Synthesis and Characterization of [PdAg 20 {S 2 PR 2 } 12 ], R = O i Pr (2a), R = O i Bu (2b), R = Ph (2c)
Beforehand, we have synthesized and structurally characterized the thermodynamically stable alloy [PdAg20{S2P(OnPr)2}12] (1). This cluster can be formally regarded as a centered icosahedral [Pd@Ag12]4+ 8-electron superatomic core (with 1S2 1P6 1D0 superatomic configuration) passivated by an outer shell made of eight Ag+ and twelve monoanionic dithiophosphate (dtp) ions in such a way the complete PdAg20 metallic kernel is lowered to ideal C2 symmetry and the whole NC to C1.32 1 is robust, yet the liability of its protecting ligands tempted us to study the ligand exchange (LE) behaviour in order to produce new NCs. As shown in the Scheme 1, the treatment of 1 with 12 equivalents of NH4[S2P(OiPr)2] at -20 ºC in tetrahydrofuran (THF) for 2 minutes led to the formation of [PdAg20{S2P(OiPr)2}12] (2a) in 70% yield within an hour. Alternatively, the same compound was produced more conveniently by direct archetypal one pot synthetic method in moderate yield (41%) (See Experimental section). In parallel to the synthesis of 2a, compound [PdAg20{S2P(OiBu)2}12] (2b) was synthesized via co-reduction methods in 40% yield. Compound [PdAg20{S2P(OPh)2}12] (2c) was synthesized via the LE method in 65% yield (Experimental section). All NCs (2a-c) have been characterized by positive-mode ESI mass spectrometry, 31P{1H} and 1H NMR (see Supporting information, Figure S1-S7).
Upon the replacement in 1 of the dithiophosphates ligands having linear alkyl chain (n-propyl) with their branched derivatives (di-isopropyl dithiophosphates), the 31P{1H} nuclear magnetic resonance (NMR) spectrum in CDCl3 displays a signal shift from 104.9 ppm to 101.66 ppm at room temperature (Figure S1 and S8). The 1H NMR spectrum of 2a in CDCl3 shows two set of signals with a multiplet ranged at δ = 4.97–4.85 ppm (corresponding to the –OCH groups) and a doublet ranged at δ = 1.35–1.33 ppm (corresponding to –(CH3)2), in an integration ratio of 1:6 which is clearly attributed to the iPr groups (Figure S2).
The ESI mass spectrum (positive-ion mode) was recorded to identify the molecular formula of 2a. The spectrum reveals a prominent band corresponding to [2a + Ag]+ at m/z 4931.19 (calcd. 4930.97), and its simulated isotopic pattern is in good agreement with the experimental one (Fig. 1). The position of the molecular ion peak in 2a matches exactly with its parent NC 1, signifying the retention metal atomicity upon LE. Moreover, the UV-vis absorption spectrum of 2a features the same absorption pattern (384, 436 nm) as its parent NC 1. Thus, from the above spectroscopic data obtained in solution state, one would presume that the structure of 2a is the same as 1.
Similarly, the 31P{1H} NMR spectrum displays one type of resonance for 2b (δ = 103.8 ppm) and for 2c (δ = 63.1 ppm). The 1H NMR spectra of 2b and 2c displayed three and two types of resonances, corresponding to iso-butoxy and phenyl groups, respectively. Further, the ESI mass spectra of 2b and 2c show prominent bands corresponding to [M + Ag]+ at m/z 5267.64 (Calcd. 5267.62) and [M + 2Ag]2+ at m/z 2628.02 (Calcd. 2628.37), respectively. In order to elucidate the structure of these nanoalloys (2a-c), single crystals X-ray diffraction studies were undertaken. We were successful to crystallize 2a and 2b. The details of their X-ray structural analysis were discussed below. All of our attempts to crystallize 2c failed.
