Michael S.
Kovacs
,
Vishakha
Monga
,
Brian O.
Patrick
and
Chris
Orvig
*
Medicinal Inorganic Chemistry Group, Department of Chemistry, University of British Columbia, 2036 Main Mall, Vancouver, B.C. V6T 1Z1, Canada. E-mail: orvig@chem.ubc.ca
First published on 25th October 2005
The tripodal amino-phosphinate ligands, tris(4-(phenylphosphinato)-3-benzyl-3-azabutyl)amine (H3ppba·2HCl·H2O) and tris(4-(phenylphosphinato)-3-azabutyl)amine (H3ppa·HCl·H2O) were synthesized and reacted with Al3+, Ga3+, In3+ and the lanthanides (Ln3+). At 2 : 1 H3ppba to metal ratios, complexes of the type [M(H3ppba)2]3+ (M = Al3+, Ga3+, In3+, Ho3+–Lu3+) were isolated. The bicapped [Ga(H3ppba)2](NO3)2Cl·3CH3OH was structurally characterized and was shown indirectly by various techniques to be isostructural with the other [M(H3ppba)2]3+ complexes. Also, at 2 : 1 H3ppba to metal ratios, complexes of the type [M(H4ppba)2]5+ (M = La3+–Tb3+) were characterized, and the X-ray structure of [Gd(H4ppba)2](NO3)4Cl·3CH3OH was determined. At 1 : 1 H3ppba to metal ratios, complexes of the type [M(H4ppba)]4+ (M = La3+–Er3+) were isolated and characterized. Elemental analysis and spectroscopic evidence supported the formation of a 1 : 1 monocapped complex. Reaction of 1 : 1 ratios of H3ppa with Ln3+ and In3+ yielded complexes of the type [M(H3ppa)]3+ (M = La3+–Yb3+) but with Ga3+, complex of the type [Ga(ppa)]·3H2O was obtained. Reaction of 1 : 1 ratios of H3ppa with Ln3+ and In3+ yielded complexes of the type [M(H3ppa)]3+ (M = La3+–Yb3+) but with Ga3+ a neutral complex [Ga(ppa)]·3H2O was obtained. The formation of an encapsulated 1 : 1 complex is supported by elemental analysis and spectroscopic evidence.
Efforts to explore amino-phosphinate ligands with the group 13 metals and the lanthanides have focused on DOTA-type ligands and tren-based tripodal ligands (Scheme 1). The former have been more thoroughly investigated, and a variety of work has been published on their synthesis, structures of their lanthanide complexes, solution behavior and luminescence properties.5–11 1 : 1 Complexes with the lanthanides have been obtained with this type of ligand system and the resulting stereochemistry has been extensively investigated.9,12–15 In addition to the clockwise and counterclockwise wrapping isomers, six diastereomers have been characterized using a variety of NMR techniques.9,12–15 The DOTA phosphinate ligands have also been modified to act as bifunctional chelates.16
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Scheme 1 |
The tripodal ligand H3ppma was found to form 2 : 1 bicapped complexes with group 13 metals and the lanthanides.17–19 The S6 symmetry of these bicapped complexes made unique 27Al, 71Ga and 31P NMR spectroscopic studies amenable that allowed the determination of stability constants below the pH limit of traditional potentiometric techniques.17 Encapsulated 1 : 1 complexes were not obtained in the tripodal amino-phosphinate system. For application in nuclear medicine, this result was a significant setback because 1 : 1 encapsulated complexes are ideal. Such a complex should have higher thermodynamic stability than would a 2 : 1 bicapped complex; the coordination sphere would contain only donors from the ligand, unlike in the monocapped case, where kinetically labile water molecules or counterions are coordinated. Encapsulated 1 : 1 complexes are also much less sensitive to entropic effects that occur at extreme dilution. Kinetically inert complexes with high thermodynamic stability are required to prevent demetallation of the complex in vivo.
