Tiago A.
Fernandes
a,
Hana
Solařová
a,
Ivana
Císařová
a,
Filip
Uhlík
b,
Martin
Štícha
c and
Petr
Štěpnička
*a
aDepartment of Inorganic Chemistry, Faculty of Science, Charles University in Prague, Hlavova 2030, 12840 Prague 2, Czech Republic. E-mail: stepnic@natur.cuni.cz
bDepartment of Physical and Macromolecular Chemistry, Faculty of Science, Charles University in Prague, Hlavova 2030, 12840 Prague 2, Czech Republic
cDepartment of Organic Chemistry, Faculty of Science, Charles University in Prague, Hlavova 2030, 12840 Prague 2, Czech Republic
First published on 24th December 2014
The reaction of in situ generated 1′-(diphenylphosphino)-1-lithioferrocene with carbamoyl chlorides, ClC(E)NMe2, affords the corresponding (thio)amides, Ph2PfcC(E)NMe2 (E = O (2), S (3); fc = ferrocene-1,1′-diyl). These compounds as well as their analogues, Ph2PfcC(O)NHMe (4) and Ph2PfcC(O)NH2 (5), prepared from 1′-(diphenylphosphino)ferrocene-1-carboxylic acid (Hdpf) were studied as ligands for the Group 11 metal ions. In the reactions with [Cu(MeCN)4][BF4], the amides give rise to bis-chelate complexes of the type [Cu(L-κ2O,P)2][BF4]. Similar products, [Ag(L-κ2O,P)2]ClO4, are obtained from silver(I) perchlorate and 2, 4 or 5. In contrast, the reaction of AgClO4 with 3 produces a unique molecular dimer [Ag(3)(ClO4-κO)]2, where the metal centres are bridged by the sulfur atoms of the P,S-chelating thioamides. The reactions of 2–5 with [AuCl(tht)] (tht = tetrahydrothiophene) afford the expected gold(I)–phosphine complexes, [AuCl(L-κP)], containing uncoordinated (thio)amide moieties. Hemilabile coordination of the phosphinoamide ligands in complexes with the soft Group 11 metal ions is established by the crystal structure of a solvento complex, [Cu(5-κ2O,P)(5-κP)(CHCl3-κCl)][BF4], which was isolated serendipitously during an attempted crystallisation of [Cu(5-κ2O,P)2][BF4]. All of the compounds are characterised by spectroscopic methods, and the structures of several representatives of both the free phosphinoamides and their complexes are determined by X-ray diffraction analysis and further studied by DFT calculations and cyclic voltammetry.
During our studies3 on phosphinoferrocene carboxamides, we have also typically relied on the amide coupling reactions,4 employing 1′-(diphenylphosphino)ferrocene-1-carboxylic acid (Hdpf),5 suitable functional amines and conventional peptide coupling agents (route A in Scheme 1). Although this synthetic strategy proved very efficient, we felt that the search for alternative synthetic routes that are more straightforward and avoid the use of expensive stoichiometric reagents was still desirable. Thus far, we have demonstrated that phosphinoferrocene carboxamides can be synthesised equally well by lithiation of 1′-(diphenylphosphino)-1-bromoferrocene (1)6 and subsequent reaction of the lithiated intermediate with isocyanates (route B in Scheme 1).7
![]() | ||
Scheme 1 Synthetic routes to phosphinoferrocene carboxamides: conventional amidation (A) and lithiation/electrophilic quenching (B and C; E = O and S). |
In an attempt to extend this preparative strategy, we decided to replace isocyanates with carbamoyl chlorides (route C in Scheme 1).8 Although the choice of substituents is inherently limited in carbamoyl halides because of their high reactivity, we reasoned that a reaction of lithiated intermediates with these reagents9 could possibly offer an alternative direct route to phosphinoamides and their corresponding thioamides that do not require protection of the already present phosphine moiety from an undesired oxidation.10 In this regard, a practical synthesis of phosphine-thioamides is particularly attractive as it may provide access to this type of mixed-donor ligands and thus initiate investigations into their coordination properties, which still remain largely unexplored.11 To the best of our knowledge, there is only one report on the synthesis of a phosphine-thioamide donor via the rather unconventional Diels–Alder [4 + 2]-cycloaddition of N,N-dimethylthioacrylamide across 3,4-dimethyl-1-phenyl-1H-phosphole bonded to a Pd(II) centre.12 This solitary example markedly contrasts with the numerous studies that focus on the chemistry of phosphine-carbothioamides, Ph2PC(S)NR2.13
In this contribution, we describe the synthesis of a phosphinoferrocene carboxamide and thioamide via lithiation and electrophilic functionalisation of 1, and their model compounds obtained by the conventional amidation of Hdpf. The resulting hybrid ligands14 are structurally characterised through a combination of physicochemical and computational methods and further employed as donors for the soft Group 11 metal ions in order to investigate their coordination properties.
![]() | ||
Scheme 2 Preparation of phosphinoferrocene amide 2 and thioamide 3 from 1 and the corresponding carbamoyl halides. |
In view of the intended coordination study, the series of phosphinoamide donors was extended by the homologous secondary amide 4 (Scheme 3) and the known primary amide 1′-(diphenylphosphino)-1-(aminocarbonyl)ferrocene (5)7 for the purpose of comparison. The former compound was synthesised by the conventional amidation of Hdpf with methylamine in the presence of 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide (EDC) and 1-hydroxybenzotriazole (HOBt), resulting in an 87% yield after isolation by column chromatography. Amide 4 was further converted to the corresponding phosphine oxide (4O) and sulfide (4S) via standard oxidations with hydrogen peroxide and elemental sulfur, respectively.
![]() | ||
Scheme 3 Preparation of amide 4 and its corresponding P-oxide and P-sulfide. Legend: EDC = 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide, HOBt = 1-hydroxybenzotriazole. |
Amides 2–4 have been characterised by multinuclear NMR and IR spectroscopy, electrospray ionisation (ESI) mass spectrometry and elemental analysis. Phosphines 2–4 display singlets in their 31P{1H} NMR spectra at δPca. 17, close to that of Hdpf itself,5 while the signals of the P-oxidised derivatives appear shifted to lower fields (δPca. 32 and 43 for 4O and 4S, respectively).5,15 The 1H and 13C{1H} NMR spectra reveal signals typical for the 1′-(diphenylphosphino)ferrocenyl moieties. The amide resonances are observed at δCca. 170 for the amides and at δC 199 for thioamide 3. As a result of the limited molecular mobility typical for conjugated amides, the signals of the methyl substituents in the spectra of the tertiary amides are observed either as a broadened singlet (2) or a pair of non-equivalent signals (3) at room temperature. On the contrary, the 1H NMR signals of the methyl groups in the spectra of secondary amides 4, 4O and 4S are seen as NH-coupled doublets associated with quartets attributed to the NH proton at a lower field.
The type of amide pendant is manifested in the IR spectra, showing bands resulting from the C–N and CE16 stretching vibrations (2: 1502 and 1650 cm−1, 3: 1508 cm−1). The spectra of the secondary amides further display bands due to NH stretching modes above 3000 cm−1. Additional characterisation of 2 and 3 by DFT computations, UV-vis spectroscopy and by cyclic voltammetry are described below.
