Eliane
Deschamps
,
Bernard
Deschamps
,
Jeanne
Laure Dormieux
,
Louis
Ricard
,
Nicolas
Mézailles
and
Pascal
Le Floch
*
Laboratoire Hétéroéléments et Coordination
, Department of Chemistry, UMR CNRS 7653, DCPH, Ecole Polytechnique, 91128, Palaiseau Cedex, France. E-mail: lefloch@poly.polytechnique.fr; Fax: +33 1 69333990
First published on 28th October 2005
New kinetically stabilized mono- and bis-phosphaalkene ligands (2 and 3, respectively) were synthesized via the phospha-Wittig approach. Ligand 3 was characterized by X-ray diffraction. The coordinating behaviour of the bidentate ligand was investigated towards group 11 metal centers in order to test its capacity to bind two coordination sites located in a trans-fashion. The [Au(3)][BF4], [Ag(3)(H2O)][BF4] and [Cu(3)(CH3CN)][BF4] complexes 4, 5 and 6, respectively, were characterized by X-ray diffraction. The peculiar geometries of 4 and 6 were rationalized by means of DFT calculations.
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Scheme 1 |
As part of a program aimed at developing the use of such polydentate ligands featuring sp2-hybridized phosphorus atoms in coordination chemistry and catalysis,8 we recently investigated the synthesis of bidentate structures featuring the dibenzofuran skeleton. Indeed, 4,6-bis(carbaldehyde)dibenzofuran proved to be a convenient precursor for the elaboration of bidentate ligands featuring imines9 or oxazolines (DBFOX ligands) as pendant ligands which can bind a metal centre in a trans-fashion. Some DBFOX-based complexes proved to be particularly efficient in some catalytic transformations.10 Herein, we wish to report on these syntheses as well as on the coordinating behaviour of this new type of ligands towards group 11 metals.
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Scheme 2 The phospha-Wittig approach. |
As a prerequisite to these syntheses, 4,6-bis(carbaldehyde)dibenzofuran was synthesized according to a well-known reported procedure that involves the dimetallation of dibenzofuran with n-butyllithium followed by a trapping reaction with dimethylformamide.13 The phospha-Wittig reagent 1 was conventionally prepared by reacting Mes*PCl2 with PMe3 (2.6 equiv.) in the presence of Zn as reductant in THF at 0 °C. Reaction of 1.1 equivalent of 1 with 4,6-bis(carbaldehyde)dibenzofuran readily occurred at room temperature to cleanly yield phosphaalkene 2. After 3 h of reaction, analysis of the crude mixture by 31P NMR spectroscopy revealed the presence of a very characteristic downfield shifted signal at 273.9 ppm. After extraction with dichloromethane, washings with water and crystallization from MeOH, compound 2 was isolated in a 60% yield as a very air stable pale yellow powder. The E-stereochemistry of 2 was confirmed by the analysis of the 1H NMR spectrum which exhibits a doublet at 8.58 ppm (2J(H–P) = 25.3 Hz). No trace of the Z-isomer was observed in the crude mixture (Scheme 3). The formulation proposed for 2 was confirmed by NMR and mass spectrometry as well as by elemental analyses.
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Scheme 3 Reagents and conditions: (i) THF, RT, 3 h. |
The bis-phosphaalkene derivative 3 was prepared following a similar strategy by using the phospha-Wittig reagent 1 in excess (2.2 equivalents). A prolonged reaction time (15 h) was needed to obtain a complete conversion. Importantly, 31P NMR spectroscopy revealed that only one stereoisomer is formed. Compound 3 was isolated following a similar workup in a 50% yield as a very stable pale yellow solid. The structure of 3 was easily established on the basis of 1H, 13C NMR data, mass spectrometry and elemental analyses. As in 2, the presence of a PC double bond was evidenced by the presence of a downfield signal in 31P NMR (δ(THF)
= 273 ppm)
(Scheme 4). The presence of two phosphaalkene moieties is proven first by 1H NMR. The signal of the phosphaalkene appears as a deceptively simple doublet of doublet (AA′XX′ spin system) at 8.4 ppm (∑J(H–P)
= 42 Hz, ∑ means sum). In the 13C NMR spectrum, the corresponding signal appears as the expected second-order signal at 167.1 ppm (AXX′ spin system, ∑J(C–P)
= 51.7 Hz).