To investigate the possibility of isolating 1 : 1 encapsulated complexes containing group 13 metals or the lanthanides, modifications to the tripodal amino-phosphinate ligands are described herein. Attempts were made to prepare new ligands with modifications occurring at the phosphinate R group and/or the amine R group. Although modification at the phosphinate R group proved difficult, synthesis of the benzylated amino-phosphinate ligand tris(4-(phenylphosphinato)-3-benzyl-3-azabutyl)amine (H3ppba) was successful. Two distinct classes of 2 : 1 complexes, and one class of 1 : 1 complex were prepared and characterized with the group 13 metal ions (Al3+, Ga3+, In3+) and the lanthanides. H3ppba was also used as a synthetic precursor to obtain the unique amino-phosphinate ligand tris(4-(phenylphosphinato)-3-azabutyl)amine (H3ppa) by N-debenzylation. H3ppa contains a secondary amine, a functionality that has been elusive in amino-phosphinate systems until this report.
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Scheme 2 |
The possibility of modification at the amine was also investigated. It was expected that the presence of the three bulky benzyl groups would discourage 1 : 1 encapsulated complex formation. Removal of these groups by catalytic hydrogenation, however, afforded the novel secondary amine tripod tris(4-(phenylphosphinato)-3-azabutyl)amine (H3ppa·HCl·H2O) (Scheme 3). The reaction is easily monitored by the loss of the methylene resonance of the benzyl group in the 1H NMR spectrum at 4.45 ppm. Catalytic hydrogenation of N-benzyl groups is known to be difficult because of the propensity of free amines to poison the Pd catalyst.22 High pressure and a large excess of Pd catalyst were required for this reaction to proceed. Hydrogenation reactions are known to produce pure products in high yield; the products of the reaction are H3ppa and toluene, and the problem of purifying the zwitterionic product from the Moedritzer–Irani reaction is avoided. H3ppa is highly water-soluble; the ligand is also soluble in alcohols such as methanol and ethanol.
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Scheme 3 |
Complexes of the ligand H3ppma were clearly shown to be 2 : 1 bicapped complexes of the type [M(H3ppma)2](NO3)3, where M = Al3+, Ga3+, In3+ and Ln3+.17–19 Therefore, the first step of this study was to prepare 2 : 1 ligand : metal complexes for comparison. All complexes were prepared under similar conditions, but two distinct classes of 2 : 1 bicapped complexes were identified.
Reaction of one equivalent of Ga(NO3)3·6H2O with two equivalents of H3ppba·2HCl·H2O in methanol results in the formation of the 2 : 1 bicapped complex [Ga(H3ppba)2](NO3)2Cl·3CH3OH (1). Indicating that complex formation occurs in methanol solution, the 31P NMR singlet of H3ppba shifted upfield from 23.2 to 14.4 ppm for the complex, but little other information is obtained from NMR spectroscopy. A number of metal salts were tried, including chloride, triflate and perchlorate, but only the mixed nitrate/chloride product formed crystals that were amenable to X-ray structural analysis and had consistent composition. Reactions with Al3+, In3+, and the lanthanides Ho3+ through Lu3+ formed the same type of tricationic complex. Isolated yields ranged from 31 to 84%. In the case of the lanthanides, the complexes appeared to have somewhat higher solubility, and yields were difficult to improve. Any attempt to improve the yields by removing the solvent resulted in the formation of glassy solids with inconsistent compositions according to their elemental analyses.
An X-ray structural analysis was performed on a crystal of 1 isolated from the reaction of H3ppba with Ga3+ (Fig. 1, Table 1). The Ga3+ ion is clearly bicapped by two H3ppba ligands; examination of the bond lengths and a difference map indicate that each of the three arm N atoms are protonated on each H3ppba ligand. The ligands are best regarded as neutral zwitterions, thus, the complex has an overall +3 charge. The Ga3+ ion is coordinated only by the phosphinato O atom donors with one symmetry-imposed Ga–O bond length of 1.9501(13) Å. The two H3ppba ligands are related to each other through a crystallographic inversion center at the Ga3+ ion. Although the portion of the unit cell containing [Ga(H3ppba)2]3+ is well established, large void spaces exist where satisfactory modeling of mixed NO3−, Cl− and CH3OH was not possible. Correction of the disordered data in the void spaces resulted in R1 = 0.048 and no peak in the difference map exceeding 0.87 e− Å−3. The elemental analyses for the Ga3+ and other H3ppba complexes strongly support the proposed composition.