The molecular structures of 2, 3 and 3O are depicted in Fig. 1. Selected geometric parameters are summarised in Table 1. The ferrocene units in the structures of these tertiary amides exert the typical regular geometries with similar Fe–C distances and tilt angles below ca. 6° (maximum: 5.8(1)° for 3). The ferrocene cyclopentadienyl rings in 2 and 3 assume similar anticlinal eclipsed conformations that divert the substituents into mutually distant positions. The amide plane in 2 is rotated by as much as 47.4(2)° from an arrangement coplanar with its parent cyclopentadienyl ring (Cp1) with the NMe2 group pointing away from the ferrocene unit and the PPh2 substituent. The thioamide moiety in 3 is twisted considerably less (26.7(2)°) and adopts the opposite orientation with respect to the PPh2 moiety (i.e., with the CS bond more distant). In contrast, the ferrocene unit in 3O has a synclinal eclipsed conformation, which results in a rather compact structure in which both substituents are located on the same side of the ferrocene scaffold. Consequently, the rotation of the thioamide plane is increased to 41.8(2)° and the orientation of the C(S)NMe2 pendant unit is changed so that the more bulky NMe2 unit is directed away from the ferrocene unit (though on the same side as the phosphine substituent). Parameters pertaining to the amide/thioamide and (diphenylphosphino)-ferrocenyl moieties appear unexceptional in view of the data reported earlier for FcCSNH2,17 fc[CSNMe2]2,9a Hdpf and its P-oxide,5 Ph2P(O)fcCONHCy,7 and bromide 118 (Fc = ferrocenyl, fc = ferrocene-1,1′-diyl).
![]() | ||
Fig. 1 PLATON plots of the molecular structures of 2, 3 and 3O (for displacement ellipsoid plots, see ESI†). |
Parameter | 2 (E = O) | 3 (E = S) | 3O (E = S)b |
---|---|---|---|
a Definitions: Cp1 and Cp2 are the cyclopentadienyl rings C(1–5) and C(6–10), respectively. Cg1/2 denote their centroids. τ is the torsion angle C1–Cg1–Cg2–C6 and φ is the dihedral angle subtended by the amide unit (C11, E, N) and the plane of its parent ring Cp1.
b Further data: P![]() |
|||
Fe–Cg1 | 1.6462(8) | 1.6544(8) | 1.6413(7) |
Fe–Cg2 | 1.6464(8) | 1.6486(8) | 1.6402(7) |
∠Cp1, Cp2 | 2.8(1) | 5.8(1) | 4.12(9) |
τ | −151.1(1) | 143.5(1) | 71.8(1) |
C11![]() |
1.225(2) | 1.689(2) | 1.672(2) |
C11–N | 1.356(2) | 1.333(2) | 1.337(2) |
E![]() |
121.7(2) | 121.4(1) | 122.3(1) |
φ | 47.4(2) | 26.7(2) | 41.8(2) |
N–C24 | 1.460(2) | 1.465(2) | 1.468(2) |
N–C25 | 1.460(2) | 1.464(2) | 1.461(2) |
C24–N–C25 | 116.3(1) | 113.7(2) | 113.0(2) |
P–C6 | 1.820(2) | 1.811(2) | 1.788(2) |
P–C12 | 1.832(2) | 1.835(2) | 1.811(2) |
P–C18 | 1.841(2) | 1.839(2) | 1.808(2) |
Molecular structures of the secondary amides 4, 4O·CHCl3 and 4S are shown in Fig. 2. Principal geometric data are given in Table 2. The molecular parameters compare well with those reported for other structurally characterised secondary amides derived from Hdpf.19 Similar to the tertiary amides, the ferrocene units in the structures of the secondary amides are typical with tilt angles not exceeding ca. 5°. A most notable difference observed across the series is again associated with the mutual orientation of the ferrocene substituents, which are near synclinal eclipsed in 4 and 4O, staggered anticlinal in molecule 2 of 4S, or assume an intermediate conformation between anticlinal staggered and eclipsed anticlinal eclipsed (molecule 1 of 4S).
![]() | ||
Fig. 2 PLATON plots of the molecular structures of 4, 4O·CHCl3 and 4S (molecule 1). Labelling of the second independent molecule in the structure of 4S is strictly analogous. Displacement ellipsoid plots are available in the ESI.† The N–H⋯O and C–H⋯Cl hydrogen bonds in the structure of 4O·CHCl3 are shown as dashed lines. |
Parameter | 4 (E = void) | 4O (E = O1P)b | 4S (E = S1/S2)c |
---|---|---|---|
a The parameters are defined as for the tertiary amides (see Table 1). n.a. = not applicable. b The compound crystallised in the form of stoichiometric solvate 4O·CHCl3. c Data for the two structurally independent molecules (molecule 1/molecule 2). | |||
Fe–Cg1 | 1.6462(8) | 1.650(1) | 1.640(4)/1.662(4) |
Fe–Cg2 | 1.6420(7) | 1.641(1) | 1.643(4)/1.639(4) |
∠Cp1, Cp2 | 3.2(1) | 1.2(1) | 3.2(5)/4.7(5) |
τ | −82.6(1) | 71.3(2) | −162.3(5)/145.4(5) |
C11![]() |
1.242(2) | 1.233(3) | 1.222(6)/1.233(7) |
C11–N | 1.330(2) | 1.343(3) | 1.326(8)/1.309(7) |
O–C11–N | 122.1(2) | 123.3(2) | 123.6(5)/121.9(6) |
φ | 6.1(2) | 25.3(3) | 11.3(8)/13.6(7) |
N–C24 | 1.453(2) | 1.456(3) | 1.457(9)/1.45(1) |
P![]() |
n.a. | 1.495(2) | 1.951(3)/1.960(3) |
P–C6 | 1.822(2) | 1.785(2) | 1.785(8)/1.792(8) |
P–C12 | 1.835(2) | 1.809(2) | 1.826(9)/1.813(9) |
P–C18 | 1.839(2) | 1.809(2) | 1.819(7)/1.818(7) |
The rotation of the amide unit with respect to the parent cyclopentadienyl ring varies from ca. 6° in amide 4 to ca. 25° in 4O. However, these structural changes seem to be (at least partly) induced by different intermolecular interactions because, unlike the tertiary amides whose solid-state structures are essentially molecular,20 the molecules of the secondary amides associate in the solid state by means of hydrogen bonds formed by the NH hydrogens. Compounds 4 and 4S assemble into infinite chains consisting of molecules located around the crystallographic glide planes via N–H⋯OC hydrogen bonds (N⋯O = 2.835(2) Å for 4 and 2.797(6)/2.834(6) for molecules 1/2 of 4S). Conversely, the solvated phosphine oxide 4O forms an intramolecular hydrogen N–H⋯O
P bond towards the highly polarised21 phosphoryl oxygen (N⋯O = 2.838(2) Å) rather than the amide C
O moiety, while the C
O group is employed in binding the solvent molecule via the soft C–H⋯O interaction (Cl3C–H⋯O
C, C⋯O = 3.013(3) Å).
The LUMO, HOMO and two next molecular orbitals below HOMO are depicted in Fig. 3. In the case of 2, the HOMO and HOMO−1 show dominant contributions from d orbitals on Fe, while for 3, the HOMO consists mainly of non-bonding orbital located on sulfur (lone pair). The next two lower molecular orbitals of 3 are of similar nature as HOMO and HOMO−1 of 2 (similar to diagonal relationship), but with certain contribution from atomic orbitals located on the sulfur atom and with somewhat lower energies. This corresponds well with the lower ionisation potential and higher softness of sulfur with respect to oxygen. This principal difference in the structure of the highest occupied molecular orbitals is most likely responsible for the different electrochemical behaviour of 2 and 3 (vide infra).
