Mechanistic Aspects of the Photofunctionalisation of Tetraalkylammonium Cations by [PtCl₆]²⁻

Abstract

Unexpected activation of the tetrabutylammonium cation in the presence of hexachloroplatinate(IV) under light to give a dinuclear complex of trans-μ²:η²,η²-1,3-butadiene-bis(trichloroplatinate(II)) along with a proposed mechanism of the activation has been reported. The mechanism has been investigated using a combination of photodissociation photodetachment mass spectrometry, and frozen-matrix EPR spectroscopy, in addition to 1D and 2D NMR spectroscopy. In addition to the Bu₄N⁺ salts of [PtCl₆]²⁻ that were part of the original observations, the reactivity of Bu₄P⁺, Pr₄N⁺, and Pe₄N⁺ (Pe = pentyl) salts has also been investigated, and, in addition, the possible involvement of η²-butene complex intermediates has been investigated. The combined results provide additional evidence and support for the originally proposed mechanism of activation of the Bu₄N⁺ cation.

1. Introduction

As part of a study on possible syntheses of chloro-bridged, mixed-metal complexes of platinum, palladium and gold, we previously reported that it was possible to prepare the anion [Cl₂Pd(μ-Cl)₂PtCl₂]²⁻ [1]. It was obtained as its [K(18-crown-6)]⁺ salt as a statistical, ca 25% part of a mixture that also contained [Pd₂Cl₆]²⁻ and [Pt₂Cl₆]²⁻, following a purely thermal reaction of K₂[PtCl₄] and K₂[PdCl₄] in the presence of [K(18-crown-6)]⁺. In then attempting to prepare an analogous anion containing both platinum and gold, K[AuCl₄] and K₂[PtCl₄] were reacted together in water, leading to a redox reaction and formation of [PtCl₆]²⁻ and either [AuCl₂]⁻ or Au⁰ depending on the ratio of salts used. In determining the course of these reactions and the products formed, [Bu₄N]⁺ was added to the solution post reaction, which resulted in the formation of [Bu₄N]₂[PtCl₆]. On one occasion in the course of this work, a sample was left in an NMR tube from which crystals were recovered that turned out to be of the [Bu₄N]⁺ salt of the dinuclear Pt^II complex [Cl₃Pt(μ²:μ²-1,3-butadiene)PtCl₃]²⁻ (Figure 1, 1) [2]. This complex exists in up to four isomeric forms, and we have reported on the dynamics of these complexes in solution as studied by NMR spectroscopy [3].

We reported on this observation and our finding that the reaction was mediated photochemically through excitation of the [PtCl₆]²⁻ anion [2], even though our first isolation of the complex arose from serendipitous ambient irradiation. Understanding that the reaction was driven photochemically and using calculations of excited states and in situ EPR measurements, we were able to propose a mechanism consistent with both the observed products and with literature precedent that invoked two different C–H activation steps, each with concomitant reduction to Pt^II. We now report the results of further experiments to investigate aspects of the mechanism of this somewhat unprecedented reaction and to understand something of its scope.

2. Results

To probe the scope and hence mechanism of this reaction further, complementary experiments were identified that would provide additional support and insight, and it is these that form the basis of this paper. First, revisiting the mechanism (Figure 1) proposed originally, the photochemically driven formation of the σ-alkyl complex 2 is uncontentious, being based upon the extensive work of Shilov and Shul’pin [4,5,6,7,8,9,10,11,12], and β-hydrogen elimination from this complex to form 3 would be anticipated. Complex 3 then undergoes hydrogen abstraction followed by Hofmann elimination [7] to extrude the monoplatinum η²-butadiene complex 5, which then complexes with Pt^II to give 1. Both the formation of the σ-alkyl complex and the generation of Cl^• occur via photoexcitation that generates Pt^III and leads ultimately to Pt^II.

The lower part of Figure 1 shows photoexcitation of [PtCl₆]²⁻ leading to Cl^• (and Pt^III), which can then abstract a hydrogen from the β-position of the now functionalised alkyl group to give radical 4. In turn, this extrudes alkene 5, which reacts photochemically with [PtCl₄]²⁻ (from reduction of Pt^III) to give product 1; proposing Bu₃N^• is consistent with the observation of Bu₃NH⁺ by liquid injection field desorption/ionisation mass spectrometry reported earlier (requiring only proton abstraction in the medium) [2]. We also note that ‘consumption’ of two equivalents of Pt^IV requires the formation of a single equivalent of butadiene, and so with Bu₄N⁺ in excess, it is statistically most likely that each butadiene will result from activation of Bu₄N⁺, which would require Bu₃NH⁺ as the major nitrogen-containing product.

2.1. Photodissociation and Photodetachment Mass Spectroscopy of [Bu₄N]₂[PtCl₆]

Photodissociation and photodetachment mass spectrometry was exploited to identify species resulting from the irradiation of [PtCl₆]²⁻, offering the advantage of being able to probe the very reaction solutions used in the bulk experiments. The technique subjects the compound of interest to photoexcitation using energies in excess of those required for fragmentation and then detects the products using mass spectrometry, accessing both positive and negative ion modes. Solutions are introduced into the ion-trap mass spectrometer by electrospray methods.