a The O atoms are related to each other by symmetry. | |||
---|---|---|---|
Ga(1)–O(1) | 1.9501(13) | C(3)–P(1) | 1.8355(19) |
O(1)–P(1) | 1.5051(13) | C(4)–P(1) | 1.796(2) |
O(2)–P(1) | 1.4923(14) | ||
P(1)–O(1)–Ga(1) | 143.83(8) | O(2)–P(1)–O(1) | 120.24(8) |
O(1)–Ga(1)–O(1*)a | 88.85(6) | O(1)–P(1)–C(3) | 104.05(8) |
O(1)–Ga(1)–O(1*)a 91.15(6) | O(1)–P(1)–C(4) | 110.32(9) | |
O(1)–Ga(1)–O(1*)a | 180.00(7) | O(2)–P(1)–C(3) | 110.76(9) |
C(4)–P(1)–C(3) | 99.51(9) | O(2)–P(1)–C(4) | 109.84(9) |
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Fig. 1 ORTEP diagram of the [Ga(H3ppba)2]3+ cation with the solvent molecules and the aromatic rings removed for clarity; 50% thermal probability ellipsoids are shown. Symmetry labels: i: −y, x − y, z; ii: −x + y, −y, z; iii: −x + 1/3, −y + 2/3, −z + 2/3; iv: y + 1/3, −x + y + 2/3, −z + 2/3; v: x − y + 1/3, x + 2/3, −z + 2/3. |
Analogous to the structurally characterized [In(H3ppma)2]3+ or [Lu(H3ppma)2]3+ complexes,17,19 there is nearly perfect S6 symmetry around the Ga3+ ion. In the case of [In(H3ppma)2]3+, the crystallographic symmetry imposed perfect 90 and 180° angles between the O atoms of the phosphinato ligands.17 The 180° angles in [Lu(H3ppma)2]3+ are crystallographically imposed, and the 88.72(6) and 91.28(6)° angles are extremely close to 90°.19 The unique bond angles in 1 are 180.00, 91.15(6) and 88.85(6)°, therefore, the structure is also an octahedral complex with nearly perfect S6 symmetry. The bond lengths in each of the three complexes are comparable when the ionic radii are corrected for the three different metals.
Also analogous to the two known H3ppma complexes, the coordination of each phosphinato O atom introduces a chiral center at each P atom.17,19 In the crystal structure of 1, only the RRRSSS diastereomer is observed. In order to accommodate the bulk of the phenyl rings on the phosphinate group, the only other diastereomer that is chemically possible is the RRSSSR.17 There is no evidence for the presence of this diastereomer in the solid state in any of the studies to date.
Mass spectral (+LSIMS) data for the entire series of complexes demonstrate clearly that 2 : 1 complexes are formed (see ESI†). Peaks are seen in each case corresponding to the monocationic 2 : 1 and 1 : 1 complexes. Since the ligand peak at 879 is also observed in every case, it is reasonable to conclude that the 1 : 1 complex is formed by fragmentation in the mass spectrometer.
IR spectroscopy shows that complexes of H3ppba with Al3+, Ga3+, In3+ and the lanthanides Ho3+ through Lu3+ are completely isostructural (Fig. 2). The IR spectra have several notable features in the region shown. The peak around 1450 cm−1 is attributed to ν(P–Ph); the sharp peak at 1383 cm−1 arises from ν(NO3); the three large peaks at ca. 1190, 1130, 1070 cm−1 are attributed to ν(P–O); and the peaks around 700 cm−1 are due to ν(P–C) and ν(P–Ph). The intensity and position of all of these peaks remains relatively unchanged in all of the spectra, except in that of Dy3+, which appears to show some additional spectral features (vide infra).
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Fig. 2 IR spectra of [M(H3ppba)2](NO3)2Cl, M as indicated. |
For the series of lanthanides La3+ through Dy3+, however, the IR spectra of the complexes were found to differ greatly from the “Ga3+ type” structures. The elemental analyses (see ESI†) of the Eu3+, Gd3+ and Tb3+ complexes indicate that complexes of the type [Ln(H4ppba)2]5+ are formed wherein the apical nitrogen of each ligand is protonated to afford a +5 complex. Obtaining good elemental data for this class of complex was difficult. Isolated yields were quite low (10–15%), and only Eu3+, Gd3+ and Tb3+ complexes were isolated in pure form. Satisfactory elemental analyses for the La–Sm3+ and Dy3+ complexes were never obtained. Lying on the border between the +5 and +3 complexes, it is possible that Dy3+ formed a mixture of both complex types. The appearance of new features in the IR spectrum of the Dy3+ complex supports this hypothesis.
