Fc-1, the two iodine atoms are oriented in opposite directions (dihedral angle ∼124°, i.e., >90°), whereas in Fc-3, the triazole C–H groups are oriented in the same direction (dihedral angle ∼54°, i.e., <90°). Weak intermolecular C–H⋯N and C–I⋯N interactions are observed for Fc-3 and Fc-1, respectively, between the C–H or C–I group of one triazole and either the N atom of the pyridine ring or a N atom of a neighbouring triazole, thereby contributing to the overall packing arrangement.
Table 2 Dihedral angle of (H1/I1-triazole1-triazole2-H2/I2) values in °
Fc-1 Fc-3 (Fc-2)OTf (Fc-2)I (Fc-4)OTf
−124.537(18) −53.706(2) 1.624(15) 3.639(11) 13.254(2) 32.804(2)


The methylated analogues (Fc-2)OTf and (Fc-4)OTf crystallize in the P21/c (monoclinic system) and the P[1 with combining macron] (triclinic system) space groups, respectively. In the case of (Fc-4)OTf, two symmetry-independent molecules are present in the asymmetric unit. (Fc-4)OTf adopts a conformation similar to that of its neutral precursor Fc-3. In contrast, in (Fc-2)OTf, the two iodine atoms are oriented inward and engage in halogen bonding with the counter anion (Fig. 3). The I⋯O distances (around 3.02 Å and 2.96 Å) are approximately 15% shorter than the theoretical sum of the van der Waals radii (3.50 Å). Moreover, the nearly linear C–I⋯O angles (∼165.2–169.0°) clearly indicate highly directional halogen bonding.36,37 This behaviour is not specific to triflate, as similar features are observed when iodide acts as the counter-ion in (Fc-2)I. In this structure, the I⋯I distances (around 3.34 Å and 3.46 Å) are approximately 18% shorter than the sum of the van der Waals radii (4.10 Å), and the more linear C–I⋯I angles (∼172.3–173.2°) further highlight the presence of XB interaction in the crystal state. Interestingly, in both iodinated structures, the dihedral angle between the two triazole rings is close to 0° (∼1.6–3.6°), revealing an almost coplanar arrangement of the triazoles. For (Fc-4)OTf, weak intermolecular C–H⋯O interactions are observed between the triazole C–H groups and one oxygen atom of the triflate counter-anion. In addition, π⋯π stacking interactions between certain Cp rings and the pyridine ring of a neighbouring molecule are also present. Similarly, in both (Fc-2)OTf and (Fc-2)I, π⋯π stacking interactions between neighbouring triazole rings complement the XB interactions. In all three methylated derivatives, these non-covalent interactions act in concert to define the supramolecular architecture of the crystal.


image file: d6sc02883g-f3.tif
Fig. 3 Crystal structure wireframe representations of (Fc-2)OTf (left) and (Fc-2)I (right). Atoms involved in halogen bonding are highlighted in ball drawing, and the XB interactions are depicted as orange dashed lines and their distance values are indicated (Å). Atom colour code: purple (I), red (O), yellow (S), green (F), orange (Fe), blue (N), and grey (C). Hydrogen atoms, solvent molecules (ACN for (Fc-2)OTf and DMF for (Fc-2)I and the second position of the disordered Cp group in (Fc-2)OTf, are omitted for clarity. Selected bond distances (Å) and angles (°). (Left) I⋯O: 2.9634(53)–3.0254(52), C–I⋯O: 169.071(235)–165.238(202), (right) I⋯I: 3.3353(6)–3.4617(7), C–I⋯I: 173.179(142)–172.193(138).
Evidence of halogen bonding in solution. To evidence the formation of a XB complex in solution, various 13C NMR spectra of Fc-2+ in the presence of different anions have been recorded (Fig. S19 and S25). The carbon C6, which is connected to the iodine in the pyridinium core received the strongest influence of anion. 13C NMR in dimethylsulfoxide-d6 exhibits a difference of ca. 35 ppm between the iodide anion (δ = 88.6 ppm) and triflate anion (δ = 124.4 ppm). Interestingly, a significant downfield shift suggests the heavy atom effect by the iodide ion.38 In addition to NMR, potentiometric titration was also performed to evaluate potential anion interaction through halogen bonding. Upon the addition of Cl to Fc-1 in a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 dichloromethane/acetonitrile mixture, the system exhibits a ΔE of 21 mV with a small loss of reversibility suggesting a competition between halogen bonding interaction and chemical reaction (Fig. S11). When a weak Lewis base is added in the solution almost negligible interaction has been recorded (Fig. S12 and S13), confirming these observations.21–23,27–29 Thus our data obtained in both the crystal state and solution confirm the presence of halogen bonding. While the interaction is relatively weak, it prompted us to further investigate the oxidized forms of these complexes and their reactivity in chemical reactions.