Details of how the mass spectrometer is configured and the general way in which the experiments are carried out are found in reference [13]. To give an example, previous studies using aqueous solutions of Na₂[PtCl₆] in the presence of nucleobases showed both the formation of clusters of one or more of the bases with [PtCl₆]²⁻ upon ESI, with the cluster UV photochemistry then being studied in the mass spectrometer via laser spectroscopy [8]. Previous work using a similar instrument to investigate the photochemistry of [PtCl₆]²⁻ provided evidence for photochemically activated redox processes generating chloroplatinate anions of Pt^V, Pt^III, and Pt^II, accompanied by the formation of both chlorine radicals and chloride anions via dissociation, leading to chlorometallate(II) anions [14].

Given that in the present system, both calculation and experiment show photogeneration of Pt^III on irradiation of solutions of [PtCl₆]²⁻, which can subsequently lead to Pt^II, there was confidence that these experiments would mimic conditions of the bulk photolysis preparations that had been carried out. Indeed, similar evidence has been observed for Ru carbonyl complexes with gas-phase photolysis mirroring solution-phase photolysis [15].

The positive-ion ESI mass spectrum of an unirradiated solution of [Bu₄N]₂[Pt^IVCl₆] in acetone shows the precursor ion at m/z 1135 associated with the cluster ion {[Bu₄N]₃[Pt^IVCl₆]}⁺ and a fragment at m/z 242 corresponding to {Bu₄N}⁺ (Figure S1). The negative-ion ESI mass spectrum (Figure S2) depicts the precursor ion at m/z 926 associated with {[Bu₄N]₂[Pt^IVCl₆]Cl}⁻ with its main fragment at m/z 649—{[Bu₄N][PtCl₆]}⁻.

Irradiation was carried out at wavelengths in the range of 220 to 270 nm, and evidence from the resulting mass spectra in both the positive and negative ion modes showed the formation of platinum(II); an example from the positive mode is shown in Figure 2 (other examples in Figures S3–S5). Thus, {[Bu₄N]₃[PtCl₆]}⁺ was found to photofragment giving {[Bu₄N]₃[Pt^IICl₄]}⁺ (with the corresponding ion {[Bu₄N][Pt^IICl₄]}⁻ being seen in the negative ion spectrum). Note also that Pt^III was observed directly both as the {[PtCl₄]}⁻ anion and as {[Bu₄N]₃[Pt^IIICl₅]}⁺. These data are consistent with observations from the previous experiments using aqueous solutions of Na₂[PtCl₆], which photolysed [PtCl₆]²⁻ directly [8]. However, crucially, it was possible to detect two complexes invoked in the mechanistic proposal. Thus, zwitterionic complex 3 was observed as part of a cluster with m/z = 1061 that corresponded to {(Bu₄N)₂Cl[(Bu₃N)(C₄H₇)Pt^IICl₃]}⁺, while σ-bonded complex 1 was observed directly as {Bu₃N-C₄H₈Pt^IVCl₅}⁻ at m/z 372 (Figure S4). Finally, here, production of complex 5 from 4 produces the Bu₃N^+• radical cation, which would be expected to abstract a hydrogen in the medium to give [Bu₃NH]⁺, which was observed at m/z 186 (Figure S5).

With the ability to mimic conditions of the photolytic preparations carried out, these experiments provide valuable and compelling support for the mechanism proposed previously for this quite unique reaction.

2.2. Possible Reactivity of [PtCl₃(1-butene)]⁻ and [PtCl₃(2-butene)]⁻

One of the key ideas in the proposed mechanism is that the butyl fragment is functionalised in two steps and that in both of these it remains attached to a Bu₃N fragment—i.e., the formation of complex 2 and then 3, and also the formation and reaction of complex 4 (Figure 3). This pathway assumes that the initial C–H activation of Bu₄N⁺ occurs at a terminal carbon, leaving the modified Bu₄N⁺ with four C–N bonds. However, activation at a carbon closer to the nitrogen could conceivably have led to elimination of the alkene through the breaking of a C–N bond and the formation of [PtCl₃(η²-butene)]⁻. If this were the case, then further reaction would require activation of [PtCl₃(η²-butene)]⁻ by [PtCl₆]²⁻ in a second photochemical step to generate the product. So, depending on the way the elimination occurred, either [PtCl₃(η²-1-butene)]⁻ or [PtCl₃(η²-2-butene)]⁻ could be formed.

To investigate the viability of such a pathway, trichloroplatinate(II) complexes of 1-butene and of 2-butene were prepared as their PPN⁺ ((PPN is bis(triphenylphosphino)iminium − [N(PPh3)2]+)) salts in order to remove any reactivity associated with Bu₄N⁺. The salts were then dissolved in CD₂Cl₂ in a gas-tight NMR tube and irradiated before the ¹H NMR spectrum was recorded (CD₂Cl₂ was used owing to the much better solubility of the salt when compared with acetone). In both cases, after 5 min of irradiation, there was a small decrease in the intensity of the resonances associated with the coordinated alkene and the appearance of weak signals consistent with the free alkene (comparison with the chemical shifts in a solution of the free alkene). Interestingly, on standing after irradiation, the signals associated with the free alkene disappeared, and the intensity of the complex resonances was restored, implying re-complexation.