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Scheme 4 Reagents and conditions: (i) THF, RT, 15 h. |
Single crystals of compound 3 were obtained by crystallization in MeOH at room temperature. An X-ray crystal structure analysis was carried out and a view of one molecule of 3 is presented in Fig. 1 as well as the most relevant bond distances and bond angles. Crystal data and structural refinement details are presented in Table 1. The compound has crystallographically imposed twofold symmetry. As can be seen the E-stereochemistry of both phosphaalkene moieties is confirmed. Interestingly, one can note that two PC bonds are coplanar with the dibenzofuran skeleton probably indicating that a weak delocalization occurs between the aromatic part of the molecules and the two P
C units. Besides, this is confirmed by the short C–C connection between the C9 carbon atoms and the C13 carbon atoms of the phosphaalkenes (d(C(9)–C(13))
= 1.454(2)
Å). Apart from this, the structure of 3 deserves no special comments.
3 | 4 | |
---|---|---|
Formula | C50H66OP2 | C50H66AuBF4OP2·C4H10O |
M r | 744.97 | 1102.86 |
Crystal system | Monoclinic | Orthorhombic |
Space group | C2 | P212121 |
a/Å | 15.966(1) | 11.647(1) |
b/Å | 10.407(1) | 16.895(1) |
c/Å | 14.099(1) | 27.329(1) |
β/° | 105.260(1) | 90.00 |
Z | 2 | 4 |
µ/cm−1 | 0.130 | 2.846 |
Reflections measured | 7551 | 27925 |
Reflections used | 5376 | 13250 |
wR 2 | 0.0924 | 0.0701 |
R 1 | 0.0349 | 0.0340 |
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Fig. 1 ORTEP view of one molecule of 3 (50% ellipsoids). The numbering is arbitrary and different from that used in NMR data. Atoms marked with a prime (′) are at equivalent position (−1 − x, y, −1 − z). Selected bond lengths (Å) and bond angles (°): C(13)–P(1) 1.674(3), C(3)–P(1) 1.852(1), C(13)–C(9) 1.454(2), C(9)–C(5) 1.405(2), C(5)–O(2) 1.379(1); C(3)–P(1)–C(13) 98.72(1), P(1)–C(13)–C(9) 128.5(1). |
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Scheme 5 Reagents and conditions: THF, RT, 3 h. |
The stoichiometric reaction of [AuCl·SMe2] and ligand 3 in THF led to a pale yellow solution. A 31P NMR of this mixture showed a very broad peak which revealed a weak interaction. Addition of solid AgBF4 resulted in the very fast formation of characteristic silver salt indicating the end of chloride abstraction. 31P NMR spectroscopy showed the formation of a single complex characterized by a singlet at 201 ppm (δ(3) = 273 ppm, Δδ = −72 ppm). The mixture was filtered through a pad of Celite and concentrated to give the desired complex 4 in near quantitative yield. The complex was fully characterized by usual NMR techniques as well as elemental analyses. Compared to the spectra of the starting ligand 3, complex 4 varies only marginally. In particular, the phosphaalkene proton is upfield shifted to 8.2 ppm and appears as a virtual triplet (simplified AA′XX′ spin system), because the magnitude of the J(P–P) increases upon coordination. In the 13C spectrum the two carbon atoms which are bound to the phosphorus atom are upfield shifted by ca. 10 ppm upon coordination. Single crystals of 4 were grown by a slow diffusion of diethyl ether in a THF solution of the complex. A view of one molecule of 4 is presented in Fig. 2 as well as the most relevant bond distances and bond angles. Crystal data and structural refinement details are presented in Table 1.
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Fig. 2 ORTEP view of one molecule of 4 (50% ellipsoids). The numbering is arbitrary and different from that used in NMR data. BF4 counter ion and methyl groups of the tert-butyl substituents have been omitted for clarity. Selected bond lengths (Å) and bond angles (°): Au(1)–P(1) 2.267(1), Au(1)–P(2) 2.267(1), Au(1)⋯O(1) 2.699, C(1)–P(1) 1.669(3), C(14)–P(2) 1.663(3), C(15)–P(1) 1.804(3), C(33)–P(2) 1.807(3), C(1)–C(2) 1.449(4), C(13)–C(14) 1.443(4), C(8)–O(1) 1.396(4), C(7)–O(1) 1.383(4); P(1)–Au(1)–P(2) 167.56(3), C(1)–P(1)–Au(1) 121.8(1), C(14)–P(2)–Au(1) 120.3(1), C(1)–P(1)–C(15) 112.3(2), C(15)–P(1)–Au(1) 125.9(1), C(13)–C(14)–P(2) 134.3(3), C(2)–C(1)–P(1) 133.0(3). |
The only apparent feature of this complex is the significant deviation from linearity observed for the P–Au–P angle (167.56°). Moreover, this deviation brings the gold center away from the oxygen atom of the furan moiety. As will be seen further, this can be easily rationalized by considering a simple molecular orbital diagram.