Ferrocenium Fc-12+, Fc-23+, Fc-32+ and Fc-43+

To assess the potential reactivity of the cationic complexes and achieve adequate stabilization of the ferrocenium species, we opted to investigate chemical oxidation. For this transformation – converting the neutral XB donors into their corresponding ferricenium cations Fc+BF4 – we selected NOBF4, a well-known chemical oxidant.39 First, to validate this oxidant toward Fc derivatives, we added 1.2 equivalents of NOBF4 to a solution of Fc in a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 dichloromethane/acetonitrile mixture. This resulted in the emergence of a new absorption band at 617 nm, characteristic of a LMCT band of the Fc+ cation (Fig. 4).40,41 UV-vis absorption spectra of the oxidized dicationic states of the XB donors have thus been recorded following the same procedure. Fc-12+ displays a characteristic LMCT band at 642 nm (red trace in Fig. 4) with an estimated half-life of 15 minutes (see the SI for more details). This band is slightly red-shifted in comparison to that of Fcλ = 25 nm), which could be attributed to the change in the HOMO−1/LUMO gap in the presence of electron-withdrawing groups.42 Meanwhile, oxidation of Fc-3 by NOBF4 afforded the corresponding ferrocenium Fc-32+, with a further red-shifted absorption band at 690 nm. Fc-32+ appeared to be less stable (t1/2 ∼8 min, Fig. S3 and S4) than Fc-12+. The increased persistent character of the iodinated species suggests a significant influence due to the presence of halogen atoms in Fc-12+. In the tricationic species, the UV-vis spectra of Fc-43+ (λ = 688 nm) and Fc-23+ (λ = 642 nm) were similar to those of their respective non-methylated derivatives Fc-32+ and Fc-12+. While Fc-43+ displayed a similarly short lifetime (t1/2 ∼6 min) close to that of Fc-32+, the iodinated analogue Fc-23+ showed remarkable stability with a measured half-life of 3.7 hours in solution (Fig. S5 and S6). This result underscores the synergetic effect between halogen bonding and molecular orientation in solution.
image file: d6sc02883g-f4.tif
Fig. 4 UV-vis absorption spectra of Fc-12+ (black), Fc-23+ (red), Fc-32+ (green), Fc-43+ (blue), and Fc+ (grey) in 1[thin space (1/6-em)]:[thin space (1/6-em)]1 dichloromethane/acetonitrile. Counter anions were omitted for clarity.

Computational details

Kohn–Sham density functional theory (DFT) as implemented in the Gaussian (G16) package was used for all computations,43 employing the M06L44 functional with D3 dispersion corrections.45 The def2-TZVP basis set was used for all elements except I and F, which were treated with def2-TZVPD.46 All structures were optimized in the gas phase and were confirmed as minima by the absence of imaginary frequencies. Calculations for Fc-1 were conducted with charges 0 and +2, while charges +1 and +3 have been used for Fc-2+; in both cases the oxidized forms were more stable as triplets, as expected (Fig. 5, see the SI for more details). For both pyridine and pyridinium compounds, the electrostatic surface potential (ESP) of the respective σ-holes exhibited the effect of permanent charge. The respective σ-hole potentials of Fc-1 and Fc-2+ increased from 34.6 to 86.2 kcal mol−1, consistent with σ-hole amplification through chemical modification (Fig. 5). Interestingly, oxidation of the two ferrocene units in Fc-1 resulted in a 3.5-fold increase in σ-holes, which jumped to 120 kcal mol−1, demonstrating the positive impact of the activation of the halogen bond by redox activation. When redox activation was combined with a permanent pyridinium charge, the σ-hole value from ESP at iodine atoms in Fc-23+ increased further to 180 kcal mol−1. Considering the σ-hole value of Fc-1 the redox activation in the presence of permanently charged Fc-23+ could lead to an up to fivefold increase in the σ-hole strength, indicating that redox chemistry provides an effective means to amplify the σ-hole on demand.
image file: d6sc02883g-f5.tif
Fig. 5 Molecular electrostatic potential surface mapped at the 0.001 e au−3 isovalue for the neutral and dication of Fc-1 and monocation and trication of Fc-2 with an indication of its magnitude at the σ-hole (in kcal mol−1). Note the different colour scale set from the extrema at the lowest and highest values in the molecule for each oxidation state.