In the second experiment, [PPN]₂[PtCl₆] was added to a fresh solution of the alkene complex, and irradiation was carried out once more. In both cases, the resonances corresponding to the free alkene were more intense, and indeed, after 60 min, there were no signals from the starting alkene complex. However, after standing for 24 h, most of the intensity of the resonances associated with the starting complex was restored. The ¹H NMR spectrum also showed new, weak resonances in the region 3.5–3.8 ppm, but in the absence of any evidence of coupling to ¹⁹⁵Pt in the 2D spectra, it is assumed that these are some by-products, perhaps formed by the reaction of decomplexed alkene with [PtCl₆]²⁻.

Finally, here, a dichloromethane solution was prepared containing [PPN]₂[PtCl₆] and [PPN]₂[PtCl₃(1-butene)], which was then frozen, placed in an EPR cavity, and irradiated. The observed spectrum was compared with that obtained on performing an equivalent experiment irradiating [Bu₄N]₂[PtCl₆]. In the Pt region, the two spectra (Figure 4a) are in effect superimposable, which is consistent in both cases with the formation of [Pt^IIICl₅]²⁻ as identified previously (g = 2.408, a_Pt = 425 G). In addition, there is also a signal at g = 2.008 (Figure 4b), which is again overlaid with the signal from a photolysis of [Bu₄N]₂[PtCl₆]. While there are similarities, the two signals are evidently not the same, although that originating from the PPN⁺ salt does have a structure not unlike that arising from an N-based radical. While there appears to be little radical chemistry of the PPN cation (it tends to be used normally as an ‘innocent’ cation in conjunction with much more redox-labile metalate salts), there is a report [16] of a radical derived from an iminophosphorane dimer (Figure 5) with a_N = 2.6 G and a_P = −5.4 G. While ³¹P hyperfine is larger than that of ¹⁴N, it is nonetheless relatively small, and so it is not impossible that for two equivalent ³¹P, it will all merge to a single line, and a nitrogen radical would be observed, leaving open the possibility of a signal arising from a PPN-based radical.

While these reactions were carried out in dichloromethane on account of the better solubility of the reagents, some early experiments used acetone, and on one occasion, crystals of [PPN]₂[PtCl₄] grew from the solution where the reaction was not under constant volume (i.e., any decomplexing alkene could escape the reaction medium). The structure was solved using X-ray methods and is described below.

2.3. Possible Activation of Other Cations

2.3.1. Tetrabutylphosphonium—[Bu₄P]⁺

In common with tetraalkylammonium cations, the tetrabutylphosphonium cation can be deployed as a counter cation to anionic inorganic complexes to engender solubility in organic solvents. With (Bu₄N)⁺ identified as the source of the butadiene on photolysis of [Bu₄N][PtCl₆], it was of interest to determine whether the same chemistry might occur on irradiation of [Bu₄P][PtCl₆]. Thus, [Bu₄P]₂[PtCl₆] was prepared and photolysed in acetone under the conditions used with [Bu₄N]₂[PtCl₆] and, as a control, Bu₄PCl and [Bu₃PH][BF₄] were also irradiated separately under the same conditions.

The ¹H and ³¹P{¹H} NMR spectra of the post-irradiation solutions of Bu₄PCl and [Bu₃PH][BF₄] showed no change, whereas on irradiation of [Bu₄P]₂[PtCl₆], [PtCl₆]²⁻ was consumed, giving [PtCl₄]²⁻ (¹⁹⁵Pt NMR chemical shift), but no platinum(II)-olefin signals were observed. Furthermore, the post-photolysis ³¹P{¹H} NMR spectrum showed a signal at δ = 46 ppm corresponding to (Bu₄P)⁺. Unsuccessful attempts to isolate a product from the reaction mixture were made through crystallisation. This observation indicated the generation of active species from [PtCl₆]²⁻ under light to form the reduced species [PtCl₄]²⁻, however, the activation of the butyl going in the same manner as for the tetrabutylammonium cation did not occur.

This can be rationalised by reference to work by Oh et al., who studied reactions of tetraalkylphosphonium ionic liquids in CO₂ capture, in which the ionic liquid anion was a strongly basic amide (e.g., 2-cyanopyrrolide or 3-trifluoromethylpyrazolide) [17]. Under such conditions, it might reasonably be expected that a tetraalkylammonium cation would be unstable to deprotonation (recall that anhydrous Bu₄N⁺F⁻ is unstable with respect to elimination), but in these materials, even H/D exchange reactions were slow, and such exchange that did occur was exclusively at the hydrogens on the α-carbon. The liability of this hydrogen (compared to the β-hydrogen in alkylammonium cations) is related to the larger size of P compared to N, which then reflects a generally lower acidity for those hydrogens. Indeed, this last point is also shown by the chemical shift in the α-hydrogens, which is ca 3.7 ppm in [Bu₄N]⁺ and 1.65 ppm in [Bu₄P]⁺ [18].

2.3.2. Alkylammonium Cations—[Pr₄N]₂[PtCl₆], [Bu₄N]₂[PtCl₆] and [Pe₄N]₂[PtCl₆]

Having determined that the Bu₄P⁺ cation is unreactive under irradiation with [PtCl₆]²⁻, the question arises concerning the reactivity of other tetraalkylammonium homologues, as it seems clear that the reactivity depends on the use of an ammonium derivative. To this end, [PtCl₆]²⁻ salts of both Pr₄N⁺ and Pe₄N⁺ (Pe = pentyl) have been prepared and studied.