We next investigated the coordination to silver, which was readily achieved by the stoichiometric reaction of ligand 3 with AgBF4 (Scheme 6). After a few minutes, the 31P NMR of the crude mixture proves the formation of a single complex at 204 ppm. Unlike many Ag+ complexes, coupling of the two phosphorus atoms with both isotopes of Ag, namely Ag107 and Ag109 which both possess a spin of 1/2, was observed resulting in two sets of doublets (1J(Ag109–P) = 686 Hz and 1J(Ag107–P) = 596 Hz). After isolation, complex 5 was obtained as an air-stable solid. It was fully characterized by usual NMR techniques. In fact, a first surprising piece of information was given by a broad peak at 2.5 ppm in the 1H NMR spectrum. This peak integrated for two protons which suggested the coordination of a water molecule. We verified that the same complex is formed when the reaction is carried out in air. Therefore, it seems likely that the water-free complex adopts a distorted linear geometry like the gold analogue described above. The silver centre then picks up water from the solvent to complete the coordination sphere yielding the observed complex which possesses a trigonal planar geometry. The presence of a water molecule was confirmed by elemental analyses. In the 1H NMR spectrum also, the phosphaalkene proton appears as the expected signal for an AA′XX′ spin system (δ = 8.23 ppm, ∑J = 40 Hz). In fact, the silver analogue gives very similar spectra than the gold complex.
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Scheme 6 Reagents and conditions: CH2Cl2, air (traces of water), RT, 5 min. |
Single crystals were obtained by a slow diffusion of hexanes into a CH2Cl2 solution of the complex, in air. We were both quite surprised and pleased to see in the structure (Fig. 3) that the coordination sphere of the metal had been completed by water during crystallisation. Indeed, this definitely proves that, unlike classical phosphaalkenes, the bulky derivatives are very robust toward hydrolysis, even once coordinated to a metal centre.
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Fig. 3 ORTEP view of one molecule of 5 (50% ellipsoids). The numbering is arbitrary and different from that used in NMR data. BF4 counter ion and methyl groups of the tert-butyl substituents have been omitted for clarity. Selected bond lengths (Å) and bond angles (°): Ag(1)–P(1) 2.388(1), Ag(1)–P(2) 2.403(1), Ag(1)–O(2) 2.316(3), Ag(1)⋯O(1) 3.095, C(14)–P(2) 1.681(4), C(13)–P(1) 1.672(5), C(2)–C(13) 1.456(6), C(14)–C(11) 1.441(7), C(1)–O(1) 1.383(6), C(12)–O(1) 1.387(6), C(33)–P(2) 1.840(5), C(15)–P(1) 1.825(5); P(1)–Ag(1)–P(2) 145.14(4), P(1)–Ag(1)–O(2) 109.8(1), P(2)–Ag(1)–O(2) 103.3(1), C(14)–P(2)–Ag(1) 131.1(2), C(13)–P(1)–Ag(1) 130.6(2), C(11)–C(14)–P(2) 132.6(4), C(2)–C(13)–P(1) 132.1(4), C(13)–P(1)–C(15) 102.5(2). |
The P–Ag bond lengths Ag(1)–P(1) 2.388(1)
Å, Ag(1)–P(2) 2.403(1)
Å) are significantly longer than the P–Au bond lengths (Au(1)–P(1) 2.267(1)
Å, Au(1)–P(2) 2.267(1)
Å) as expected. The geometry at silver is trigonal planar (∑angles = 358.24°) with a wide P(1)–Ag(1)–P(2) angle at 145.14(4)°. This increase in the angle (compared to the gold complex) is accompanied by an increase in the CP–M angle from ca. 120 to ca. 130°
(C(13)–P(1)–Ag(1) 131.1(2)). The fact that phosphaalkene ligands can accommodate readily such changes in coordination angles reflects the diffuse nature of the lone pair of sp2 hybridized phosphorus.