![]() | ||
Fig. 3 Plots of LUMO, HOMO and two lower molecular orbitals of 2 and 3 showing contours at the ±0.05 a.u. level. |
Changes in electronic structure associated with the (formal) replacement of the amide oxygen with sulfur prompted us to investigate the representative amides 2 and 3 by UV-vis spectroscopy and by electrochemical methods. The UV-vis spectra (Fig. 4) comprise single bands (with a shoulder at lower energies) located at the foot of a more intense bands extending from the UV region. This band in the spectrum of 2 is observed at 445 nm, shifted slightly to lower energies as compared with ferrocene itself (440 nm; forbidden d–d transition).23 In the spectrum of 3, the absorption band is significantly red-shifted (458 nm) and also more intense, presumably owing to a more extensive conjugation.24
![]() | ||
Fig. 4 UV-vis spectra of 2 (blue line) and 3 (red line) recorded in 1,2-dichloroethane solutions (c = 5 × 10−4 M, optical path 10 mm). |
Cyclic voltammogram of amide 2 (Fig. 5) displays a one-electron oxidation at E°′ ca. 0.17 V vs. ferrocene/ferrocenium. The oxidation, which can be attributed to the FeII/FeIII couple (electron removal from HOMO located predominantly at the ferrocene unit, see above), is associated with some follow-up processes that render it quasi-reversible and also give to rise to additional redox waves at higher potentials. Nonetheless, chemical reactions of the electrochemically generated species are relatively slow because the ratio of the cathodic and anodic peak currents (ipc/ipa) significantly increases with increasing scan rate (see inset in Fig. 5), limiting to unity. Such behaviour resembles that of the parent acid Hdpf.5 The fact that the oxidation of the ferrocene unit is shifted to less positive potential than that of Hdpf (E°′ ca. 0.31 V in MeCN) is in accordance with the lower electron-withdrawing ability of the amide moiety as compared with the carboxyl group (cf. the Hammett σp constants: 0.36 for CONH2, and 0.45 for CO2H).25
The redox behaviour of thioamide 3 is much less clear-cut (Fig. 6). The compound undergoes an irreversible oxidation at ca. 0.02 V (anodic peak potential, Epa, is given), which is followed by several ill-defined irreversible oxidations that replace the original composite oxidative wave during the second and following scans (even at 1 V s−1). Such a response may well correspond with the properties of the HOMO orbital, which encompasses both ferrocene unit and the thioamide moiety.
For the sake of a simpler definition, the dihedral angle φ was replaced with the torsion angle C2–C1–C11–E (ψ). The energy profiles calculated as a function of this angle for FcCONH2 and FcCSNH2 (Fig. 7) show two equivalent minima corresponding to enantiomers. The maxima belong to conformations with amide groups perpendicular to the parent cyclopentadienyl rings, with the higher in energy corresponding to the conformation in which the NH2 unit is directed closer to the Fe atom. The practically coincident minima for both amides exhibit twists of the amide group of 18°. In the case of the more bulky N,N-dimethyl derivatives, FcC(E)NMe2, the twisting increases to 35° and 37° for E = O and S, respectively, presumably for steric reasons. The former value corresponds with that determined in the solid state (FcCONMe2: 36/37° for two independent molecules).26,27
![]() | ||
Fig. 7 Calculated energy dependence on the torsion angle ψ for FcCONH2 (blue) and FcCSNH2 (red) at T = 300 K. |
Importantly, the curvature of the energy landscape near the minima for both FcCONH2 and FcCSNH2 allows for an essentially free change of ψ by approximately 20° in both directions at room temperature, i.e., within the energy change of 1 kBT (where kB is the Boltzmann constant). In this interval, the twist angle can thus be controlled via an interplay between energy changes reflecting the extent of conjugation, steric effects, coordination and intermolecular interactions (the latter in the solid state).
Another notable feature in the energy profiles concerns small changes in the slope for conformers whose amide groups are nearly coplanar with their bonding cyclopentadienyl rings (ψ ≈ 10°). These changes result from the potential energy surface (PES) crossing other surface corresponding to an inversion of the pyramidal NH2 moiety because the two surfaces coincide for the planar arrangement of the NH2 groups (for clarity, only the PES with the lower energy is shown in Fig. 7).
These precursors reacted identically with all of the amides to afford bis-chelate complexes of the type [M(L-κ2O,P)2]X. The reaction of thioamide 3 with [Cu(MeCN)4][BF4] afforded an analogous compound 6d, the structure of which, together with other representatives (6b, 7b and 6d; vide infra), was unambiguously confirmed by single-crystal X-ray diffraction analysis. In contrast, the reaction of 3 with silver(I) perchlorate produced an evidently different product (7d) exhibiting properties very different from those of the rest of the series: the compound readily precipitated from the reaction mixture and was practically insoluble in common organic solvents (including DMSO-d6), which in turn precluded its detailed characterisation by solution techniques (e.g., NMR spectroscopy). This finding alerted us to investigate this material in more detail. Fortunately, X-ray quality crystals were obtained when the educts were allowed to mix slowly by liquid-phase diffusion. The isolated crystals proved to be identical with 7d obtained by direct mixing of the starting materials, as evidenced by the IR spectra.
The structure determination revealed 7d to be a “dimer”, wherein the thioamide coordinates in a P,S-bidentate fashion to one silver(I) centre and simultaneously acts as a bridge towards the other Ag(I) ion through its sulfur atom. The coordination sphere is completed by O-bonded perchlorate, resulting in tetrahedral coordination around the chemically equivalent metal centres. As the consequence, the complex has an overall 1:
1 ligand-to-metal stoichiometry, which clearly differentiates 7d from the rest of the Cu(I) and Ag(I) complexes.
Complexes 6 and 7 were characterised by elemental analysis, IR and NMR spectroscopy, and ESI MS spectrometry. The coordination of the amidophosphine ligands in these compounds is clearly manifested in the 31P NMR spectra via a shift of the 31P NMR signal to lower fields. The 31P NMR signals are observed as singlets at approximately −11 ppm for the Cu(I) complexes 6a–d, and as 107/109Ag-coupled doublets at ca. 3–4 ppm for 7a–c. Compound 7d gives rise to a broad doublet at δP −0.3 with 1J(Ag,P) ≈ 510 Hz. It is also noteworthy that the 31P and 1H NMR signals are typically broadened, indicating that some dynamic processes are taking place in the solution. In their ESI mass spectra, the “mononuclear” complexes 6a–d and 7a–c exhibit signals of the cations [ML2]+ and their fragments [ML]+. The spectrum of the disilver(I) species 7d is dominated by the ions due to [Ag(3)]+ at m/z 563/566 and further shows additional signals attributable to [Ag(3)(CH3OH)]+ (m/z 596/599). All these results (shifts of the 1H and 31P NMR signals and species observed in the ESI MS spectra) suggest the solid state structures to be retained even in solution, though perhaps with some structural dynamics.
Finally, the presence of the counter anions is reflected in the IR spectra, showing composite intense bands resulting from the ν3 vibrations28 of the tetrahedral ions BF4− and ClO4− at ca. 1030–1095 cm−1 and 1050–1130 cm−1, respectively.
The anticipated dynamic and possibly hemilabile coordination29 of the phosphinoamide donors was proven by a serendipitous isolation of several crystals of a solvento complex, [Cu(5-κ2O,P)(5-κP)(CHCl3-κCl)][BF4] (6a′), which was isolated during an attempted crystallisation of 6a and structurally characterised. It is noteworthy that this solvento complex ensued from a copper(I) complex whose amide substituents (NH2) provide the lowest steric protection and donating ability among the amides studied and comprise oxygen as a hard donor atom (N.B. Cu(I) is softer than Ag(I) according to the absolute hardness scale30).
As indicated by the formulae given above, the compounds tend to retain crystallisation solvents in their structure, which often become disordered in structural voids defined by the bulky complex molecules. A similar effect affects the counter anions, which are considerably smaller than the cations they are associated with, and even some peripheral molecular parts (e.g., phenyl rings).