Preparative Study: Both [Pr₄N]₂[PtCl₆] and [Pe₄N]₂[PtCl₆] are readily prepared from the chloride salt of the cation and K₂[PtCl₆] in water, being isolated in quantitative yield. While [Pe₄N]₂[PtCl₆] showed high solubility in acetone in common with [Bu₄N]₂[PtCl₆], the solubility of [Pr₄N]₂[PtCl₆] was significantly lower, meaning that more dilute conditions were required in order to perform reactions with homogeneous solutions. Thus, in each case, an acetone solution of the salt was irradiated for 18 h, after which the acetone was removed, and the sticky solid that remained was treated with diethyl ether. However, in neither case was it possible to isolate a tractable product.

Solution NMR Studies: Given that no isolable product was obtained from irradiation of either [Pr₄N]₂[PtCl₆] or [Pe₄N]₂[PtCl₆], a solution NMR study was conducted on these two salts along with [Bu₄N]₂[PtCl₆]. In each case, an anaerobic solution of the Pt^IV salt in an NMR tube in d⁶-acetone was irradiated, and NMR spectra were recorded either at intervals during the 18 h photolysis or at the end. Of necessity, for reasons of solubility, the concentrations of the solutions containing [Pr₄N]₂[PtCl₆] were some ten times more dilute than those of the other salts. [Bu₄N]₂[PtCl₆] and [Pe₄N]₂[PtCl₆] are considered first and then compared with [Pr₄N]₂[PtCl₆].

For both salts, following the reaction by ¹⁹⁵Pt NMR spectroscopy (Figure 6) showed an immediate decrease in the intensity of the resonance associated with the [PtCl₆]²⁻ anion at δ = 377 ppm, which was accompanied by the formation of [PtCl₄]²⁻ at δ = −1420 ppm. All [PtCl₆]²⁻ was consumed by the end of the reaction. Trace amounts of [Pt₂Cl₆]²⁻ (δ = −1164 ppm) were also observed, although this also tended to have disappeared by the end of the reaction. In addition to these chloroplatinate species, resonances were also observed in the region of the spectrum where Pt-alkene complexes are found, and it is interesting that their formation seemed to lag behind loss of Pt^IV and formation of Pt^II. Attempts to quantify these changes were frustrated by the differing T₁ values for the different species.

Then, to probe the organoplatinum complexes, 2D-(¹⁹⁵Pt-¹H) NMR spectra of the photoreaction mixture were obtained. After investigating a range of 10–135 Hz, a ¹⁹⁵Pt-¹H coupling constant of 60 Hz was found to give the best results in these experiments, and all data (

Table 1. ¹⁹⁵Pt chemical shifts in the Pt^II–alkene region with correlated hydrogens observed in 2D-HMQC-¹⁹⁵Pt-¹H NMR spectra following photolysis of [Pr₄N]₂[PtCl₆], [Bu₄N]₂[PtCl₆] and [Pe₄N]₂[PtCl₆] in acetone.

[Pr4N]2[PtCl6] δ/ppm		[Bu4N]2[PtCl6] δ/ppm		[Pe4N]2[PtCl6] δ/ppm
195Pt	1H	195Pt	1H	195Pt	1H
−2567 *	4.4; 4.2; 3.4; 1.6	−2570 *	4.15; 3.45; 1.56	−2573 *	4.4; 4.3; 3.4; 1.6
−2530	5.6; 5.2; 1.5	−2567 *	4.39; 4.33	−2569 *	4.4; 4.3; 1.6
−2520	4.5; 4.4; 1.6	−2550	4.43; 4.18	−2559	4.5; 4.2; 1.5
−2431 *	5.7; 1.6	−2536	4.50; 4.38	−2555	4.4; 4.2; 1.6
		−2431	5.74; 1.58	−2543	4.8; 4.5; 4.2; 1.7
				−2521	4.5; 4.4; 1.6
				−2434	1.6

* Seen in both 1D and 2D spectra.

) are collected using this value. Beginning with [Bu₄N]₂[PtCl₆], the 2D-HMQC-¹⁹⁵Pt-¹H NMR spectrum of a photoreaction mixture obtained in acetone is presented in Figure S11. Four platinum resonances correlated to protons are observed, and two of the signals were also observed in the 1D-¹⁹⁵Pt{¹H} NMR spectrum. None of the signals corresponds to those of the isolated butadiene-platinum(II) complexes.

The signal at −2570 ppm is seen in the 1D-¹⁹⁵Pt{¹H} and in the 2D-¹⁹⁵Pt-¹H spectra and correlates with the hydrogen resonances at 3.4 and 1.56 ppm, noting that they could not be analysed in the 1D ¹H spectrum as they were weak and poorly resolved. The signal at 3.4 ppm is likely related to −NCH₂, indicating an olefin compound consisting of alkylammonium bound to a platinum(II) species, but the presence of ¹H-¹⁹⁵Pt coupling might suggest that this arises from an internal rather than a terminal alkene. In considering this possibility, the literature precedent for the formation of 3 is very strong, and so were an internal alkene to be formed, then it may well be via an isomerisation reaction. This is not at odds with the observation of the (Bu₃N)(C₄H₇)Pt^IICl₃ fragment found using photodissociation mass spectroscopy, as this technique would not discriminate between isomers. Of course, the possibility does exist that under the conditions employed, there is a pathway that would see C–H activation at other than the terminal carbon, which could in turn more easily lead to the formation of an internal alkene.