Single crystals of suitable quality for X-ray diffraction for 2a and 2b were grown by crystallization from diffusion of hexanes into a concentrated dichloromethane solution at -4°C within couple of weeks. Surprisingly, the resulting solid-state structures unveil different configuration of the outer shell which protects the 8-electron [Pd@Ag12]4+ core, as illustrated in Fig. 2 compared to that of 1.32 In particular, the arrangements of the 8 Ag+ capping atoms around the centered icosahedral core differs from that in 1, as one can see in Fig. 2 (from Fig. 2b → 2d → 2f). Whereas in both 1 and 2a NCs the PdAg20 skeleton adopts pseudo-C2 symmetry; that of 2b the PdAg20 skeleton adopts pseudo-D3 symmetry (Figure S9). The twelve dtp ligands in 2a are equally distributed on both sides of the C2 axis (Figure S9). They are coordinated to both capping and icosahedral silver atoms (Agcap and Agico, respectively) in five different modes in a ratio of 1:1:7:1:2; bimetallic biconnectivity (η2: µ1, µ1), bimetallic triconnectivity (η2: µ2, µ1), trimetallic triconnectivity (η3: µ2, µ1), trimetallic tetraconnectivity (η3: µ2, µ2) and tetrametallic tetraconnectivity (η4: µ2, µ2) (Figure S10). Further the seven dtp ligands with trimetallic triconnectivity (η3: µ2, µ1), differ in the coordination to different combination of Agcap and Agico atoms except for a couple of dtp ligands (red box, in Figure S10). As in any 8-electron dtp- or dsep-protected M21 NC characterized so far, the eight Ag+ capping atoms in 2a lie in a nearly planar AgSe3 coordination mode, making locally stable 16-electron metal centers. With the 12 protecting ligands around the PdAg20 metal skeleton (Fig. 2c), the whole molecular symmetry of 2a is C1. On the other hand, the twelve dtp ligands in 2b are distributed in three spherical rows around the pseudo-C3 axis in 3:6:3 ratios (Figure S9). They bind to both capping and icosahedral silver atoms only through two coordination patterns: trimetallic triconnectivity and trimetallic tetraconnectivity (Figure S11), in such a way the whole NC ideal symmetry is reduced to C3. A similar C3 arrangement has been described in the related 8-electron NC [Ag21{S2P(OiPr)2}12]+.34
The inner icosahedral Pd@Ag12 cores of 2a and 2b are very similar to that of 1. The Pd-Ag radial bond distances average 2.755 Å, 2.767 Å for 2a and 2b, respectively (2.757 Å in 1) and the peripheral Agico-Agico and Agico-Agcap bond distances in 2a and 2b are also fairly similar to those of 1 (Table 2). Thus, the 8-electron nanoalloys 1, 2a and 2b whose compositions differ only by the nature of their alkyl substituents, can be considered as pseudo-isomers. The presence of different arrangements of their outer shells is likely the result of the slightly different steric factors of their alkyl chains in 1 and 2a.
Table 1
Spectroscopic data of compounds for 1, 2(a-c), 3 and 4.
Compound | 31P NMR(ppm) | UV-vis(nm) | Emission (nm)a | ESI-MS(m/z, M+) |
132 | 104.9 | 384, 436 | 748 | 4930.8 |
2a | 101.6 | 384, 436 | 741 | 4931.19 |
2b | 105.0 | 384, 436 | 732 | 5267.19 |
2c | 63.14 | 419, 486 | 669 | 2628.02 b |
3 | 67.17 | 410, 501 | 712 | 6055.77 |
4 | 74.8 | 408, 498 | 702 | 6055.88 |
aPhotoluminescence recorded in 2-Methyl tetrahydrofuran at 77K. bESI-MS peak corresponds to (M + 2Ag)2+ peak. |
[PdAg 20 {Se 2 P(O i Pr) 2 } 12 ], (3) and its 3( Pn ) solid-state structure
After successful isolation of the 2a-c NCs, it was indeed obvious to attempt the synthesis of their diselenophosphate (dsep) protected analogues via LE reactions. Compound 1 was treated with NH4[Se2P(OiPr)2] at -20 ºC in THF (Scheme 1). The reaction proceeded immediately as the color of the reaction mixture changed from brown red to purple (Figure S12). The positive-ion ESI-MS spectrum of reaction mixture displays a prominent band for molecular ion peak at m/z = 6055.77 (calcd. 6055.23) corresponding to [PdAg20{Se2P(OiPr)2}12 + Ag]+ (Figure S13).
In order to determine its molecular structure, much effort was devoted to obtain suitable crystals for single crystal X-ray diffraction. Several sets of crystallization with varied solvent combinations and in mutable temperatures ended up producing extremely bad quality crystals. Nevertheless, diffusion of hexane into a saturated acetone solution of the reaction mixture kept at -10°C yielded proper single crystals within a week. The crystals of 3 obtained from this low temperature crystallization were dissolved in d6-acetone and subjected to 31P{1H} and 1H{31P} NMR studies. The 31P{1H} NMR spectrum at ambient temperature shows a single resonance at δ = 68.16 ppm (161.9 MHz, d6-acetone) flanked with two set of satellites (1JP−Se = 604.51 and 710.40 Hz) (Figure S14). 1H{31P} NMR spectrum shows characteristic signals of isopropyl ligands of di-isopropyl diselenophosphates (Figure S15).