The crystal structure of 6d·2CHCl3 is shown in Fig. 8 (structural drawings of the analogous complexes 6b·1/4CHCl3 and 7b·CHCl3 are presented in the ESI†). Relevant geometric parameters for all three complexes are provided in Table 3. The structures support the formulation, revealing tetrahedral coordination environments around the metal centres constituted by two P,E-chelating (E = O or S) amidophosphine ligands. An inspection of the interligand angles reveals pronounced angular distortion of the coordination sphere resulting from the different steric demands of the donor moieties. In the pair of complexes derived from ligand 4 (i.e., 6b·1/4CHCl3 and 7b·CHCl3), the interligand angles increase from O–M–O via O–M–P to P–M–P. Such a feature, as well as the individual ligand–donor bond lengths, correspond with those reported for [Cu(Ph2PfcCONHCH2CO2Me-κ2O,P)2](CF3SO3).31
![]() | ||
Fig. 8 View of the cation in the structure of 6d·2CHCl3. The hydrogen atoms are omitted for clarity. |
Compound | 6b·1/4CHCl3 (M/E = Cu/O1, O2) | 6d·2CHCl3 (M/E = Cu/S1, S2) | 7b·CHCl3 (M/E = Ag/O) | 6a′·CHCl3 (M/E = Cu/O1, O2)c | |||
---|---|---|---|---|---|---|---|
Parameter | Ligand 1 | Ligand 2 | Ligand 1 | Ligand 2 | Ligand 1b | Ligand 1d | Ligand 2d |
a Definitions: Cp1 and Cp2 are the amide- and phosphine-substituted cyclopentadienyl rings, respectively. Cg1/2 are their centroids. τ is the torsion angle C1–Cg1–Cg2–C6 and φ is the dihedral angle subtended by the amide unit (E![]() |
|||||||
M–P | 2.2469(7) | 2.2256(8) | 2.2842(5) | 2.2636(5) | 2.4256(6) | 2.251(1) | 2.233(1) |
M–E | 2.174(2) | 2.102(2) | 2.3866(6) | 2.3951(7) | 2.468(2) | n.a. | 2.006(3) |
P–M–P [E–M–E] | 125.79(3) | [93.06(9)] | 127.32(2) | [108.24(2)] | 142.99(3) [80.20(6)] | 128.17(4) | n.a. |
P–M–E1 | 104.09(6) | 109.40(6) | 105.59(2) | 100.17(2) | 115.50(5) | n.a. | n.a. |
P–M–E2 | 101.29(7) | 117.74(6) | 104.98(2) | 109.33(2) | 93.16(5) | 110.95(9) | 118.04(9) |
Fe–Cg1 | 1.645(2) | 1.648(1) | 1.647(1) | 1.643(1) | 1.651(1) | 1.652(2) | 1.652(2) |
Fe–Cg2 | 1.639(1) | 1.646(1) | 1.644(1) | 1.647(1) | 1.640(1) | 1.649(2) | 1.646(2) |
∠Cp1, Cp2 | 1.0(2) | 4.0(2) | 3.5(2) | 7.5(2) | 1.0(2) | 2.7(2) | 2.2(2) |
τ | –49.4(2) | –68.2(2) | –59.5(2) | –15.2(2) | –69.5(2) | 101.0(3) | –59.4(3) |
C![]() |
1.240(4) | 1.228(3) | 1.711(2) | 1.714(2) | 1.231(3) | 1.250(4) | 1.271(3) |
C–N (amide) | 1.324(4) | 1.331(3) | 1.325(3) | 1.323(3) | 1.337(4) | 1.320(5) | 1.312(4) |
E![]() |
121.1(3) | 121.4(2) | 120.0(2) | 121.1(2) | 122.0(2) | 121.9(3) | 118.6(3) |
φ | 19.3(4) | 27.9(3) | 11.1(2) | 39.1(2) | 15.5(3) | 9.0(4) | 19.8(3) |
Upon going from 6b·1/4CHCl3 to 7b·CHCl3, a lengthening of the M–P (by ca. 0.2 Å) and, particularly, the M–O bonds (from ca. 2.10/2.17 Å for Cu(I) to 2.47 Å for Ag(I)) is observed owing to the presence of a larger central atom in the Ag(I) complex. The fact that the Cu–O distances in the structure of the former compound differ significantly (0.07 Å) can be associated with a relatively weaker coordination of the hard donor group, which may in turn allow for structural distortions without any dramatic destabilisation (increase in the overall energy; cf. the DFT calculations above). On the other hand, the bond lengths within the amide pendant change only marginally upon coordination (see the data for 4 above) but the ligand undergoes conformational reorganisation. The ferrocene-bound donor moieties are rotated closer to each other and the amide planes are twisted so as their oxygen atoms can reach the metal centre.
The Cu(I) complex bearing the thioamide ligands, 6d·2CHCl3, also possesses a tetrahedral structure, but because of longer Cu–S bonds, it appears to be more sterically relaxed. This is manifested in the interligand angles among which the S–Cu–S is no longer the most acute. Notably, the two structurally independent P,S-chelating ligands in the structure of 6d differ by conformation as evidenced by the τ and φ angles (Table 3; N.B. similar though less pronounced differences can be observed in the structure of 6b).
Opening of one of the chelate rings, such in the structure of 6a′·CHCl3 (Fig. 9 and Table 3), does not result in an equalisation of the interligand angles (ca. 87–128°), presumably because the amide oxygen is replaced with a relatively bulky chloroform molecule. The Cu–Cl1 distance of 3.138(2) Å approaches the threshold of the van der Waals contacts (3.15 Å32). According to a search in the Cambridge Structural Database (CSD),33 analogous Cu⋯Cl–CHCl2 interactions are rare and can be detected in the crystal structures of chloroform solvates of molecular triangles (Cu3)34 and squares (Cu4)35 built up from bis(acetylacetonate) ligands and Cu(II) ions, in which the chloroform occupies an apical position in a square pyramid around the Cu(II) ions (Cu⋯Cl ≈ 3.11–3.25 Å).
The different roles that the two amidophosphine ligands play in the complex cation of 6a′ are reflected in their conformations. Thus, the donor substituents in the chelating ligand adopt a conformation between synclinal staggered and synclinal eclipsed (τ ≈ −59°), and the amide planes are rotated by ca. 20° with respect to the parent cyclopentadienyl ring. On the other hand, the P-bound ligand assumes a more opened anticlinal conformation (τ ≈ 101°) and the amide plane is twisted by only ca. 9°. The CO distances are affected only marginally but in the expected manner as the coordinated C
O bond is ca. 0.02 Å longer than the uncoordinated one.
NH protons in the structures of complexes with coordinated 4 (i.e., 6b and 7b) are involved in hydrogen bonding to the respective counter anion in the crystal state. Those in molecules of 6a′ interconnect the complex units into dimers positioned around the inversion centres (Fig. 9). In the latter case, each P-bound ligand is linked to its inversion-related counterpart via a pair of N–H⋯OC hydrogen bonds from the NH hydrogen closer to the amide oxygen, whereas the other hydrogen forms an N–H⋯F hydrogen bridge to one of the BF4− anions. Amide hydrogens in the P,O-chelating ligand participate in similar interactions towards the oxygen in the P-monodentate ligand (O1) bonded to the same metal centre and towards another BF4 fluorine, respectively.
As it was stated above, complex 7d (Fig. 10 and Table 4) is a dimer, in which the phosphinoamide ligands coordinate in a chelating manner and are further involved in bridging of the “other” Ag(I) ion through the sulfur atom. The donor set around each Ag(I) is supplemented with an O-bonded perchlorate anion into a distorted tetrahedron. The Ag–O distance of 2.814(6) Å falls well below the sum of the van der Waals radii (3.24 Å), suggesting a relatively weaker yet significant interaction between the anion and Ag(I).