Despite the fact that pure complexes could not be obtained for all of the early Ln3+ series, the +LSIMS data and IR spectroscopy indicate that these complexes have similarities to the Eu3+, Gd3+ and Tb3+ complexes. The large shift in frequency of the IR bands associated with P and O bonding may be attributed to a change in the intramolecular H-bonding involving the protonated N atoms. If this is the case, the positions of the transitions in the IR spectra are a remarkably sensitive probe of the intramolecular H-bonding. Although the Sm3+ complex has an identical IR spectrum to those of the Gd3+ and Tb3+ complexes, strangely the Eu3+ complex does not, even though its elemental analysis supports its formulation as [Eu(H4ppba)2]5+. The Nd3+ spectrum is identical to the Eu3+ spectrum. The early Ln3+ may have a propensity to form a mixture of 2 : 1 and 1 : 1 complexes (vide infra). This may explain why satisfactory elemental analyses could not be obtained for La3+–Sm3+, and may also explain the presence of the 2 : 1 peaks in the +LSIMS spectra.
From the reaction mixture of Gd3+ and H3ppba, a single crystal was obtained and was used in an X-ray structural analysis (Fig. 3, Table 2). The complex has a bicapped structure similar to that found in 1. Each arm of the tripod is related to the other arms by six-fold crystallographic symmetry. Both the pendant amines and the apical amines are protonated to afford the product complex as [Gd(H4ppba)2](NO3)4Cl·3CH3OH (2). The geometry around Gd3+ is nearly octahedral, with unique bond angles of 180.00, 87.52(6) and 92.48(6)° between the O phosphinato donor atoms. As in 1, the P atoms in 2 have a RRRSSS configuration and this is the only diastereomer seen in the solid state. The presence of the [M(H4ppba)2]5+ complex in the unit cell is very clear, but the six-fold symmetry of the R unit cell complicated the identification of the five counterions and the CH3OH in the large void spaces of the unit cell. This disorder was modeled with help from the analytical data and was refined to R1 = 0.034.
a The O atoms are related to each other by symmetry. | |||
---|---|---|---|
Gd–O(2) | 2.2841(17) | P(1)–C(1) | 1.797(3) |
P(1)–O(1) | 1.500(2) | P(1)–C(7) | 1.845(3) |
P(1)–O(2) | 1.5104(16) | ||
Gd–O(2)–P(1) | 143.85(10) | O(1)–P(1)–C(1) | 112.67(11) |
O(2)–Ga–O(2*)a | 87.52(6) | O(1)–P(1)–C(7) | 108.17(10) |
O(2)–Ga–O(2*)a | 92.48(6) | O(2)–P(1)–C(1) | 107.45(11) |
O(2)–Ga–O(2*)a | 180.00 | O(2)–P(1)–C(7) | 107.94(10) |
O(1)–P(1)–O(2) | 117.45(11) | C(1)–P(1)–C(7) | 101.97(12) |
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Fig. 3 ORTEP diagram of the [Gd(H4ppba)2]5+ cation with the solvent molecules and the aromatic rings removed for clarity; 50% thermal probability ellipsoids are shown. Symmetry labels: i: −y, x − y, z; ii: −x + y, −x, z; iii: −x, −y, −z; iv: y, −x + y, −z; v: x − y, x, −z. |
The switch from [M(H4ppba)2]5+
(M = La3+–Tb3+) to [M′(H3ppba)2]3+
(M′
= Al3+, Ga3+, In3+, Ho3+–Lu3+) is an interesting phenomenon that was not observed in the H3ppma system. It is possible that the size of the metal ion and the nature of the H-bonding network in the uncoordinated upper part of the tripodal ligand have some role in this behavior. It is a well-known fact that early lanthanide trivalent metal ions are larger than late lanthanide trivalent metal ions. The angles between the phosphinate O donors in 1 have two unique angles of 88.88(6) and 91.12(6)°, whereas the unique angles in the 2 are 87.52(6) and 92.48(6)°. It is possible that the larger Ln3+ ions can tolerate this compression of the bond angles better than the smaller Ln3+ and group 13 metal ions. As a result of the compression at the bottom of the tripod, the upper tripod can open up and a rearrangement of the H-bonding network can occur (including the apical N proton) to produce the observed +5 complex. This explanation is also supported by the dramatic change in the PO and P–O stretching frequencies in the IR spectra of the complexes.