Single crystals obtained were subjected to the X-ray diffraction study. Their analysis reveals that 3 crystallize in Pn space group. Its solid-state structure is labeled 3(Pn) in the following. It is shown in Fig. 3 and exhibits a Pd-centered icosahedral Ag12 core inscribed in a cube made up of 8 capping Ag atoms, in such a manner that the entire Pd@Ag12@Ag8 framework attains ideal Th symmetry. The whole metal kernel is protected by 12 dsep ligands situated on the 12 edges of the cube, in such a way that the whole NC ideal symmetry is reduced to T. The detailed molecular structure of 3(Pn) is identical to that of 3a, discussed in the next section below.
It should be also mentioned that the molecularly pure as-synthesized NC 2a also was used as starting precursor for LE reaction in order to produce 3. Therefore, the reaction of 2a with NH4[Se2P(OiPr)2] at -20 ºC in THF was performed (Scheme 1). Likewise, in the transformation from 1 to 3 the solution undergoes an instant colour change from brown to purple. The work up of the reaction mixture was done immediately. The 31P{1H} NMR spectrum of the reaction mixture exclusively shows single resonance at δ = 68.16 ppm in d6-acetone, the same resonance as observed in 31P{1H} NMR spectrum of 3. Thus, the transformation from 2a to 3 was confirmed by 31P NMR spectroscopy.
The 3( P 3 1 c ) solid-state structure of [PdAg 20 {Se 2 P(O i Pr) 2 } 12 ]
Single-crystals of 3 could also be obtained by slow diffusion in hexane into the saturated acetone solution of reaction mixture at ambient temperature. Their X-ray analysis reveals that in such conditions 3 crystallizes in the P31c space group. This solid-state phase is labeled 3(P31c) in the following. It reveals an isomeric NC pair of [PdAg20{Se2P(OiPr)2}12] clusters (3a and 3b), co-crystallized in the unit cell in a 1:1 ratio, with T and C3 pseudo-symmetry, respectively (Fig. 4).33 The molecular structure of 3a (T symmetry) is the same as that of 3(Pn), as well as that of the previously reported isoelectronic monocationic [MAg20{Se2P(R)2}12]q+ (M = Ag or Au; R = OEt; q = 1: M = Pt; R = Oi/nPr; q = 0).20,21 The structural metrics of 3a and 3(Pn), are similar (Table 2). Their icosahedral Pd@Ag20 core embedded within a cuboid made of eight capping Ag atoms, resulting in a PdAg20 framework of Th symmetry, is shown in Fig. 3b-d and 4b. Their twelve dsep ligands display trimetallic triconnectivity (η3: µ2, µ1) bridging pattern with two capping Ag atoms (Agcap) and one icosahedral Ag atom (Agico), reducing the whole ideal NC symmetry to T. The molecular structure of 3b (C3 symmetry) is similar to that of 2b (see above) and [Ag21{S2P(OiPr)2}12]+.34 The differences in the positions of the outer capping Ag atoms in 3a and 3b, and their possible interchange pathway, is illustrated in Figure S16. To the best of our knowledge clusters 3a and 3b constitute the first pair of true isomers within the family of Se-protected NCs certified by X-ray crystallography. The Pd-Agico average distances in 3a and 3b are equivalent (2.758(10) Å and 2.754(10) Å, respectively), as well as their average Agico-Agico distance (2.901(9) Å and 2.896(10) Å, respectively). Thus, the structure of the Pd@Ag12 core in 3a and 3b is quite independent from the configuration of the outer sphere (see Table 2). The average Agico@Se distance in both 3a and 3b are larger than the Agcap@Se distances. The Se···Se bite distances in 3a and 3b are fairly similar (Table 2) and slightly shorter than those observed in [Ag21{Se2P(OEt)2}12]20 (3.697 Å) and [AuAg20{Se2P(OEt)2}12]20 (3.697 Å).