To complete this investigation we examined the coordinating behaviour of 3 toward the catalytically relevant Cu(I) centre. Acetonitrile ligand was readily displaced from the [Cu(CH3CN)4][BF4] precursor to form a single complex 6 (Scheme 7). It appears as a singlet at 207 ppm in the 31P NMR spectrum. This complex was fully characterized by usual NMR techniques as well as elemental analysis.
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Scheme 7 Reagents and conditions: CH2Cl2, RT, 5 min. |
Single crystals of complex 6 were obtained by slow diffusion of hexanes in a CDCl3 solution of complex 6. A view of one molecule of 6 is presented in Fig. 4 that also lists the most significant bond lengths and angles. Crystal data and structural refinement details are presented in Table 2.
5 | 6 | |
---|---|---|
Formula | C50H66AgBF4O2P2·1/2CH2Cl2 | C52H69BCuF4NOP2·2CHCl3 |
M r | 1040.57 | 1175.11 |
Crystal system | Monoclinic | Triclinic |
Space group | C2/c |
P![]() |
a/Å | 35.058(3) | 11.931(1) |
b/Å | 11.084(1) | 14.527(1) |
c/Å | 30.013(3) | 19.169(1) |
α/° | 90.00 | 107.920(1) |
β/° | 116.700(2) | 92.030(1) |
γ/° | 90.00 | 109.710(1) |
Z | 8 | 2 |
µ/cm−1 | 0.602 | 0.748 |
Reflections measured | 17591 | 16842 |
Reflections used | 7576 | 13870 |
wR 2 | 0.2282 | 0.1806 |
R 1 | 0.0724 | 0.0628 |
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Fig. 4 ORTEP view of one molecule of 6 (50% ellipsoids). The numbering is arbitrary and different from that used in NMR data. BF4 counter ion and methyl groups of the tert-butyl substituents have been omitted for clarity. Selected bond lengths (Å) and bond angles (°): Cu(1)–P(1) 2.221(1), Cu(1)–P(2) 2.230(1), Cu(1)–N(1) 1.958(4), Cu(1)⋯O(1) 2.456, C(1)–P(1) 1.654(5), C(14)–P(2) 1.671(4), C(1)–C(2) 1.456(6), C(13)–C(14) 1.453(6), C(1)–O(1) 1.393(4), C(8)–O(1) 1.389(4), C(17)–P(1) 1.834(4), C(35)–P(2) 1.827(4); P(1)–Cu(1)–P(2) 132.60(4), P(1)–Cu(1)–N(1) 113.5(1), P(2)–Cu(1)–N(1) 113.7(1), C(1)–P(1)–Cu(1) 116.5(2), C(14)–P(2)–Cu(1) 120.6(2), C(2)–C(1)–P(1) 130.7(3), C(13)–C(14)–P(2) 127.3(3), Cu(1)–P(1)–C(17) 101.6(2). |
As can be seen, the geometry at the copper center is trigonal planar (∑angles = 359.8°) with a wide P(1)–Cu(1)–P(2) angle at 132.60(4)°. The P–Cu bond distances are normal at 2.221(1) and 2.230(1)
Å. The other bond distances and angles are quite similar than the above mentioned ones, and therefore will not be further commented on. This complex possesses however a very significant feature, namely the metal centre is located well above the plane of the ligand, as clearly shown on the ORTEP plot (dihedral angle C2–C1–P1–Cu1 = 9°). This geometry results in a bond distance of 2.456 Å, more consistent with a weak interaction than a true bond. Indeed, typical Cu–O bond distances of 2.208 Å are found with neutral ligands such as carbaldehyde–pyridine coordination to the [Cu(PPh3)2]+ fragment.14 For several carboxylate complexes of the type [Cu(PPh3)2(O2CR)], Hart et al. have shown that the Cu–OC linkage can vary from a true bond for R = CH3
(2.257(7)
Å) to a weak interaction for R = CHF2
(2.465(6)
Å) or R = CF3
(2.545(5)
Å).15 In fact, for these two last cases, addition of ethanol resulted in the breaking of this carboxylate interaction and ethanol coordination. How can the geometry at the copper centre of our complex be rationalized? Being in sharp contrast to the other geometries of the Au and Ag complexes, this fact can not be fortuitous. Like in the case of 4 and 5, this particular feature can be easily rationalized first through a qualitative molecular orbital diagram, and more quantitative DFT calculations.