![]() | ||
Fig. 10 View of the molecular structure of 7d. The prime-labelled atoms are generated by the crystallographic inversion. |
a All parameters are defined as for the free ligand (see Table 1). The prime-labelled atoms are generated by the (1 − x, 2 − y, 2 − z) symmetry operation. | |||
---|---|---|---|
Ag–P | 2.426(1) | P–Ag–S | 121.68(4) |
Ag–S | 2.663(1) | P–Ag–S′ | 143.55(5) |
Ag–S′ | 2.572(1) | P–Ag–O1 | 95.9(1) |
Ag–O1 | 2.814(6) | S–Ag–S′ | 85.44(4) |
Ag⋯Ag′ | 3.8469(7) | S–Ag–O1 | 117.6(1) |
S⋯S′ | 3.552(2) | S′–Ag–O1 | 90.9(1) |
Fe–Cg1 | 1.647(2) | ∠Cp1, Cp2 | 5.1(3) |
Fe–Cg2 | 1.651(2) | τ | –80.9(3) |
C11![]() |
1.719(4) | S–C11–N | 120.3(3) |
C11–N | 1.306(6) | φ | 37.8(5) |
The Ag–S distance pertaining to the sulfur atom from the chelating ligand is ca. 0.1 Å longer than the Ag–S distance to the bridging sulfur, and the central Ag4S4 ring has a twisted rhomboidal shape (S–Ag–S′ = 85.44(4)°, Ag–S–Ag′ = 94.56(4)°). The ferrocene ligands adopt a conformation near to synclinal eclipsed (ideal value: τ = 72°) and their amide pendants are twisted by ca. 38°.
Compounds 8a–d were characterised similarly to the Cu(I) and Ag(I) complexes discussed above. In addition, the molecular structure of 8d was determined by single-crystal X-ray diffraction analysis. The 1H and 31P{1H} NMR spectra of 8a–d show signals of the phosphinoferrocene ligands and sharp singlets at ca. δP +29, respectively. The ESI MS spectra of these complexes display signals attributable to cationic fragments resulting from the loss of chloride ion ([M − Cl]+) and, for 8a–c, also the signals due to the pseudomolecular ions ([M + Na]+ and [M + K]+).
The amidophosphine ligands in the two molecules exert negligible tilting on the ferrocene unit (1.9(5)° and 3.4(5)°) and adopt conformations close to synclinal eclipsed (cf. τ with the ideal value of 72°). The amide substituents are rotated by ca. 33° and 40° (for molecules 1/2) from the planes of their parent cyclopentadienyl rings so that the bulky NMe2 unit are directed away from the ferrocene unit. The structure of 8d is essentially molecular; no Au⋯Au contacts indicative of possible aurophilic interactions39 were detected.
Thus, in cyclic voltammetry, compound 6c undergoes an oxidation which can be tentatively attributed to the oxidation of its ferrocene ligands (Fig. 12). However, the observed redox wave is composite, presumably owing to a convolution of two narrow-spaced oxidations (peak potentials: anodic 0.49 V, cathodic 0.34 V). This is clearly manifested in differential pulse voltammograms (see Figure in the ESI†). The associated redox process appears to be reversible, though only when the wave is scanned separate over a narrow range. If the scan is extended beyond this first redox event, an irreversible oxidative and two reduction waves appear, replacing the original redox response during the second and following scans (Fig. 12). The response of the analogous Ag(I) complex 7c in cyclic voltammetry is very similar (peak potentials for the composite wave: approx. 0.50 and 0.37 V).
On the other hand, the redox behaviour of the Cu(I)–thioamide complex 6d differs from that of 6c (Fig. 13) in that compound 6d undergoes an irreversible oxidation at ca. 0.41 V (peak potential). When the scan window is enlarged, a pair of redox waves appears at ca. 0.66 and 0.32 V that practically supersede the original oxidative wave. Finally, the gold(I) monophosphine complex 8c undergoes a standard one-electron oxidation at E°′ = 0.375 V. It is noteworthy that the wave, which can be ascribed to the ferrocene/ferrocenium couple, is electrochemically reversible, very likely because the lone pair at phosphorus as a reactive site is no longer available.5 The shift of the redox wave towards more positive potential with respect to free 2 corresponds with the expected electron density lowering at the ferrocene unit associated with coordination.
![]() | ||
Fig. 13 Representative cyclic voltammograms of 6d as recorded at a glassy carbon electrode and 0.1 V s−1 scan rate (the second scan is shown as a dashed line). |
As evidenced by the structures of the free donors and their complexes, the molecules of 1′-(diphenylphosphino)ferrocene amides and thioamides are flexible, allowing for a pre-organisation of the donor moieties into positions suitable for coordination via rotation of the ferrocene cyclopentadienyls and twisting of the amide unit around the pivotal C–C bond at no substantial energy cost. The hybrid nature of these donors, particularly the amides combining hard and soft donor groups, results in hemilabile coordination in complexes with the soft Group 11 metal ions that in turn affects the stability and structural dynamics of these coordination compounds. The coordination variability is in no way reduced upon the replacement of amide oxygen with the soft sulfur atom. The thioamides may thus not only simply parallel the behaviour of their amide analogues but can also behave differently, taking advantage of the specific qualities of the thioamide moiety (longer CS bond, softer and less electronegative donor atom, etc.) and thus give rise to new and unique structural motifs (cf. the structure of 7d). All of these factors render the coordination chemistry of phosphino-thioamides an attractive research target that has not yet been explored in great detail.
IR spectra were recorded with an FTIR Nicolet 760 instrument in the range 400–4000 cm−1. NMR spectra were obtained on a Varian UNITY Inova 400 spectrometer at 25 °C unless noted otherwise. Chemical shifts (δ/ppm) are referenced to internal tetramethylsilane (for 1H and 13C NMR spectra) and external 85% aqueous H3PO4 (31P NMR spectra). Alongside the standard notation of signal multiplicity, vq and vt are used to distinguish virtual quartets and triplets arising from the magnetically non-equivalent protons at the phosphine- and carbamoyl-substituted cyclopentadienyl rings, respectively.
Electrospray ionisation mass spectra (ESI MS) were recorded with a Bruker Esquire 3000 spectrometer using samples dissolved in HPLC-grade methanol. High-resolution (HR) ESI mass spectra were measured on a LTQ Orbitrap XL spectrometer. UV-vis spectra were recorded with a Unicam UV300 spectrometer in 1,2-dichloroethane. Elemental analyses were determined with a PE 2400 Series II CHNS/O Elemental Analyser (Perkin Elmer). The amount of clathrated solvent (if any) was verified by NMR analysis.
Safety note. Caution! Although we have not encountered any problems, it must be noted that perchlorate salts of complexes with organic ligands are potentially explosive and should be handled with care and only in small quantities.
1H NMR (399.95 MHz, CDCl3): δ 3.04 (br s, 6 H, NMe2), 4.14 (vq, J′ ≈ 1.7 Hz, 2 H, fc), 4.19 (vt, J′ = 1.9 Hz, 2 H, fc), 4.47 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 4.52 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 7.28–7.39 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, CDCl3): δ −16.8 (s). 13C{1H} NMR (100.58 MHz, CDCl3): δ 37.5 (very br, NMe2), 70.73 (CH of fc), 71.44 (CH of fc), 73.46 (d, JPC = 4 Hz, CH of fc), 74.18 (d, JPC = 15 Hz, CH of fc), 79.20 (C-CONMe2 of fc), 128.17 (d, 3JPC = 7 Hz, PPh2 CHmeta), 128.58 (PPh2 CHpara), 133.43 (d, 2JPC = 20 Hz, PPh2 CHortho), 138.60 (d, 1JPC = 9 Hz, PPh2 Cipso), 170.07 (CO). The signal due to C-PPh2 was not observed. IR (Nujol): νmax 1615 vs (amide I), 1502 s (amide II) cm−1. ESI+ MS: m/z 442 ([M + H]+). HR MS (ESI) calcd for C25H25FeNOP ([M + H]+) 442.1018, found 442.1019. Anal. Calcd for C25H24FeNOP (441.3): C 68.04, N 3.17, H 5.48%. Found: C 67.74, N 3.04, H 5.32%.