In order to investigate further the strange behavior of the 2 : 1 La3+–Sm3+ complexes, including the possibility of 1 : 1 complex formation, a study of the system in 1 : 1 ratios was initiated. Under similar conditions to those which produced the 2 : 1 complexes, 1 : 1 ratios of M(NO)3 (M = La3+–Lu3+) and H3ppba were reacted in methanol. These reactions afforded complexes of the type [M(H4ppba)]4+ in 14–34% yield. Upon mixing of the starting materials, a finely-divided precipitate immediately formed for most of the lanthanides. Towards the end of the series (Tm3+–Lu3+), no precipitate formed and prismatic crystals appeared corresponding to the [M(H3ppba)2]3+ complexes over a period of 48 h. This was verified crystallographically for the Yb3+ complex (the full solution of the structure was not completed once this was discovered).
Unlike those of the 2 : 1 complexes, the +LSIMS mass spectra of the 1 : 1 complexes show no substantial evidence of 2 : 1 peaks. In some of the complexes, 2 : 1 peaks were observed at trace levels (20× gain). The possibility exists that a small excess of ligand may have been present in these cases. Lanthanide nitrate salts are very hygroscopic and the excess water would not have been accounted for if it were present.
The IR spectra of the 1 : 1 complexes La3+–Er3+ are remarkably similar. The ν(NO3) peak is at 1384 cm−1, which is the same frequency as that seen in the 2 : 1 complexes. With the exception of complexes of La3+ Sm3+, and Er3+ which have an additional peak at 1238 cm−1, all the other complexes share similar features in the ν(PO) region of the spectrum (1303, 1181, 1134, 1054 cm−1). The IR spectrum of the Ho3+ complex has a peak at 1238 cm−1 which is seen as a small shoulder on the broad peak at 1181 cm−1. The fact that this same peak is seen the 2 : 1 Nd3+ and Eu3+ IR spectra (see electronic supplementary information) supports the possibility that a 1 : 1 complex may be present depending on the exact conditions of preparation of the early lanthanide 2 : 1 complexes. The IR spectra of the late lanthanide 2 : 1 complexes (Fig. 2) demonstrate that these metals have no propensity to form 1 : 1 complexes under these conditions.
With a small variation in hydration, the elemental analyses for the 1 : 1 complexes are very consistent. All the complexes appear to have the formulation [M(H4ppba)](NO3)3Cl·xH2O. As expected, the carbon content is much lower than in any of the 2 : 1 complexes, and the nitrogen content is much higher, owing to the lack of a second carbon-rich ligand. The analyses of the Ho3+ and Er3+ complexes appear to have slightly higher levels of carbon, perhaps because of the preference of the late Ln3+ to form 2 : 1 complexes in this system.
Because all the 1 : 1 complexes precipitate as highly insoluble powders, no crystals suitable for an X-ray structural analysis could be obtained. The complexes only have limited solubility, even in solvents such as DMSO; after dissolution they are unrecoverable. Given that the elemental analysis supports the formulation [M(H4ppba)]4+, wherein all four N atoms are protonated, it seems highly unlikely that an encapsulated complex is formed. The ν(NO3) in the IR spectra is identical to that of the two structurally characterized 2 : 1 complexes, therefore, it is unlikely that the NO3− ligands are coordinated to Ln3+ in the 1 : 1 complexes. Given this combined evidence, the most reasonable assumption is that the complexes are monocapped, with 3–5 H2O molecules completing the coordination sphere.