Application in organic synthesis: redox activation of the XB donors for promoting Friedel–Crafts alkylation

The catalytic activity of the well-characterized bidentate XB donor catalysts, as well as their non-halogenated analogues, was then evaluated in organocatalytic reactions. The Friedel–Crafts alkylation reaction was selected as a benchmark due to its high sensitivity to Lewis acid activation, which allows for a clear quantification of the halogen bonding effect.47,48 In fact, previous studies have established that bidentate XB donors can achieve significantly higher reaction rates compared to their hydrogen-bonding (HB) analogues in dichloromethane. The XB catalyst activates the labile C–X bond of benzhydryl halide thus accelerating the cleavage of the C–X bond and generating a benzhydryl cation,49–52 which promptly reacts with the nucleophilic 1,3,5-trimethoxybenzene 2 following a conventional electrophilic aromatic substitution mechanism.
Friedel–Crafts alkylation with C–Br bond cleavage. The first Friedel–Crafts alkylations were performed using Fc-1. The active species, Fc-12+, was generated by the addition of a Fc-1 solution to the NOBF4 oxidant, which was then transferred to a solution containing benzhydryl bromide 1 and 1,3,5-trimethoxybenzene 2 in an NMR tube. These primary screenings employed a stoichiometric amount of the XB donor and 1, consistent with established literature protocols, and an excess of Cs2CO3 to scavenge any Brønsted acids, thereby ruling out ‘hidden’ acid catalysis. To evaluate solvent effects on catalytic efficiency, screenings were conducted in dichloromethane-d2 (CD2Cl2), 1[thin space (1/6-em)]:[thin space (1/6-em)]1 dichloromethane-d2/acetonitrile-d3 (CD2Cl2/CD3CN), and acetonitrile-d3 (CD3CN).

As shown in Table 3, in the presence of the activated catalyst Fc-12+ in CD2Cl2, product 3 was obtained in trace amounts after 24 h, as expected for the insoluble XB donor. Surprisingly, in a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 mixture of CD2Cl2/CD3CN (entry 2, Table 3) the yield could be increased up to 59% (after 24 h). While this yield is moderate compared to the early reports in similar non-polar solvents (e.g., yields >90% in CH2Cl2),47 our ferrocene-derived catalyst maintains catalytic activity in CH3CN, unlike previously reported bidentate XB donors, known to suffer from severe competitive inhibition in polar and coordinating solvents.48

Table 3 Reaction yields of product 3 in Friedel–Crafts alkylationa

image file: d6sc02883g-u1.tif

Entry Solvent Catalyst NMR yieldb
2 h 24 h
a Standard reactions conditions: 0.05 mmol of the catalyst in dry deuterated solvent under Ar, 1 eq. of 2, 2 eq. Cs2CO3.b 1H NMR yields using t-amyl methyl ether as an internal standard.
1 CD2Cl2 Fc-12+ 1 2
2 1[thin space (1/6-em)]:[thin space (1/6-em)]1 CD2Cl2/CD3CN Fc-12+ 54 59
3 CD3CN Fc-12+ 65 74
4 1[thin space (1/6-em)]:[thin space (1/6-em)]1 CD2Cl2/CD3CN Fc-23+ 80 98


In addition, in a pure acetonitrile solution, 1H-NMR monitoring of the conversion yield revealed an acceleration of the reaction kinetics with a yield of 65% after only 2 h. After 24 hours, the yield was 74% (entry 3, Table 3), slightly higher in a CD2Cl2/CD3CN mixture. We attribute this observation to the unique redox-induced σ-hole strength amplification, which highlights the importance of the polar solvent in the reaction kinetics. However, due to the poor solubility in acetonitrile of the neutral XB donor in prior oxidation, the 1[thin space (1/6-em)]:[thin space (1/6-em)]1 CD2Cl2/CD3CN mixture seemed to us to be a good compromise and was used for further studies.

Based on the computational data, the presence of three positive charges in Fc-23+ should further enhance reactivity. In fact, the use of Fc-23+, the oxidized form of Fc-2+, furnished the desired products in excellent yield (80% and 98%) within 2 h and 24 h, respectively (entry 4, Table 3). This suggested that the synergistic effect between the permanent positive charge and the redox activation enables such a significantly strong XB donor. Indeed, by switching from Fc-12+ to Fc-23+, we were able to increase the yield by approaching almost total conversion after 24 hours.

