We report a self-recognition phenomenon based on an assembly process in a homogeneous dilute aqueous solution of two nano-scaled, spherical polyprotic metal oxide-based macroions (neutral species in crystals), also called Keplerates of the type [(linker)₃₀(pentagon)₁₂]≡[{M(H₂O)}₃₀{(Mo)Mo₅}₁₂] where M is Fe(III) or Cr(III). Upon deprotonation of the neutral species, the resulting macroions assemble into hollow "blackberry"-type structures through very slow homogeneous dimer-oligomerization processes. Although the geometrical surface structures of the two macroions are practically identical, mixtures of these form homogeneous superstructures, rather than mixed species. The phase separation is based on the difference in macroionic charge densities present during the slow homogeneous dimer or oligomer formation. The surface water ligands' residence times of Cr(III) and Fe(III) differ markedly and lead to very different interfacial water mobilities between the Keplerates.
The 16-Fe(III)-containing 48-tungsto-8-phosphate [P(8)W(48)O(184)Fe(16)(OH)(28)(H(2)O)(4)](20-) (1) has been synthesised and characterised by IR and ESR spectroscopy, TGA, elemental analyses, electrochemistry and susceptibility measurements. Single-crystal X-ray analyses were carried out on Li(4)K(16)[P(8)W(48)O(184)Fe(16)(OH)(28)(H(2)O)(4)]66 H(2)O2 KCl (LiK-1, orthorhombic space group Pnnm, a=36.3777(9) A, b=13.9708(3) A, c=26.9140(7) A, and Z=2) and on the corresponding mixed sodium-potassium salt Na(9)K(11)[P(8)W(48)O(184)Fe(16)(OH)(28)(H(2)O)(4)].100 H(2)O (NaK-1, monoclinic space group C2/c, a=46.552(4) A, b=20.8239(18) A, c=27.826(2) A, beta=97.141(2) degrees and Z=4). Polyanion 1 contains--in the form of a cyclic arrangement--the unprecedented {Fe(16)(OH)(28)(H(2)O)(4)}(20+) nanocluster, with 16 edge- and corner-sharing FeO(6) octahedra, grafted on the inner surface of the crown-shaped [H(7)P(8)W(48)O(184)](33-) (P(8)W(48)) precursor. The synthesis of 1 was accomplished by reaction of different iron species containing Fe(II) (in presence of O(2)) or Fe(III) ions with the P(8)W(48) anion in aqueous, acidic medium (pH approximately 4), which can be regarded as an assembly process under confined geometries. One fascinating aspect is the possibility to model the uptake and release of iron in ferritin. The electrochemical study of 1, which is stable from pH 1 through 7, offers an interesting example of a highly iron-rich cluster. The reduction wave associated with the Fe(III) centres could not be split in distinct steps independent of the potential scan rate from 2 to 1000 mV s(-1); this is in full agreement with the structure showing that all 16 iron centres are equivalent. Polyanion 1 proved to be efficient for the electrocatalytic reduction of NO(x), including nitrate. Magnetic and variable frequency EPR measurements on 1 suggest that the Fe(III) ions are strongly antiferromagnetically coupled and that the ground state is tentatively spin S=2.
Dedicated to Professor Francis SØcheresse on the occasion of his 60th birthdayPolygons can be placed on spherical surfaces such that periodical structures of a cyclic nature result, while these can be considered as discrete models for two-dimensional (extended) structures. If we wish to construct a chemical structure on a spherical capsule surface in the same way, we have to remember that 1) pentagons are the basic units for sphere constructions, as is well known, for example, from virus structures, 2) they exist, for example, in the form of { ( [5b]). However, until now it was not possible to synthesize a spherical capsule surface directly by the addition of linkers to the pentagonal units that are available in a dynamic library. [1][2][3][4][5] It is significant that in the Keplerates the linkers describe generic Archimedean solids: in the case of dinuclear linkers M 2 a distorted truncated icosahedron, {M 2 } 30 , and in the case of mononuclear linkers the unique icosidodecahedron (Figure 1) [6] {M 30 }, which has-geometrically speaking-linked M 3 triangles. Surprisingly the related consequences for chemistry have not been discussed until now. In the {M 30 } situation, there is a network of corner-shared triangles on the sphere surface, this can result unique magnetic properties as in the case of the "classical" Keplerate {(Mo VI )Mo . [7, 8] This is the first laboratory example of a "zero-dimensional" system that at low temperatures embodies characteristics of geometrical frustration/magnetic ordering [8b] which otherwise have only been observed in selected one-, two-, and three-dimensional lattice spin systems.[9] Herein we report on the spherical cluster 1 a where the twelve {(Mo VI )Mo VI 5 } type units fix 30 d 1 V IV linkers/centers with spin S = 1/2 in the form of an icosidodecahedron, and thus 1) demonstrating for the first time that the spherical capsule/Keplerate can be directly constructed from the mononuclear linkers and the appropriate molybdate library, [5c] 2) providing the chance to obtain new information regarding the unique molecular magnetism of the {M 30 } type network of linkers/triangles, and 3) clarifying the quantum effects of the spin S = 1/2 vanadyl linkers especially in connection with the two-dimensional S = 1/2 KagomØ lattice which contains linked triangles and exhibits unique magnetic properties.[9a]After adding vanadyl sulfate to an acidified molybdate solution, in the presence of K + ions, compound 1 precipitates after some time in high yield. (A simpler expression for the