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Scheme 8 Qualitative interaction diagram showing the four-electron destabilizing interactions occurring between the filled d-orbitals at the metal and 2px and 2py orbitals at the oxygen atom. |
Theoretical calculations were carried out on a model complex I in which the Mes* groups were replaced by xylyl groups. A view of the optimized structure is presented in Fig. 5. Though the substitution scheme of the phosphorus atom is different, a reasonable agreement was found between theoretical and experimental data (Fig. 5). Thus, the P–Au bonds falls at 2.311 Å for 2.267(1) Å in 4 and the P–Au–P bending is relatively well reproduced (165.83° for 167.56(3)° in 4). Examination of MOs allowed to check our hypothesis and as can be seen in the following figure several MOs account for this four-electron destabilizing interaction (see Fig. 6). The H-11 MO and H-13 correspond to the antibonding interaction between the dx2−y2 and the dz2 with the 2py AO at oxygen, respectively, whereas the H-12 is antibonding between the dxy at Au and the 2px at O.
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Fig. 5 Optimized geometry of the model complex I. Mes* groups at phosphorus have been replaced by xylyl groups. Selected bond lengths (Å) and bond angles (°): Au(44)–P(25) 2.311, P(25)–C(22) 1.682, C(22)–C(3) 1.445, C(3)–C(4) 1.409,C(4)–O(19) 1.371; P(24)–Au(44)–P(25) 165.826, Au(44)–P(25)–C(22) 121.050, P(25)–C(22)–C(3) 134.597, C(22)–C(3)–C(4) 128.947, C(3)–C(4)–O(19) 126.254. |
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Fig. 6 H-11, H-12 and H-13 MO of complex I. |
Having rationalized the geometry of the gold and silver complexes, we then turned our attention to the copper complex. The particular structural arrangement in complex 6 can be explained as follows. In d10 ML3 16 VE complexes, the five d orbitals are also filled and but a vacant 3py orbital which is perpendicular to the plane defined by the three ligands is found as the LUMO. In complex 6, this orbital points towards the lone pair at the oxygen atom. Note that the dy2−z2 orbital which is involved in the bonding with the two phosphorus atoms has the right symmetry to interact with the oxygen lone pair (Scheme 9). Therefore the bonding between Cu and O can be described as a classical four-electron interaction involving three orbitals.
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Scheme 9 Interaction diagram showing the two-electron stabilizing interaction occurring between the vacant 3py-orbital at the metal and 2py orbital at the oxygen atom. |
The theoretical structure of complex 6 was calculated. A first calculation carried out on the model complex featuring xylyl groups at phosphorus yielded a structure in which the O–Cu bond distance was found to be by far too long (2.638 Å in IIvs. 2.456(3) Å in 6). Therefore, supposing that in this case, the presence of the two very bulky tert-butyl groups at the ortho positions would probably tend to pucker the copper metal towards the oxygen atom of the furan ligand, calculations were carried out on a complex featuring these two t-Bu groups. The optimization was carried out using the ONIOM method (B3PW91/UFF). A view of the optimized structure is presented in Fig. 7. As can be seen upon examining the theoretical data, there is a very good agreement with experimental metric parameters. Importantly, the Cu–O bond distance at 2.486 Å is rather well reproduced as well as the P–Cu–P angle (132.00 in IIvs. 132.60° in 6).
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Fig. 7 Optimized geometry of the model complex II. Selected bond lengths (Å) and bond angles (°): Cu(26)–P(25) 2.288, P(25)–C(22) 1.683, C(22)–C(3) 1.448, C(3)–C(4) 1.406, C(4)–O(19) 1.380, Cu(26)–N(27) 2.054; P(24)–Cu(26)–P(25) 132.004, Cu(26)–P(25)–C(22) 118.546, P(25)–C(22)–C(3) 129.602, C(22)–C(3)–C(4) 127.453, C(3)–C(4)–O(19) 125.805, P(24)–Cu(26)–N(27) 115.341, P(25)–Cu(26)–N(27) 112.340, P(24)–Cu(26)–P(25) 132.003. |
As expected, molecular orbital analysis revealed that a bonding interaction develops between the oxygen and the copper atom. As can bee seen in Fig. 8 the most important contribution to the bonding is provided by the interaction between the vacant 3py and 3dy2−z2 AOs at Cu and the 2py AO of the oxygen atom (HOMO-19).