The remaining signals show ¹H-¹⁹⁵Pt coupling only into the coordinated alkene region (ca 4.0–4.5 ppm) of the ¹H spectrum, with all Pt resonances consistent with coordinated alkene, but none corresponds with chemical shifts observed for either the 1-butene or 2-butene complex. One resonance could, however, correspond to the monoplatinated diene complex 5.

To see if there was a dynamic process, such as an exchange occurring during spectral acquisition, a variable-temperature ¹⁹⁵Pt{¹H} NMR experiment was conducted, recording in the Pt-olefin area between 200 and 298 K (Figure S12). As predicted [19,20], the chemical shifts decreased by 40 ppm when the temperature lowered from 298 K to 200 K. Moreover, the peaks were broader and less intense on cooling, but the pattern remained the same, implying an absence of a dynamic process; the broad peaks perhaps being attributed to a decrease in solubility at lower temperature. When the temperature increased back to 298 K, the spectrum reverted to the original intensities and resolution.

Now considering [Pe₄N]₂[PtCl₆], the ¹⁹⁵Pt{¹H} NMR spectra (Figure S13) of the reaction mixture also showed a signal corresponding to [PtCl₄]²⁻ at −1425 ppm, indicating the reduction of [PtCl₆]²⁻ as found in the photolysis of [Bu₄N]₂[PtCl₆]. In addition, the 1D-¹⁹⁵Pt{¹H}-NMR spectrum showed resonances associated with olefin-platinum(II) complexes at −2573 and −2569 ppm, while the 2D-(¹⁹⁵Pt-¹H) spectra (Figure S14) showed additional signals at −2559, −2555, −2543 and −2521 ppm. In common with the spectra obtained on irradiation of [Bu₄N]₂[PtCl₆], one resonance (–2573 ppm) shows coupling between Pt and a signal at 3.4 ppm, which we have tentatively assigned as belonging to Pt bound to an internal alkene that remains bound to nitrogen. As for the other Pt signals, they are all coupled to ¹H resonances in the range 4.0–4.5 ppm—indicative of coordinated alkene hydrogens—as well as a resonance at ca 1.6 ppm, which, by comparison with the spectra obtained for the complexes of 1-butene and 2-butene, could arise from either a CH₂ or CH₃ hydrogen adjacent to a coordinated double bond. Given the extra carbon in the chain in the [Pe₄N]⁺ cation, then the possibility exists for more isomeric forms, either of a coordinated N-bound or free alkene, consistent with the similarities in the chemical shifts in the species observed after reaction of the two different cations. Indeed, the Supporting Information shows the results of quantum chemical calculations on the relative stability of the different possible dinuclear diene products.

[Pr₄N]₂[PtCl₆] turned out to be much less soluble in acetone than the related Bu₄N⁺ or Pe₄N⁺ salts, so that only a fraction of the material was in solution at the beginning of the reaction. If, however, the photolysis was continued using what was in effect a solution and a suspension of the complex, then a homogeneous solution did, in due course, result. However, this led to rather long reaction times, and so experiments were instead conducted at concentrations some ten times lower. This presented challenges in terms of sensitivity in NMR experiments and, as a result, many signals present in the ¹H NMR spectra were simply too weak to allow interpretation. Nonetheless, useful data could be obtained from both 1D ¹⁹⁵Pt{¹H} and 2D ¹⁹⁵Pt–¹H spectra.

Thus, post-irradiation 1D ¹⁹⁵Pt{¹H} spectra showed the presence of [PtCl₄]²⁻ (δ = −1425 ppm), an unidentified signal at −1631 ppm, and two signals in the Pt^II-alkene region (δ = −2430 and −2567 ppm). The 2D ¹⁹⁵Pt–¹H spectra (Figure S16) showed correlation of the resonance at −2567 ppm with ¹H resonances in the region of coordinated alkene (δ ≈ 4.4 ppm), next to nitrogen (δ ≈ 3.4 ppm), as well as those from hydrogen atoms attached to a saturated carbon (δ ≈1.6 ppm). This implies the zwitterionic complex [Cl₃Pt⁻(H₃CCH=CHN⁺Pr₃)] with internal alkene. This is consistent with the formation of a σ-alkyl complex analogous to 2, followed by β-hydrogen elimination to generate the analogue of 3.

The resonance at −2430 ppm correlated weakly with a ¹H resonance at δ ≈ 5.7 ppm and again with one at δ ≈ 1.7 ppm; its origin is currently less clear.

2.4. EPR Study of Frozen Solutions

The EPR spectra of photolysed, glassy solutions of each of the three salts dissolved in CH₂Cl₂ at 120 K are given in Figure 7. The signals in the organic region with g = 2.013 and arising from a N-based cation are to all intents and purposes the same, while at lower field a signal is seen corresponding to paramagnetic platinum(III). For the Pe₄N⁺ and Bu₄N⁺ salts g = 2.402 with a(¹⁹⁵Pt) = 1560 and 1590 MHz, while for the Pr₄N⁺ salt, there are two signals with g = 2.393 and 2.463 and a(¹⁹⁵Pt) = 1500 and 1430 MHz, respectively. The former would seem to be the same species as found for the other two salts, while the latter is new and of unclear origin.