Dedicated to Professor Peter Day on the occasion of his 70th birthdayIn the field of polyoxometalate chemistry, porous spherical molybdenum oxide-based clusters of the type {(Mo VI )Mo VI 5 } 12 (linker) 30 , [1] called Keplerates, [2a,b] are notable not only from an aesthetic point of view [2c] but also because they show properties of interest for different areas of science. Some of these clusters can act as artificial cells exhibiting gated pores while interacting specifically with their environments; others are of interest for several aspects of materials science. [3][4][5] In detail, of interest are a) solution properties in connection with a new type of assembly process leading to vesicles, including magnetic ones, [6a,b] b) the option to employ the characteristic interactions with amphiphiles for the generation of monolayers and Langmuir-Blodgett films [6c] as well as highly ordered honeycomb nanostructures at airwater interfaces, [6d] c) the integration into sol-gel-derived silica to obtain unprecedented hybrids, [6e] and d) the discovery of novel magnetic properties, [6f]
Our measurements of the differential susceptibility ∂M/∂H of the frustrated magnetic molecules {Mo72Fe30} and {Mo72Cr30} reveal a pronounced dependence on magnetic field (H) and temperature (T ) in the low H -low T regime, contrary to the predictions of existing models. Excellent agreement with experiment is achieved upon formulating a nearest-neighbor classical Heisenberg model where the 60 nearest-neighbor exchange interactions in each molecule, rather than being identical as has been assumed heretofore, are described by a two-parameter rectangular probability distribution of values of the exchange constant. We suggest that the probability distribution provides a convenient phenomenological platform for summarizing the combined effects of multiple microscopic mechanisms that disrupt the idealized picture of a Heisenberg model based on a single value of the nearest-neighbor exchange constant.
The deliberate synthesis of the Keplerate [K(20) subset{(W)W(5)O(21)(SO(4))}(12)(VO)(30)(SO(4))(H(2)O)(63)](18-) with 20 pores all closed by K(+) in a supramolecular fashion proves that it is possible to follow new routes in polyoxotungstate chemistry based on pentagonal {(W)W(5)}-type units and to tune magnetic exchange couplings in {(M)M(5)}(12)M'(30) type Keplerates.
Variable-temperature 17O NMR experiments were conducted on the nanometer-sized Keplerate Mo72Fe30 cluster, with the stoichiometry [Mo72Fe30O252(CH3COO)12[Mo2O7(H2O)]2[H2Mo2O8(H2O)](H2O)91]. approximately 150H2O. This molecule contains on its surface 30 Fe(H2O) groups forming a well-defined icosidodecahedron, and we estimated the rates of exchange of the isolated >FeIII-OH2 waters with bulk aqueous solution. Both longitudinal and transverse 17O-relaxation times were measured, as well as chemical shifts, and these parameters were then fit to the Swift-Connick equations in order to obtain the rate parameters. Correspondingly, we estimate: k(ex)298 = 6.7(+/-0.8) x 106 s-1, which is about a factor of approximately 4 x 104 times larger than the corresponding rate coefficient for the Fe(OH2)63+ ion of k(ex)298 = 1.6 x 102 s-1 (Grant and Jordan, 1981; Inorg. Chem. 20, 55-60) and DeltaH and DeltaS are 26.3 +/- 0.6 kJ mol-1 and -26 +/- 0.9 J mol-1 K-1, respectively. High-pressure 17O NMR experiments were also conducted, but the cluster decomposed slightly under pressure, which precluded confident quantitative estimation of the DeltaV. However, the increase in the reduced transverse-relaxation time with pressure suggests a dissociative character, such as a D or Id mechanism. The enhanced reactivity of waters on the Mo72Fe30 cluster is associated with an increase in the FeIII-OH2 bond length in the solid state of approximately 0.1 A relative to the Fe(OH2)63+ ion, suggesting that a correlation exists between the FeIII-OH2 bond length and k(ex)298. Although there are only few high-spin Fe(III) complexes where both exchange rates and structural data are available, these few seem to support a general correlation.
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