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Fig. 8 A view of one of the MO describing the Cu–O bond in the model complex II. The methyl groups of the t-Bu substituents at supermesityl groups have been omitted for clarity. |
31P NMR (121.5 MHz, THF, 298 K): δ 6.6 ppm (1J(P–P) = 577.9, Mes*P), −132.5 ppm (1J(P–P) = 577.9, PMe3).
1H NMR (300 MHz, CD2Cl2, 298 K): δ 1.48 (s, 18H, para C(CH3)3), 1.67 (s, 36H, ortho C(CH3)3), 7.43 (t, 1H, 3J(H–H) = 7.5, H8), 7.51 (t, 1H, 3J(H–H) = 7.3, H2), 7.60 (s, 2H, H12), 7.85 (dd, 1H, 3J(H–H) = 7.5, 4J(H–H) = 3.5, H3), 7.92 (dd, 1H, 3J(H–H) = 7.7, 4J(H–H) = 1.4, H7), 7.99 (dd, 1H, 3J(H–H) = 7.7, 4J(H–H) = 1.2, H9), 8.22 (dd, 1H, 3J(H–H) = 7.6, 4J(H–H) = 1.2, H1), 8.58 (d, 1H, 2J(H–P) = 25.3, H10) 10.75 (s, 1H, CHO). 31P NMR (121.5 MHz, CD2Cl2, 298 K): δ 273.9 ppm. 13C NMR (75.5 MHz, CD2Cl2, 298 K): δ 30.34 (s, para C(CH3)3), 32.96 (d, 3J(C–P) = 7.2, ortho C(CH3)3), 34.12 (s, paraC(CH3)3), 37.42 (s, orthoC(CH3)3), 119.01 (d, 3J(C–P) = 7.1, C7), 120.31 (s, C4 or C9b), 121.20 (s, C13, C15), 122.23 (s, C2), 122.38 (d, 4J(C–P) = 2.8, C9a), 122.98 (d, 4J(C–P) = 3.9, C8), 124.49 (d, 3J(C–P) = 23.0, C3), 124.66 (d, 2J(C–P) = 14.5, C6), 124.89 (s, C9), 124.96 (s, C9b or C4), 125.80 (s, C1), 138.96 (d, 1J(C–P) = 54.4, C11), 149.18 (s, C12, C16), 151.87 (d, 3J(C–P) = 11.3, C5a), 153.28 (s, C14), 155.67 (s, C4a), 166.60 (d, 1J(C–P) = 39.0, C10).
MS: 485 (M + H, 100%).
1NMR (300 MHz, CD2Cl2, 298 K): δ 1.40 (s, 18H, para C(CH3)3), 1.56 (s, 36H, ortho C(CH3)3), 7.37 (t, 2H, 3J(H–H) = 7.6, H2, H8), 7.50 (s, 4H, H13), 7.77 (d, 2H, 3J(H–H) = 5.3, H3, H7), 7.90 (d, 2H, 3J(H–H) = 7.4, H1, H9), 8.48 (m, AA′XX′, m, ∑J = 41.9, H10, H10′). 31P NMR (121.5 MHz, CD2Cl2, 298 K): δ 271.5 ppm. 13C NMR (75.5 MHz, CD2Cl2, 298 K) δ 30.4 (s, para C(CH3)3), 33.0 (d, 4J(C–P) = 3.0, ortho C(CH3)3), 34.1 (s, paraC(CH3)3), 37.4 (s, orthoC(CH3)3), 118.94 (s, C1, C9), 121.01 (s, C13), 122.36 (s, C2, C8), 123.70 (m, C4, C6, C3, C7), 124.57 (vt, AXX′, ∑J(C–P) = 14.4, C9a, C9b), 140.71 (m, AXX′, ∑J(C–P) = 62.7, C11, C11′), 148.90 (s, C12), 151.55 (vt, AXX′, ∑J(C–P) = 12.0, C4a, C5a), 153.17 (s, C14), 167.09 (m, AXX′, ∑J(C–P) = 51.7, C10, C10′). MS: 746 (M + H, 100%).