2.5. Molecular Structures of [PPN]₂[PtCl₄] and of [Pr₄N]₂[PtCl₄]

Crystals of the PPN⁺ salt were obtained as an acetone solvate and were twinned, crystallising in the P–1 space group and refined to an R-factor of 5.3% (CCDC: 2477527), while those of the Pr₄N⁺ salt in the monoclinic space group C2/c were refined to an R-factor of 3.1% and were solvent-free (CCDC: 2477528). In [PPN]₂[PtCl₄] there are two 180° trans-Cl–Pt–Cl angles and a very small deviation from orthogonality (cis-Cl–Pt–Cl angles = 89.79(4)° and 90.21(4)°), while for [Pr₄N]₂[PtCl₄] the trans Cl–Pt–Cl angles are 180.0° and 179.61(4)° with cis angles of 89.805(19)° and 90.195(19)°. Curiously, while for [PPN]₂[PtCl₄] the Pt–Cl distances are very similar at 2.3096(11) Å and 2.3020(11) Å (symmetry-related pairs) and comparable with the three other structures of the [PtCl₄]²⁻ anion held in the Cambridge Crystallographic Database (846887, 1298726, 126477), [21,22,23] in [Pr₄N]₂[PtCl₄] they are appreciably longer at 2.3459(10) Å, 2.3669(10) Å and 2.3211(8) Å (Cl₁–Pt–Cl₃ lies on a two-fold axis).

Implementing Olex2 [24], the structure was solved with the Superflip [25,26,27] structure solution program using Charge Flipping and refined with the ShelXL [28] refinement package using Least Squares minimisation. Crystallographic data are found in Table S1 in the Supporting Information.

In both structures, the [PtCl₄]²⁻ sits in a ‘pocket’ (Figure 8) defined by six cations (plus two molecules of acetone for [PPN]₂[PtCl₄]). A cation pocket in [Pr₄N]₂[PtCl₄] is defined by three tetrachloroplatinate(II) anions, whereas for [PPN]₂[PtCl₄], two cations are located in a pocket formed of six tetrachloroplatinate(II) anions and four acetones of solvation. In both cases, there are contacts at ca 2.8 Å with hydrogen atoms of the respective cation.

3. Materials and Methods

3.1. Instrumentation

3.1.1. NMR Spectroscopy

¹H NMR spectra were recorded using Jeol (Tokyo, Japan) ECS400 and Jeol ECX400 spectrometers operating at 400 MHz (¹H). ¹H (500 MHz), ³¹P{¹H} (202.4 MHz), ²D NMR spectra (76.8 MHz) and ¹⁹⁵Pt{¹H} (107 MHz) spectra were recorded on Bruker (Billerica, MA, USA) Avance 500 spectrometer. Two-dimensional ¹⁹⁵Pt-¹H and ¹⁵N-¹H NMR spectra were acquired via heteronuclear zero and double quantum coherence with decoupling during acquisition using gradient pulses for selection. The processing of all spectra was carried out using MestreNova software. For ¹H-NMR, the residual protic solvent was used as the internal standard (CDCl₃: 7.26 ppm, CD₂Cl₂: 5.32 ppm, CD₃COCD₃: 2.04 ppm), for the ¹⁹⁵Pt-NMR spectra were referenced to K₂[PtCl₆] in D₂O.

3.1.2. Electron Paramagnetic Resonance Spectroscopy

EPR spectroscopy was performed using a JEOL JES-RE1X-ESR spectrometer equipped with a 100 W Mercury lamps without a filter (λ > 250 nm). A sample of a solution of the analyte was loaded into a flat, quartz cell. A background spectrum was recorded at room temperature followed by the spectrum of sample at 120 K with a sweep time of 120 s and time constant of 0.3 s. At 176 K or above, no signals were observed. Before sample analysis, a background was recorded at an identical temperature over a wide range where the sweep width was 750 G and centre of the field was 3254 G. The internal standard was di(phenyl)(2,4,6-trinitrophenyl)iminoazanium (DPPH) with a g value of 2.0036. Parameters of the analysis and observed g value of samples are showed in Table S3. The spectra were processed using the EasySpin toolbox [29].

3.1.3. UV-Mass Spectrometry

Experiments were performed using a modified Bruker Esquire 6000 quadrupole ion trap mass spectrometer. The mass spectrometer was modified for the laser experiments by drilling holes (1 mm) in the ion trap ring electrode to allow laser access [13]. The source of UV photons for the laser spectroscopy experiments was from an Nd:YAG (Powerlite) pumped OPO (Panther Ex), producing ~2 mJ across the range 220–280 nm. (Bu₄N)₂[PtCl₆] dissolved in water was prepared for the electrospraying.

3.2. ¹H NMR Spectra from the Reaction of [PPN]₂[PtCl₆] with [PPN][PtCl₃(1-butene)]⁻ or [PPN][PtCl₃(2-butene)]

To demonstrate the occurrence of the decomplexation, the mixture of the 1-butene-platinum(II) and hexachloroplatinate(IV) complexes in dichloromethane solution was irradiated in a Young’s NMR tube and the reaction was monitored using ¹H NMR spectroscopy. The free 1-butene was removed using the freeze-pump-thaw method −116 °C, at which temperature, dichloromethane freezes whereas 1-butene is in the liquid phase. The ¹H-NMR spectrum of the solution was then recorded and showed roughly about 50% reduction of the integration corresponding to the hydrogen signals of free 1-butene. The observation demonstrated the removal of 1-butene through freeze-pump-thaw and implied the decomplexation of 1-butene-platinum(II) to free 1-butene. On heating of the mixture of the [PtCl₃(1-butene)]²⁻ and [PtCl₆]²⁻ in dichloromethane at 40 °C for 48 h under the dark conditions, the decomplexation was absent implying the important role of light in the process. Note that (Figure S7) there is no change in the ¹H NMR spectrum on simply applying vacuum in the absence of irradiation.