The two isomers assemble in a layer-by-layer mode. Each layer consists of pure 3a(T) or 3b(C3) (Fig. 5a). The T and C3 layer are alternately stacked along the [001] direction (Fig. 5b). The three-fold rotational axes of 3a and 3b are parallel to the c axis of the trigonal lattice. Finally, it is worth mentioning at this point that the isomer selectivity of the low temperature crystallization (3(Pn), T isomer) facilitates its further spectroscopic characterizations.
[PdAg20{Se2P(OnPr)2}12], (4)
Given the synthesis of 2a-3 via ligand-exchange-induced structure transformation (LEIST) route it is indeed inevitable not to synthesize another normal propyl alkyl chain analogue. Note that the precedence of structurally precise selenium protected alloy clusters is awfully inadequate. Thus, as shown in scheme 1, we have endeavoured the ligand replacement of dithiophosphates on 1 by diselenophosphates with linear alkyl chain (n-propyl). The reaction leads to the formation of [PdAg20{Se2P(OnPr)2}12] (4) in 75% yield. Its 31P{1H} spectrum in CDCl3 displays a signal at δ = 73.59 ppm flanked with two set of satellites (1JP−Se = 616.41 and 719.23 Hz) at room temperature (Figure S17). The 1H{31P} NMR spectrum of 4 in CDCl3 reveals three set of signals with multiplets ranged at δ = 4.03–4.02 ppm (corresponds to –OCH2 group), δ = 1.78–1.70 ppm (corresponds to –CH2) and at δ = 0.95 − 0.92 ppm (corresponds to –CH3) in an intigration ratio of 1:1:1.5, which is clearly attributed to nPr group of di-propyl diselenophosphate ligands (Figure S18). The ESI mass (positive-ion mode) spectrum shows a prominent band corresponding to [4 + Ag]+ at m/z = 6055.88 (calcd. 6055.23), and its simulated isotopic pattern is in good agreement with the experimental one (Figure S19). Based on these spectroscopic evidences, the molecular structure of 4 should adopt the same T arrangement as that of 3a. This is confirmed by the solid-state structure of 4 obtained from single-crystal X-ray diffraction (Fig. 3 and S20). Its structural metrics are similar to those of 3(Pn) and 3a (Table 2). Interestingly, 4 crystallize as a racemate in the P21 space group.
Table 2
Selected structural metrics (average (top line) and ranges (bottom line)) of compounds for 1, 2a-b, 3, 3a-b and 4.
Entry | Agico-Agico | Agico-Agcap | Agico-E | Agcap-E | E-E |
1 | 2.897 | 2.971 | 2.687 | 2.540 | 3.414 |
2.827–2.987 | 2.856–3.346 | 2.471–3.047 | 2.480–2.726 | 2.772–2.747 |
2a | 2.896(7) | 3.020(7) | 2.605(14) | 2.542(19) | 3.399 |
2.807(1)- 2.997(1) | 2.863(1)-3.287(1) | 2.486(4)-2.933(4) | 2.472(5)-2.651(4) | 3.304–3.456 |
2b | 2.893(6) | 3.014(5) | 2.542(2) | 2.506(1) | 3.400 (3) |
2.829(8)- 2.930(1) | 2.847(9)-3.204(7) | 2.480(3)-2.590(2) | 2.330(1)-2.590(3) | 3.380(4)-3.430(2) |
3 (Pn) | 2.902(11) | 2.949(100) | 2.683(10) | 2.614(15) | 3.688 |
2.845(2)-2.969(2) | 2.899(2)-3.005(2) | 2.666(3)-2.696(3) | 2.595(3)-2.639(3) | 3.655–3.704 |
3(P31c) | 3a | 2.901(9) | 2.950(8) | 2.668(7) | 2.607(10) | 3.665 |
2.841(2)-2.957(3) | 2.901(3)-2.989(2) | 2.662(4)-2.674(3) | 2.600(3)-2.617(3) | 3.646–3.691 |
3b | 2.896(10) | 2.965(9) | 2.739(8) | 2.607(12) | 3.668 |
2.845(3)-2.945(2) | 2.880(3)-3.123(3) | 2.628(3)-3.104(4) | 2.576(3)-2.673(3) | 3.653–3.694 |
4 | 2.893(2) | 2.949(2) | 2.668(2) | 2.618(2) | 3.698 |
2.833(2)-2.961(2) | 2.902(2)-3.009(2) | 2.630(2)-2.699(2) | 2.607(2)-2.637(2) | 3.677–3.721 |
Optical Properties of the title NCs
It is interesting to note that the side chain in dithiophosph(in)ate ligands can lead to the variance of photoluminescence properties. The differed alkyl chains such as n-propyl (1), i-propyl (2a), i-butyl (2b), have least variance and look reddish while the phenyl derivative (2c) which was only obtained by ligand exchange appear to be orange to the naked eye. The UV-Vis spectra of 1, 2a and 2b show similar broad optical absorption bands at 384 and 436 nm, the latter band being intense (see Table 1, Fig. 6a). On the other hand, the phenyl derivative 2c features different absorption bands (419 and 486 nm) where the former is found to be more intense (Fig. 6b). The absorption bands in 2c are red-shifted to their alkyl relatives. The change from alkyl to phenyl of the dtp substituents can alter the photoluminescence intensity. Compounds 1, 2a, and 2b show photoluminescence in solution at 77K. Their emission maxima in 2-methyl tetrahydrofuran (MeTHF) occur at λmax = 748 nm, 741 nm and λmax = 732 nm, respectively (Fig. 5a and Figure S21-S23). Cluster 2c is also emissive in solution state at 77K. Its emission maximum appears at 669 nm in MeTHF (Fig. 6b and Figure S23) which is blue shifted to its parent cluster 1.