1H NMR (399.95 MHz, CDCl3): δ 3.31 (br s, 3 H, NMe), 3.43 (br s, 3 H, NMe), 4.12 (vq, J′ ≈ 1.8 Hz, 2 H, fc), 4.24 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 4.50 (vt, J′ ≈ 1.8 Hz, 2 H, fc), 4.59 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 7.29–7.39 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, CDCl3): δ −16.8 (s). 13C{1H} NMR (100.58 MHz, CDCl3): δ 44.19 (NMe), 45.08 (NMe), 70.62 (CH of fc), 72.99 (CH of fc), 75.39 (d, JPC = 14 Hz, CH of fc), 75.81 (d, JPC = 4 Hz, CH of fc), 88.02 (C-CSNMe2 of fc), 128.17 (d, 3JPC = 7 Hz, PPh2 CHmeta), 128.57 (PPh2 CHpara), 133.46 (d, 2JPC = 20 Hz, PPh2 CHortho), 138.73 (d, 1JPC = 10 Hz, PPh2 Cipso), 199.24 (CS). The signal due to C-PPh2 was not observed. IR (Nujol): νmax 1508 (νC–N) cm−1. ESI+ MS: m/z 480 ([M + Na]+). HR MS (ESI) calcd for C25H25NSPFe ([M + H])+ 458.0789, found 458.0789.
1H NMR (399.95 MHz, CDCl3): δ 2.83 (d, 3JHH = 4.9 Hz, 3 H, NMe), 4.07 (vq, J′ ≈ 1.9 Hz, 2 H, fc), 4.22 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 4.44 (vt, J′ ≈ 1.8 Hz, 2 H, fc), 4.55 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 5.60 (br q, 3JHH ≈ 5 Hz, 1 H, NH), 7.31–7.41 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, CDCl3): −16.7 (s). 13C{1H} NMR (100.58 MHz, CDCl3): δ 26.50 (NMe), 69.38 (CH of fc), 71.31 (CH of fc), 72.71 (d, JPC = 4 Hz, CH of fc), 74.31 (d, JPC = 14 Hz, CH of fc), 128.30 (d, 3JPC = 7 Hz, PPh2 CHmeta), 128.80 (PPh2 CHpara), 133.48 (d, 2JPC = 20 Hz, PPh2 CHortho), 138.34 (d, 1JPC = 9 Hz, PPh2 Cipso), 170.30 (CO). Signals due to ferrocene Cipso were not observed. IR (Nujol): νmax 3308 m (νN–H), 1628 s (amide I), 1545 s (amide II) cm−1. ESI+ MS: m/z 428 ([M + H]+). HR MS (ESI) calcd for C24H22FeNNaOP ([M + Na]+) 450.0681, found 450.0680. Anal. Calcd for C24H22FeNO (427.3): C 67.46, N 3.28, H 5.19%. Found: C 67.07, N 3.24, H 5.03%.
1H NMR (399.95 MHz, CDCl3): δ 2.93 (d, 3JHH = 4.7 Hz, 3 H, NMe), 4.07 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 4.14 (vq, J′ ≈ 1.9 Hz, 2 H, fc), 4.58 (vq, J′ ≈ 1.8 Hz, 2 H, fc), 4.99 (vt, J′ ≈ 1.9 Hz, 2 H, fc), 7.44–7.58 (m, 6 H, PPh2), 7.65–7.73 (m, 4 H, PPh2), 8.76 (br q, 3JHHca. 4.5 Hz, 1 H, NH). 31P{1H} NMR (161.90 MHz, CDCl3): δ 31.6 (s). 13C{1H} NMR (100.58 MHz, CDCl3): δ 26.46 (NMe), 70.26 (CH of fc), 70.74 (CH of fc), 72.56 (d, JPC = 11 Hz, CH of fc), 73.07 (d, 1JPC = 114 Hz, C-PPh2 of fc), 74.91 (d, JPC = 13 Hz, CH of fc), 79.63 (C-CONH of fc), 128.45 (d, JPC = 12 Hz, PPh2 CH), 131.43 (d, JPC = 10 Hz, PPh2 CH), 131.94 (d, 4JPC = 2 Hz, PPh2 CHpara), 133.10 (d, 1JPC = 108 Hz, PPh2 Cipso), 170.35 (CO). IR (Nujol): νmax 3246 m, 1657 s (amide I), 1556 s (amide II) cm−1. ESI+ MS: m/z 466 ([M + Na]+). HR MS (ESI) calcd for C24H23FeNO2P ([M + H]+) 444.0810, found 444.0809. Anal. Calcd for C24H22FeNO2·1/4CH2Cl2 (464.5): C 62.71, N 3.02, H 4.88%. Found: C 62.70, N 2.81, H 4.73%.
1H NMR (399.95 MHz, CDCl3): δ 2.92 (d, 3JHH = 4.8 Hz, 3 H, NMe), 3.96 (vt, J′ ≈ 2.0 Hz, 2 H, fc), 4.23 (vq, J′ ≈ 2.0 Hz, 2 H, fc), 4.62 (vq, J′ ≈ 2.0 Hz, 2 H, fc), 4.90 (vt, J′ ≈ 2.0 Hz, 2 H, fc), 7.41 (br q, 3JHH ≈ 5 Hz, 1 H, NH), 7.43–7.56 (m, 6 H, PPh2), 7.68–7.76 (m, 4 H, PPh2). 31P{1H} NMR (161.90 MHz, CDCl3): δ 42.9 (s). 13C{1H} NMR (100.58 MHz, CDCl3): δ 26.13 (NMe), 70.86 (CH of fc), 71.00 (CH of fc), 73.05 (d, JPC = 10 Hz, CH of fc), 74.81 (d, JPC = 12 Hz, CH of fc), 75.98 (d, 1JPC = 97 Hz, C-PPh2 of fc), 79.01 (C-CONH of fc), 128.40 (d, JPC = 13 Hz, PPh2 CH), 131.60 (d, JPC = 10 Hz, PPh2 CH), 131.62 (d, 4JPC = 4 Hz, PPh2 CHpara), 133.51 (d, 1JPC = 88 Hz, PPh2 Cipso), 169.88 (CO). IR (Nujol): νmax 3298 m, 3229 m, 1628 s (amide I), 1558 s (amide II) cm−1. ESI+ MS: m/z 482 ([M + Na]+). HR MS (ESI) calcd for C24H23FeNOPS ([M + H]+) 460.0582, found 460.0583. Anal. Calcd for C24H22FeNOPS·1/2CH2Cl2 (501.2): C 58.64, N 2.79, H 4.62%. Found C 58.57, N 2.71, H 4.53%.
1H NMR (399.95 MHz, dmso-d6): δ 4.15 (br s, 2 H, fc), 4.19 (vt, 2 H, J′ = 1.7 Hz, fc), 4.51 (vt, 2 H, J′ = 1.7 Hz, fc), 4.82 (br s, 2 H, fc), 7.40 (s, 1 H, NH2), 7.42–7.52 (m, 10 H, PPh2), 7.71 (s, 1 H, NH2). 31P{1H} (161.90 MHz, dmso-d6): δ −10.1 (br s). IR (Nujol): νmax 3450 (m), 3362 (m), 1650 (s) 1583 (s), 1481 (m), 1437 (m), 1405 (m), 1167 (m), 1095 (s), 1069 (s), 1029 (s), 837 (m), 748 (m), 697 (m), 517 (m), 502 (m) cm−1. ESI+ MS: m/z 889 ([Cu(5)2]+), 476 ([Cu(5)]+). Anal. calcd for C46H40BCuF4Fe2N2O2P2·1/2CH2Cl2 (1019.3): C 54.79; N 2.75, H 4.05%. Found C 54.51; N 3.00, H 4.27%.