Reaction of tris(4-(phenylphosphinato)-3-azabutyl)amine (H3ppa·HCl·H2O) with Ga(NO3)3·6H2O in methanol at a 1 : 1 molar ratio results in the formation of a finely-divided white precipitate after standing for 48 h. Elemental analysis of this precipitate gives the composition [Ga(ppa)]·3H2O (6). Clearly, this is a very interesting result because it is possible that an encapsulated 1 : 1 complex has formed. The lack of counterions strongly suggests that the pendant N donors are not protonated NH2+, but rather the neutral NH. Unlike the [M(H4ppba)]4+ complexes described previously, the formation of an encapsulated 1 : 1 complex is a distinct possibility. The +LSIMS data support the formulation as 1 : 1; a large peak at m/z 675 corresponding to [Ga(Hppa)]+ is seen. Only a trace peak is seen at m/z 1285 corresponding to the 2 : 1 complex [GaH4(ppa)2]+. In order to investigate further this behavior and to compare the reactivity of lanthanides with H3ppa, similar reactions were carried out with indium and lanthanide (M = La3+–Yb3+) nitrate salts. A study of the system in 1 : 1 ratios of M(NO3)3 : H3ppa in methanol was initiated to explore the possibility of 1 : 1 complex formation. These reactions afforded complexes of the type [M(H3ppa)]3+, just as the lanthanide complexes with H3ppba in good yields (50–83%). Upon mixing of the starting materials, a finely-divided precipitate immediately formed for the indium complex and most of the lanthanides. It was interesting to note that the indium complex with this ligand forms complexes resembling the lanthanides rather than gallium.
Analogous to the 1 : 1 M3+ : H3ppba complexes, the +LSIMS and ESIMS mass spectra of the 1 : 1 M3+ H3ppa complexes show no substantial evidence of 2 : 1 peaks (see ESI†). In some of the complexes, 2 : 1 peaks were observed at trace levels (20× gain). Lanthanide nitrate salts are very hygroscopic and the excess water would not have been accounted for if it were present. With a small variation in hydration, the elemental analyses for the 1 : 1 complexes are very consistent. All the Ln complexes appear to have the formulation [M(H3ppa)](NO3)3Cl·xH2O whereas the In complex was isolated as [In(H3ppa)](NO3)3Cl·2CH3OH.
Because all of the In and Ln complexes precipitate as highly insoluble powders, crystals suitable for an X-ray structural analysis could not be obtained. The complexes only have limited solubility, even in solvents such as DMSO; after dissolution they are unrecoverable. Given that the elemental analysis supports the formulation [M(H3ppa)]3+, wherein three of the N atoms are protonated, it seems highly unlikely that an encapsulated complex is formed. The ν(NO3) in the IR spectra is identical to that of the two structurally characterized 2 : 1 complexes of these metal ions with H3ppba, therefore, it is unlikely that the NO3− ligands are coordinated to In3+ and Ln3+ in the 1 : 1 complexes. Given this combined evidence, the most reasonable assumption is that the complexes are monocapped, with 3–5 H2O molecules (or CH3OH in case of In) completing the coordination sphere.
The IR spectra of the H3ppa ligand and the Ga, In and Ln complexes have several notable features. One of the ν(PO) bands shifts from 1188 to 1181 cm−1 upon complex formation. The band at 954 cm−1 in the free ligand disappears completely. Unlike all other complexes with H3ppa, there is no indication of a free nitrate in the IR spectrum of the gallium complex at ca. 1385 cm−1. The broad ν(NH) peak shifts from 3414 cm−1 in the free uncomplexed ligand to 3421 cm−1 in the complexes, which may indicate that the N donors are involved in complex formation. The seemingly unusual strengthening of the N–H bond upon coordination may occur because the N atom is first deprotonated from NH2+ to NH, then is subsequently coordinated to Ga3+. Since this is a two-step process, it is difficult to state with absolute certainty that the N donors are coordinated to Ga3+ on the basis of IR spectroscopy alone. With respect to the free ligand and the gallium complex, the IR spectra of all other complexes show more distinct features in the fingerprint region.
The 31P NMR spectrum of 6 in methanol is complicated and contains at least seven resonances between 23.7 and 24.9 ppm, shifted downfield from the ligand in which it is seen as a singlet at 21.1 ppm. Unlike the gallium complex, the 31P NMR resonances of In and La complexes shifted upfield to 16.1–19.2 ppm. The 1H NMR spectra of the complexes and the free ligand demonstrate significant shifts of the CH2 groups compared to the free ligand. Although the speciation in solution is complicated, the shifts of the pendant CH2 arms are strongly indicative of pendant N atom coordination to the metal. It is plausible to regard the complex as encapsulated, but in the absence of X-ray structural data, it can not be stated for certain.
CCDC reference numbers 275600 and 275601.
See http://dx.doi.org/10.1039/b507905e for crystallographic data in CIF or other electronic format.
Footnote |
† Electronic supplementary information (ESI) available: Experimental section. See http://dx.doi.org/10.1039/b507905e |
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