Friedel–Crafts alkylation with C–Cl bond cleavage. Encouraged by these results, we extended our study towards the benzhydryl chloride analogue 4.53,54 The main difficulty in using the chlorinated derivative 4 stems from the higher bond dissociation energy (BDE) of the C–Cl bond compared to the C–Br bond (74 versus 63 kcal mol−1, respectively) making the C–Cl bond harder to cleave.55 In the first attempt we tested Fc-12+ in the presence of 4, under the same conditions as previously used with 1. After 2 hours, the product 3 was obtained in 40% yield, suggesting a slightly slower kinetics profile than that of the brominated derivative 1 (Table 4, entry 1 vs. Table 3 entry 2). However, in terms of thermodynamics, Fc-12+ did not show any difference in efficiency. In fact, after 24 hours, a yield of 64% was obtained similar to that obtained with 1 (59%). As expected, the use of the tricationic Fc-23+ complex (Table 4, entry 2) induces a significant increase in reactivity compared to the Fc-12+ derivative, both kinetically (64% in 2 hours) and thermodynamically (70% in 24 hours) (Table 4, entry 2).
Table 4 Yield of product 3 in the reaction starting from 4a

image file: d6sc02883g-u2.tif

Entry Catalyst Calculated σ-holeb NMR yieldc
2 h 24 h
a Standard reactions conditions: 0.05 mmol of the catalyst in dry deuterated solvent under Ar, 1 eq. of 2, 2 eq. Cs2CO3.b σ-Hole magnitude in kcal mol−1.c 1H NMR yields using t-amyl methyl ether as an internal standard.d 4 times repetition with 1.25% as the standard deviation.
1 Fc-12+ 120 40 64
2d Fc-23+ 180 64 70
3 Fc-1 86.2
4 Fc-2 34.6
5 Fc-32+
6 Fc+
7 I2 <5
8 p-TsOH <5


In order to confirm the fundamental impact of the halogen bonding in this Friedel–Crafts alkylation reaction, a series of control experiments was carried out. First, using non-oxidized or activated catalysts Fc-1 and Fc-2+ (Table 4, entries 3–4) completely hampered the reactivity with no detection of the expected product. This behavior can be attributed to the low value of the σ-hole compared to their oxidized counterpart. Ferrocenium Fc+ (Table 4, entry 5) and hydrogen bond donor Fc-32+ (Table 4, entry 6) also blocked the reactivity, suggesting that the reactivity did not originate from ferrocenium or other non-covalent interactions. Replacing the XB donor with elemental iodine (Table 4, entry 7) or with p-toluenesulfonic acid (Table 4, entry 8) exhibited the formation of a trace amount of product 3 (<5% yield) after 24 hours. All these findings strongly suggest that a strong halogen bonding is the key interaction promoting this reactivity. Moreover, the amplification of the σ-hole value is crucial for reactivity in polar solvents.

Based on the combined experimental and DFT observations, we further hypothesized that, in the presence of a coordinating solvent, acetonitrile, the halide abstraction reaction might proceed catalytically. To test this hypothesis, we varied the loading of the Fc-23+ catalyst, the most active XB donor (Fig. 6).


image file: d6sc02883g-f6.tif
Fig. 6 Yield vs. time diagram for the formation of 3 in the reaction from 4 using 100 mol% (8.33 mM, black circle), 50 mol% (4.17 mM, red triangle), 25 mol% (2.09 mM, blue square), 10 mol% (1.05 mM, grey empty square) and 2.5 mol% (0.26 mM, green star) of the Fc-23+ catalyst. All reactions were conducted on a 0.05 mmol scale (8.33 mM), using dry 1[thin space (1/6-em)]:[thin space (1/6-em)]1 acetonitrile-d3/dichloromethane-d2 solvent under Ar, 1 eq. of 2, 2 eq. Cs2CO3. The yield of 3 has been determined according to 1H-NMR analysis with t-amyl methyl ether as an internal standard.

While keeping the substrate concentration constant, reducing the catalyst loading to 50 mol% slightly diminished reactivity, yielding 60% of product 3 after 24 hours. This suggests that the reaction may indeed be catalytic. However, since the molecule contains two iodine atoms, the observed reactivity could still be considered stoichiometric per iodine atom.

Further reducing the amount of Fc-23+ to 25 mol% and 10 mol% had a noticeable impact on the initial reaction rate. Nevertheless, the system maintained remarkable reactivity under these conditions, delivering 75% and 52% yields for 25 mol% and 10 mol% of Fc-23+, respectively. UV-vis analysis with substrates and 10 mol% Fc-23+ was also conducted, and the characteristic Fc-23+ absorption at 640 nm persisted for 18 h, indicating that the catalyst remains present in equilibrium with other species in solution (Fig. S15). At the lowest catalyst Fc-23+ loading (2.5 mol%), reactivity dropped, with the yield failing to exceed 30% after 24 hours. This suggests that the catalyst is involved in the rate-determining step but remains catalytic, with a turnover number (TON) up to 10.