1H NMR (399.95 MHz, dmso-d6): δ 2.73 (d, 3JHH = 4.5 Hz, 3 H, NMe), 4.15 (vt, J′ = 1.8 Hz, 2 H, fc), 4.18 (vt, J′ = 1.8 Hz, 2 H, fc), 4.52 (vt, J′ = 1.8 Hz, 2 H, fc), 4.75 (vt, J′ = 1.8 Hz, 2 H, fc), 7.38–7.50 (m, 10 H, PPh2), 8.24 (br d, 3JHH ≈ 4.5 Hz, 1 H, NH). 31P{1H} NMR (161.90 MHz, dmso-d6): δ −11.5 (br s). IR (Nujol): ν 3397 (m), 1618 (s), 1601 (w), 1558 (s), 1435 (m), 1411 (m), 1310 (m), 1165 (w), 1061 (s), 1029 (s), 830 (m), 816 (m), 747 (s), 699 (s), 519 (s), 510 (m), 488 (s), 462 (m) cm−1. ESI+ MS: m/z 917 ([Cu(4)2]+), 490 ([Cu(4)]+). Anal. Calcd for C48H44BCuF4Fe2N2O2P2·CH2Cl2 (1089.8): C 54.00, N 2.57, H 4.25%. Found C 54.28, N 2.47, H 4.20%.
1H NMR (399.95 MHz, dmso-d6): δ 2.93 (br s, 3 H, NMe), 3.02 (br s, 3 H, NMe), 4.19 (vt, J′ = 1.8 Hz, 2 H, fc), 4.21 (vt, J′ = 1.8 Hz, 2 H, fc), 4.53 (br s, 2 H, fc), 4.60 (vt, J′ = 1.8 Hz, 2 H, fc), 7.42–7.53 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6): δ −10.5 (br s). IR (Nujol): νmax 1582 (s), 1575 (s), 1505, (m), 1435 (w), 1401 (m), 1377 (m), 1112 (m), 1096 (m), 1050 (s) 1032 (s), 745 (m), 696 (s), 511 (s), 495 (s) cm−1. ESI+ MS: m/z 945 ([Cu(2)2]+), 504 ([Cu(2)]+). Anal. calcd for C50H48BCuF4Fe2N2O2P2 (1032.9): C 58.14, N 2.71; H 4.68%. Found: C 58.63, N 2.52, H 4.94%.
1H NMR (399.95 MHz, dmso-d6, 25 °C): δ 3.28 (br s, 3 H, NMe), 3.53 (s, 3 H, NMe), 4.15 (br s, 2 H, fc), 4.35 (br s, 2 H, fc), 4.60 (br s, 2 H, fc), 4.64 (br s, 2 H, fc), 7.30–7.52 (m, 10 H, PPh2). 1H NMR (399.95 MHz, dmso-d6, 50 °C): δ 3.19 (s, 3 H, NMe), 3.53 (s, 3 H, NMe), 4.16 (br s, 2 H, fc), 4.35 (vt, J′ = 1.9 Hz, 2 H, fc), 4.59 (vt, J′ = 1.9 Hz, 2 H, fc), 4.74 (br s, 2 H, fc), 7.35–7.50 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6, 25 °C): δ −11.0 (br s). IR (Nujol): νmax 1712 (w), 1526 (m), 1436 (w), 1277 (m), 1059 (s) 1135 (m), 825 (m) 745 (m), 697 (m), 511 (m), 491 (w) cm−1. ESI+ MS: m/z 977 ([Cu(3)2]+), 520 ([Cu(3)]+). Anal. Calcd for C50H48BCuF4Fe2N2P2S2·1/4CH2Cl2 (1086.3): C 55.56, N 2.58, H 4.50%. Found: C 55.53, N 2.57, H 4.77%.
1H NMR (399.95 MHz, CDCl3): δ 4.11 (br vt, J′ = 1.9 Hz, 2 H, fc), 4.46 (br s, 2 H, fc), 4.72 (vt, J′ = 1.9 Hz, 2 H, fc), 4.84 (br vt, J′ = 1.8 Hz, 2 H, fc), 6.24 (br s, 1 H, NH), 6.75 (br s, 1 H, NH), 7.39–7.56 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, CDCl3): δ 3.1 (broad d, 1J(107/109Ag, 31P) ≈ 510 Hz). IR (Nujol): νmax 3444 (m), 3340 (m), 1645 (s), 1591 (s), 1555 (m), 1479 (w), 1436 (s), 1396 (m), 1168 (m), 1098 (br s), 1027 (s), 910 (m), 837 (m), 826 (m), 747 (s), 735 (s), 697 (s), 624 (m), 532 (w), 506 (s), 489 (m), 465 (m) cm−1. ESI+ MS: m/z 933 ([Ag(5)2]+), 520 ([Ag(5)]+). Anal. Calc. for C46H40AgClFe2N2O6P2·CH2Cl2 (1118.7): C 50.46, H 3.76, N 2.50%. Found: C 49.95, H 3.58, N 2.62%.
1H NMR (399.95 MHz, dmso-d6): δ 2.67 (d, 3JHH = 4.6 Hz, 3 H, NMe), 4.12 (vt, J′ = 1.9 Hz, 2 H, fc), 4.29 (vt, J′ = 1.9 Hz, 2 H, fc), 4.60 (vt, J′ = 1.9 Hz, 2 H, fc), 4.85 (vt, J′ = 1.9 Hz, 2 H, fc), 7.44–7.60 (m, 10 H, PPh2), 8.09 (q, 3JHH = 4.6 Hz, 1 H, NH). 31P{1H} NMR (161.90 MHz, dmso-d6): δ 2.6 (pair of d, 1J(107Ag, 31P) = 543 Hz, 1J(109Ag, 31P) = 471 Hz). IR (Nujol): νmax 3389 (m), 3079 (w), 1629 (s), 1615 (s), 1544 (s), 1480 (w), 1435 (m), 1412 (m), 1301 (m), 1194 (m), 1174 (m), 1095 (s), 1067 (br s), 1050 (w), 1031 (m), 914 (m), 816 (m), 748 (s), 697 (s), 623 (m), 529 (m), 509 (s), 492 (m), 467 (m) cm−1. ESI+ MS: m/z 961 ([Ag(4)2]+), 534 ([Ag(4)]+). Anal. Calc. for C48H44AgClFe2N2O6P2·CH2Cl2 (1146.7): C 51.32, H 4.04, N 2.44%. Found: C 50.90, H 3.75, N 2.13%.
1H NMR (399.95 MHz, dmso-d6): δ 2.91 (br s, 3 H, NMe), 2.99 (br s, 3 H, NMe), 4.22 (br s, 2 H, fc), 4.32 (br s, 2 H, fc), 4.61 (vt, J′ = 1.9 Hz, 2 H, fc), 4.65 (vt, J′ = 1.9 Hz, 2 H, fc), 7.49–7.56 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6): δ 4.2 (pair of concentric d, 1J(107Ag, 31P) = 770 Hz, 1J (109Ag, 31P) = 685 Hz). IR (Nujol): νmax 1557 (s), 1492 (s), 1436 (m), 1127 (m), 1109 (s), 1097 (m), 1071 (w), 1050 (s), 824 (w), 758 (m), 747 (m), 695 (m), 679 (s), 623 (s), 514 (w), 503 (w), 490 (m), 467 (w) cm−1. ESI+ MS: m/z 989 ([Ag(2)2]+), 548 ([Ag(2)]+). Anal. Calc. for C50H48AgClFe2N2O6P2·1/2CH2Cl2 (1132.3): C 53.56, H 4.36, N 2.47%. Found: C 53.30, H 4.15, N 2.35%.