The UV-vis spectra feature two major broad absorption bands for 3 (λmax = 410 and 501 nm) and 4 (λmax = 408 and 498 nm) (Figure S24) which are red shifted with respect to those observed in their parent cluster 1 (λmax = 384 and 436 nm) (Fig. 7a). Cluster 3 and 4 displays photoluminescence in solution at 77K where the emission maximum in 2-methyl tetrahydrofuran occurs at 712 and 702 nm, respectively which are slightly blue shifted with respect to those of its dithiophosphate analogue 1 (Fig. 7a and Figure S25).
Computational Studies of title NCs
In a recent DFT investigation on the alloying of dichalcogenolate-protected Ag21 species,35 we have shown that in the case of 8-electron NCs of the type [MAg20{dtp/dsep}12]±q (M = group 9 to group 12 metal), when M is a group 9 or 10 metal, it strongly prefers occupying the centre of the icosahedron, i.e., [M@Ag20{dtp/dsep}12]±q. The reason lies in the involvement of the nd(M) valence orbitals in the metal-metal bonding through their stabilization by the vacant superatomic 1D shell. Calculations on the T, C3 and C132 structures of [M@Ag20{dtp/dsep}12]±q indicated also a small energy differences between these structures, in particular between T and C3, independently from the nature of M. Calculations on the simplified model [PdAg20{Se2PH2}12] with a slightly different basis set as previously35 found the T isomer to be slightly more stable, both in total energy (ΔE = 3.7 kcal/mol) and free energy (ΔG = 0.2 kcal/mol), this last value being not significantly different from zero. Calculations on the less simplified model [PdAg20{Se2P(OMe)2}12] found similar results with ΔE = 3.7 kcal/mol and ΔG = 2.7 kcal/mol. Although calculations on the real clusters 3a and 3b were not performed owing to their large size, these results confirm our previous finding that the T and C3 structures are close in energy, with the T isomer tending to be slightly more favoured in the case of diselenolate ligands. The very small computed energy difference between the two isomers is fully consistent with their observation as co-crystallized species. The C1 structure adopted by compound 2a was also calculated in the case of the [PdAg20{Se2PH2}12] model. It was also found less stable than its T isomer (ΔE = 10.3 kcal/mol and ΔG = 4.8 kcal/mol). In the case of the dithiolate model [PdAg20{S2PH2}12], this energy difference is reduced (ΔE = 4.6 kcal/mol and ΔG = 0.0 kcal/mol), in agreement with the observation of 2a. They illustrate close similarities in the bonding situation of the various isomers, in full consistency with their closeness in energy. All these computed species have their three highest occupied orbitals of 1P nature, whereas the 1D level correspond the lowest vacant orbitals.
TD-DFT calculations on [PdAg20{S2PH2}12] (C1) and [PdAg20{Se2PH2}12] (T and C3), as models for 2a, 3a and 3b, provided the simulated UV-Vis spectra shown in Fig. 7b. They are in good agreement with their experimental counterparts (Fig. 7a). The low-energy band is of 1P → 1D nature and a comparison of Figs. 7a and 7b let to suggest that the T isomer of 3 might be the dominant species in solution.