Additionally, since the plateau yield observed at 25 mol% catalyst loading after 24 hours is nearly identical to the yield under stoichiometric conditions, we further explored the role of catalyst concentration in the reaction kinetics. First, we examined how catalyst concentration affects the reaction, while maintaining the absolute ratio with compound 4 as a constant, i.e. 25 mol%. The reaction with a higher catalyst concentration (Table 5, entry 3) progressed significantly faster than the more diluted version (Table 5, entry 6). Both conditions eventually reached a comparable maximum, which suggests that the reaction order with respect to total concentration is greater than zero, meaning that collisions between reactive species become a limiting factor under dilute conditions.

Table 5 Initial kinetics rate and NMR yield after 24 h of the standard (Table 4) with various catalysts and substrate loadingsa
Entry Substrate loadingb Catalyst loadingc kreld NMR yielde
a Standard reactions conditions: 0.05 mmol of the catalyst in 0.6 mL dry deuterated solvent under Ar, 2 eq. Cs2CO3.b Substrate loading (both 2 and 4) in µmol.c (Fc-2)3+ loading (%).d Relative initial rates after 1 h of reaction time, referenced to entry 3.e 1H NMR yields using t-amyl methyl ether as an internal standard.
1 5 100 3.0 73
2 5 50 2.0 59
3 5 25 1 75
4 5 10 0.68 54
5 5 2.5 0.87 30
6 20 25 19 77


In the second step, we studied the impact of the concentration of substrate 4 while keeping the concentration of Fc-23+ constant. Interestingly, the substrate concentration had a less pronounced impact on the kinetic profile (Table 5, entry 1 and 6). By fixing the catalyst concentration, reactions conducted at ∼8 mM or ∼33 mM concentration exhibited very similar kinetic profiles, both reaching a plateau of 70–75% yield within 6 hours. While the higher substrate concentration (33 mM) showed a faster initial rate, the difference was much less dramatic than the effect of varying the catalyst concentration. Even though this catalytic behavior is counterintuitive to typical halogen bonding reactivity, the catalytic activity may be attributed to coordination by the polar solvent, which facilitates halide decoordination after abstraction and thereby regenerates the active XB donor.

Conclusions

In conclusion, we have demonstrated the redox activation of chelating halogen bond donors for the promotion of a chemical reaction. A molecular bidentate system based on iodine-ferrocene architecture has been designed and its structure–property relationship, investigated. We found that only ferrocenium XB donors Fc-12+ and Fc-23+ are chemically more stable than HB donors Fc-32+ and Fc-43+, with a half-life of up to 4 h under Ar. Assessment of ‘σ-hole’ strength in the neutral and ferrocenium state revealed that redox activation is a powerful complement to structural modifications, enabling an up to five times increase in ‘σ-hole’ strength relative to the neutral state of the redox couple. This redox-activation provided an opportunity to use oxidized XB donors in the halide abstraction reaction affording TON = 10 at 2.5 mol% catalyst loading. We attribute this unprecedented catalytic performance to the presence of a coordinating solvent, which may act as a competing ligand, facilitating dynamic halide anion de-coordination in order to regenerate the XB-catalyst. While the consequences of these observations remain to be explored, their potential impact is of fundamental interest for exploring a broader scope of chemical transformations and designing new functional and more stable redox-active halogen bond donors for better control in organic synthesis.

Author contributions

CF and BS conceptualized the project. CF, BS and SCK directed the project. SG, SA, UO, JF and SCK performed the experiments. SMH performed the calculations. All authors co-wrote the manuscript, discussed the results, and commented on the manuscript.

Conflicts of interest

There are no conflicts to declare.

Data availability

CCDC 2536425–2536429 (Fc-1, (Fc-2)OTf, (Fc-2)I, Fc-3 and (Fc-4)OTf) contain the supplementary crystallographic data for this paper.56a–e

Data are available upon reasonable request.

Supplementary information (SI): electrochemical investigation, NMR spectra and further experimental details. See DOI: https://doi.org/10.1039/d6sc02883g.

Acknowledgements

We thank the Ministère de l'Enseignement Supérieur, de la Recherche et de l'Innovation, the Centre National de la Recherche Scientifique (CNRS). Elric Engelage and Geoffery Gontard for X-Ray structures. SMH acknowledges Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy – EXC 2033 – 390677874 – RESOLV for access to a computational cluster.

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Footnote

Both authors contributed equally.

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