3.3. Quantum Chemical Calculations

In order better to understand the complexes that may result from the reactions using the tetrapentylammonium cation, DFT calculations were undertaken to find the conformers and isomers that may form preferentially. In principle, six such structures are possible (Figure S17), although as we have shown previously with closely related complexes of butadiene, not all of the possible structures exist separately.

The geometries were optimised at the M06/def2-TZVPP [30,31] level of theory with an effective core potentials (ECP) used for platinum atoms using Gaussian 16 package [32]. Calculated vibrational frequencies contained no imaginary values showing that each optimised geometry corresponds to a minimum on the respective potential energy surface. The calculated structures (S1, S3, S5 and S6) are shown in Figure S18 and the corresponding geometries with Cartesian coordinates of atomic positions are given in the separate coordinates file.

3.4. Synthesis

Salts with a tetrabutylammonium cation were prepared as described earlier.[2]

3.4.1. Tetrapropylammonium, Tetrapentylammonium and Tetrabutylphosphonium Hexachloroplatinate(IV)

These salts are prepared by stirring at room temperature and in the dark a suspension of potassium hexachloroplatinate (2.37 mmol) in acetone (15 cm³) and then adding the relevant cation as its chloride salt (4.74 mmol) as a solid in small batches. Once addition was complete, stirring continued overnight to afford an orange solution and a colourless precipitate. The solution was filtered in vacuo to remove the precipitate and then the solvent was removed resulting in an orange precipitate, which was dried in vacuo to give a crystalline orange solid. Isolated yields were effectively quantitative.

Tetrapropylammonium hexachloroplatinate(IV). Anal. calc. for C₂₄H₅₆N₂Cl₆Pt: Calc.: C = 36.93, H = 7.23, N = 3.59%. Found: C = 36.75, H = 7.20, N = 3.47%. ¹H NMR, δ (400 MHz, d6-acetone): 1.02 (24 H, t, -CH₃), 1.89 (16 H, m, -CH₂-), 3.48 (16 H, m, -NCH₂-). IR (νPt-Cl): 316 cm⁻¹. ¹⁹⁵Pt NMR: δ = 236 ppm.

Tetrapentylammonium hexachloroplatinate(IV). Anal. calc. for C₄₀H₈₈N₂Cl₆Pt: Calc.: C = 47.81, H = 8.83, N = 2.79%. Found: C = 47.57, H = 8.75, N = 2.71%. ¹H NMR, δ (500 MHz, d6-acetone): 0.90 (24 H, t, -CH₃), 1.39 (32 H, m, -CH₂-CH₂), 1.84 (16 H, m, -CH2), 3.49 (16 H, m, -NCH₂-). ¹⁹⁵Pt NMR: δ = 375 ppm.

Tetrabutylphosphonium Hexachloroplatinate(IV). Anal. calc. for C₃₂H₇₂P₂Cl₆Pt: Calc.: C = 41.48, H = 7.83%. Found: C = 41.92, H = 7.75%. ¹H NMR, δ (500 MHz, d6-acetone): 0.95 (24 H, t, -CH₃), 1.54 (16 H, m, -CH₂), 1.66 (16 H, m, -CH₂), 2.51 (16 H, m, -PCH₂-). ¹⁹⁵Pt{¹H} NMR: δ = 373 ppm. ³¹P{¹H} NMR: δ = 33.6 ppm.

3.4.2. Photolysis of Analogous Hexachloroplatinate(IV) Complexes

The method and equipment used for the irradiation of the analogous complexes was identical to the one employed to irradiate (NBu₄)₂[PtCl₆] complex described previously. The photolysis experiments were carried out in Young’s NMR tubes for followed by ¹H and ¹⁹⁵Pt{¹H} NMR spectroscopy. Quantities of the starting materials used are tabulated below (

Table 2. Amount of starting materials for the photolysis of analogous hexachloroplatinate(IV) complexes.

Substrates	Quantities
(Pe4N)2[PtCl6]	21.30 mg (0.02 mmol in dry acetone (1 cm3)
(Pr4N)2[PtCl6]	14.67 mg (0.02 mmol) in dry acetone (12.5 cm3)
(Pr4N)2[PtCl6]	3.57 mg (0.0045 mmol) in CD2Cl2 (0.5 cm3)
(Bu4P)2[PtCl6]	8.24 mg (0.008 mmol) in d6-acetone (2 cm3)

).

3.4.3. Irradiation of [PtCl₃(butene)]− Complexes

The method and equipment used for the irradiation of the [PtCl₃(butene)]⁻ complexes were identical to those employed to irradiate (Bu₄N)₂[PtCl₆] described previously. The photolysis experiments were carried out in Young’s NMR tubes and followed by ¹H and ¹⁹⁵Pt{¹H} NMR spectroscopy. Quantities of the starting materials used are tabulated below (

Table 3. Descriptions quantities of starting materials used and conditions of reactions.