1H NMR (399.95 MHz, dmso-d6): δ 3.39 (s, 3 H, NMe), 3.56 (s, 3 H, NMe), 4.12 (dt, J = 3.0, 1.8 Hz, 2 H, fc), 4.30 (vt, J′ = 1.9 Hz, 2 H, fc), 4.73 (vt, J′ = 1.8 Hz, 2 H, fc), 5.06 (vt, J′ = 1.9 Hz, 2 H, fc), 7.50–7.57 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6): δ −0.3 (broad d, 1J(107/109Ag, 31P) ≈ 510 Hz). IR (Nujol): νmax 1551 (s), 1436 (m), 1280 (m), 1144 (m), 1108 (s), 1096 (s), 1061 (m), 1030 (m), 979 (m), 851 (m), 818 (w), 749 (m), 695 (m), 623 (m), 507 (m), 465 (m) cm−1. ESI+ MS: m/z 564 ([Ag(3)]+), 597 ([Ag(3)(CH3OH)]+). Anal. Calc. for C50H48Ag2Cl2Fe2N2O8P2S2 (1329.3): C 45.17, H 3.64, N 2.11%. Found: C 44.83, H 3.81, N 1.90%.
1H NMR (399.95 MHz, dmso-d6): δ 4.28 (vt, J′ = 1.9 Hz, 2 H, fc), 4.48 (dt, J = 3.0, 1.9 Hz, 2 H, fc), 4.59–4.61 (m, 2 H, fc), 4.78 (vt, J′ = 1.9 Hz, 2 H, fc), 7.02 (br s, 1 H, NH), 7.37 (br s, 1 H, NH), 7.54–7.64 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6): δ 28.7 (s). IR (Nujol): νmax 3421 (m), 1667 (s), 1612 (m), 1432 (m), 1349 (m), 1176 (m), 1099 (m), 1027 (m), 843 (m), 822 (m), 745 (m), 688 (s), 526 (m), 511 (m), 496 (w), 477 (s) cm−1. ESI+ MS: m/z 610 ([8a − Cl]+), 668 ([8a + Na]+), 684 ([8a + K]+). Anal. Calcd for C23H20AuClFeNOP (645.6): C 41.75, N 2.12, H 3.05%. Found: C 41.56, N 1.93, H 2.96%.
1H NMR (399.95 MHz, CDCl3): δ 2.93 (d, 3JHH = 4.8 Hz, 3 H, NMe), 4.19 (vt, J′ = 1.8 Hz, 2 H, fc), 4.23 (dt, J = 2.9, 1.9 Hz, 2 H, fc), 4.68–4.70 (m, 2 H, fc), 4.87 (vt, J′ = 1.9 Hz, 2 H, fc), 6.07 (q, 3JHH = 4.8 Hz, 1 H, NH), 7.44–7.61 (m, 10H, PPh2). 31P{1H} NMR (161.90 MHz, CDCl3): δ 28.8 (s). IR (Nujol): νmax 3369 (m), 1628 (s), 1544 (m), 1440 (m), 1298 (m), 1173 (m), 1103 (w), 1029 (m), 1000 (w), 842 (m), 743 (m), 691 (m), 628 (w), 555 (w), 529 (w), 515 (w), 494 (w), 480 (w) cm−1. ESI+ MS: m/z 624 ([8b − Cl]+), 680 ([8b + Na]+), 698 ([8b + K]+). Anal. Calcd for C24H22AuClFeNOP·1/2CHCl3 (719.3): C 40.90, N 1.95, H 3.15%. Found C 41.04, N 1.79, H 3.09% (analytical sample crystallised from chloroform/pentane).
1H NMR (399.95 MHz, dmso-d6): δ 2.85 (s, 3 H, NMe), 3.00 (s, 3 H, NMe), 4.30 (vt, J′ = 1.9 Hz, 2 H, fc), 4.43 (dt, J = 3.0, 1.8 Hz, 2 H, fc), 4.61 (vt, J′ = 1.8 Hz, 2 H, fc), 4.73–4.76 (m, 2 H, fc), 7.54–7.65 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6): δ 28.9 (s). IR (Nujol): νmax 3103 (m), 1622 (s), 1585 (m), 1499 (m), 1439 (s), 1393 (m), 1308 (m), 1265 (m), 1225 (m), 1180 (m), 1173 (m), 1107 (s), 1039 (m), 1032 (m), 840 (m), 821 (m), 758 (s), 752 (s), 704 (s), 558 (m), 535 (m), 526 (s), 504 (s), 490 (s), 474 (m) cm−1. ESI+ MS: m/z 638 ([8c − Cl]+), 696 ([8c + Na]+), 712 ([8c + K]+). Anal. Calcd for C25H24AuClFeNOP (673.7): C 44.57, N 2.08, H 3.59%. Found: C 44.22, N 2.01, H 3.50%.
1H NMR (399.95 MHz, dmso-d6): δ 3.27 (s, 3 H, NMe), 3.29 (s, 3 H, NMe), 4.34 (vt, J′ = 1.9 Hz, 2 H, fc), 4.35 (dt, J = 3.0, 1.8 Hz, 2 H, fc), 4.73 (vt, J′ = 1.9 Hz, 2 H, fc), 4.76–4.79 (m, 2 H, fc), 7.54–7.65 (m, 10 H, PPh2). 31P{1H} NMR (161.90 MHz, dmso-d6): δ 28.7 (s). IR (Nujol): νmax 1712 (w), 1512 (s), 1435 (m), 1309 (m), 1274 (m) 1174 (m), 1138 (m), 1101 (s), 1062 (w), 1034 (w), 1025 (w), 989 (w), 973 (w), 838 (m), 824 (m), 814 (w), 764 (w), 749 (m), 695 (s), 556 (m), 530 (m), 509 (s), 498 (w), 477 (m) cm−1. ESI+ MS: m/z 654 ([8d − Cl]+. Anal. calcd for C25H24AuClFeNPS (689.8): C 43.53, N 2.03, H 3.51%. Found: C 43.88, N 1.87, H 3.45%.
All structures were solved by direct methods (SHELXS9742) and refined by full-matrix least-squares based on F2 (SHELXL9742). The non-hydrogen atoms were refined with anisotropic displacement parameters. The amide hydrogen atoms (NH; if present) were located on the difference electron density maps and refined as riding atoms with Uiso(H) set to a 1.2Ueq(N). Hydrogens residing on the carbon atoms were included in their calculated positions and refined similarly with Uiso(H) = 1.5Ueq(C) for the methyl groups and 1.2Ueq(C) for all other CHn moieties. Particular details of the structure refinement are as follows.
Compound 4S crystallises in the chiral Pc space group with two molecules per asymmetric unit. However, all atoms except for the amide moiety in these two independent molecules match each other because of an inversion centre from the space group P21/c (the maximum distance of the overlapping atoms in the phosphinoferrocenyl units is 0.53 Å). Such a virtually higher symmetry results in large correlations during the refinement and, therefore, restrictions to anisotropic displacement parameters had to be applied to several atoms.
Parts of some structures (7b·CHCl3: the solvent and the perchlorate anion; 6b·1/4CHCl3 and 6a′·CHCl3: one of the phosphorus-bound phenyl rings and the BF4− anion) are disordered and were refined over two positions (with isotropic displacement parameters, if necessary). Moreover, the solvating molecules in the structures of 6b·1/4CHCl3 and 6a′·CHCl3 are severely disordered in structural voids and were modelled by PLATON/SQUEEZE.43
All geometric calculations were performed and the diagrams were obtained with the PLATON program.44 All numerical values were rounded with respect to their estimated deviations (ESDs) given to one decimal place. Parameters relating to atoms in constrained positions (hydrogens) are given without ESDs.
Footnote |
† Electronic supplementary information (ESI) available: Summary of crystallographic parameters, an overlap of the two independent molecules in the structure of 8d, displacement ellipsoid plots for all structurally characterised compounds, comparison of the DFT optimised and experimental structures of 2 and 3, and DFT calculated coordinates for compounds 2, 3 and FcC(E)NR2 (E = O, S; R = H, Me) as XYZ files. CCDC 1029509–1029520. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c4dt03279a |
This journal is © The Royal Society of Chemistry 2015 |