1H NMR (300 MHz, CDCl3, 298 K): δ 1.40 (s, 18H, para C(CH3)3), 1.68 (s, 36H, ortho C(CH3)3), 7.58 (t, 2H, 3J(H–H) = 7.6, H2, H8), 7.67 (s, 4H, H13), 8.17 (t, 3J(H–H) = 8.8, 2H, H3, H7), 8.37 (m, AA′XX′, m, ∑J = 7.0, H10, H10′). 31P NMR (121.5 MHz, CDCl3, 298 K): δ 200.2. 13C NMR (75.5 MHz, CDCl3, 298 K): δ 32.9 (s, para C(CH3)3), 36.5 (s, ortho C(CH3)3), 37.2 (s, paraC(CH3)3), 40.6 (s, orthoC(CH3)3), 118.2 (s, C9a,9b), 121.1 (m, C1,2,8,9), 122.3 (s, C13), 122.4 (s, C4,6), 131.1 (m, C3,7,11), 148.2 (AA′XX′, m, ∑J = 8.0, C4a,5a), 151.7 (s, C12), 152.9 (s, C14), 157.9 (AA′XX′, m, ∑J = 69, C10,10′).
1H NMR (300 MHz, CD2Cl2, 298 K): δ 1.39 (s, 18H, para C(CH3)3), 1.63 (s, 36H, ortho C(CH3)3), 2.52 (s, H2O), 7.41 (d, 2H, 3J(H–H) = 7.7, H1,9), 7.53 (t, 3J(H–H) = 7.7, 2H, H2,8), 7.63 (s, 4H, H13), 8.18 (dd, 2H, 3J(H–H) = 7.7, 4J(H–P) = 1.3, H3,7), 8.23 (AA′XX′, m, 2H, ∑J = 41.9, H10,10′). 31P NMR (121.5 MHz, CD2Cl2, 298 K): δ 204.9 (d + d, 1J(P–Ag) = 686, 1J(P–Ag) = 596). 13C NMR (75.5 MHz, CD2Cl2, 298 K): δ 31.7 (s, para C(CH3)3), 35.4 (d, 4J(C–P) = 3.0, ortho C(CH3)3), 36.1 (s, paraC(CH3)3), 39.7 (s, orthoC(CH3)3), 122.2 (s, C9a,9b), 123.8 (m, C1,2,8,9), 125.1 (s, C13), 125.7 (s, C4,6), 129.2 (d, 1J(P–C) = 15.5, C11), 133.8 (C), 153.4 (AXX′, m, ∑J(C–P) = 7.5, C4a,5a), 154.2 (s, C12), 156.3 (s, C14), 169.6 (AXX′, m, ∑J(C–P) = 40.3, C10).
1H NMR (300 MHz, CD2Cl2, 298 K): δ 1.38 (s, 18H, para C(CH3)3), 1.61 (s, 36H, ortho C(CH3)3), 7.34 (m, H2,8), 7.50 (m, 2H, H1,9), 7.61 (s, 4H, H13), 8.10 (m, 4H, H3,7,10,10′). 31P NMR (121.5 MHz, CD2Cl2, 298 K): δ 207.6. 13C NMR (75.5 MHz, CD2Cl2, 298 K): δ 31.3 (s, para C(CH3)3), 34.9 (s, ortho C(CH3)3), 35.6 (s, paraC(CH3)3), 39.0 (s, orthoC(CH3)3), 123.1 (s, C9a,9b), 123.3 (s, C1,2,8,9), 123.6 (s, C13), 125.4 (s, C4,6), 129.4 (d, 1J(P–C) = 20, C11), 131.4 (m, ∑J = 26, C3,7), 152.4 (AXX′, m, ∑J(C–P) = 14, C4a,5a), 153.7 (s,C12), 156.2 (s, C14), 163.8 (AXX′, m, ∑J(C–P) = 46, C10).
CCDC reference numbers 275394–275397.
For crystallographic data in CIF or other electronic format see DOI: 10.1039/b508678g
Footnote |
† Electronic supplementary information (ESI) available: View, cartesian coordinates and frequencies of the theoretical structures I and II. See http://dx.doi.org/10.1039/b508678g |
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