Substrates	Quantities
(PPN)[PtCl3(2-butene)]	9.14 mg (0.01 mmol) + (PPN)2[PtCl6] (14.50 mg, 0.01 mmol) in CD2Cl2 illuminated with λ > 305 nm
(PPN)[PtCl3(1-butene)]	9.01 mg (0.01 mmol) + (PPN)2[PtCl6] (13.53 mg, 0.01 mmol) in CD2Cl2 illuminated with λ > 305 nm
(PPN)[PtCl3(1-butene)]	8.19 mg (0.013 mmol) + (PPN)2[PtCl6] (15.34 mg, 0.016 mmol) in CD2Cl2 heated under reflux in the dark.
(Bu4N)[PtCl3(1-butene)]	18.56 mg (0.03 mmol) in d6-acetone illuminated with λ > 305 nm.

). Control reactions in the dark were also carried out.

4. Discussion and Conclusions

Key to this work is the photoactivity of [PtCl₆]²⁻, which generates Pt^III species and Cl^• and leads to reduction to Pt^II as shown by studies in the 1970s [33,34]. Among more recent studies on the photochemistry of Pt^IV complexes by Gelbov and co-workers, [35,36,37,38] they reported studies of the stationary photolysis and flash photolysis of both [Bu₄N]₂[Pt(NO₃)₆] and [Bu₄N]₂[PtCl₆] dissolved in acetonitrile or chloroform, respectively. In both cases and by analogy with the earlier work, Pt^III is generated along with a radical derived from the ligand (NO₃^• or Cl^•, respectively), ultimately generating Pt^II, yet despite both complexes having Bu₄N⁺ as the counter cation, no activation was reported [39,40].

Therefore, to investigate this reactivity further and, in so doing, attempt to find further evidence supporting the proposed mechanism, photodissociation photodetachment mass spectrometry proved invaluable as it was able to identify solution species that had been proposed mechanistically, some of which were also identified by NMR spectroscopy.

Likewise, another crucial observation was that of the lack of reactivity of trichloroplatinate(II) complexes of 1-butene and 2-butene, which also provides support for the regiospecificity suggested by the mechanism.

Against these observations, perhaps the most intriguing aspect of the study centres around the photoreactivity of the tetraalkylammonium salts as studied by ¹H and ¹⁹⁵Pt NMR spectroscopy and by EPR spectroscopy. These studies showed that there is commonality between the signals observed on irradiation of the different salts and, where there are differences, then at a qualitative level they can be rationalised according to the different lengths of the alkyl chain bound to nitrogen.

Pulling all of these observations together allows for a more coherent understanding to emerge. Thus, the photodissociation mass spectrometry studies of [Bu₄N]₂[PtCl₆] are consistent with EPR spectra in showing the presence of (photogenerated) platinum(III) in addition to platinum(II), and this is consistent with the known photochemistry of [PtCl₆]²⁻. The mass spectrometry studies also show the presence of both unreacted platinum(IV) and of platinum(IV) σ-bound to the functionalised alkylammonium (2). Further, the results show the presence of zwitterionic η²-alkene complexes akin to 3 or an isomer thereof.

Curiously, complex 2 is not seen in any of the NMR spectra (signal would be expected at ca −700 ppm in the ¹⁹⁵Pt spectrum [41]), but resonances in the alkene region of the spectra viewed in conjunction with 2D ¹H-¹⁹⁵Pt data are consistent with Pt-alkene complexes. Furthermore, for each salt studied, there is a resonance that shows evidence of Pt coupling to a methylene hydrogen that is bound to nitrogen (δ ≈ 3.4 ppm in the ¹H spectra), which suggests a Pt complex of an isomer of 3 (or related species where the cation is [Pr₄N]⁺ or [Pe₄N]⁺). Other resonances are consistent with coordination to an alkene as found in 3, although it is not possible unequivocally to rule out that one or more species arise from complexation to free alkene. Another important observation is that there are more Pt-alkene species as the cation chain length increases from Pr to Pe, which speaks both to the possibility of the internal alkene isomerisation mentioned, plus the possibility of ‘free alkene’ complexes where the hydrocarbon fragment has broken its link to the nitrogen centre. Therefore, while unable to provide support for each step individually, when taken together, the data above are entirely consistent with the proposed mechanism.

However, one rather key observation is absent. Thus, where the starting material is [Bu₄N]₂[PtCl₆], chemical shift and coupling constant data for the isolated butadiene-containing product (1, Figure 1), including its isomeric forms, have been recorded and reported previously [3]. However, in none of the post-irradiation spectra obtained using [Bu₄N]₂[PtCl₆] is there any evidence of the product having formed and simply waiting to be precipitated out of solution. Indeed, this is true for experiments conducted by photolysis in NMR tubes, photolysis experiments conducted on a more preparative scale in larger photolysis tubes, and even the very early experiments conducted in more conventional glassware with adventitious ambient illumination and stirring, both with and without heating. It seems, therefore, that on the addition of diethyl ether to post-reaction solutions using [Bu₄N]₂[PtCl₆] as starting material, the product forms. This is not to imply chemical reactivity on the part of the ether anti-solvent, rather simply to observe that its addition and the presence of the different species in solution lead to the formation of the bimetallic butadiene complex. It is also important to recall here that isolated yields of the product are ca 70%, so that this is not a minor side-product of some other reaction. What this suggests is that, at least for [Bu₄N]₂[PtCl₆], whatever is present in solution, the bimetallic product complex 1 represents a thermodynamic minimum and so during crystallisation, this product forms preferentially from the solution species.