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Kinetics and equilibria of the interactions of hydroxamic acids with gallium(III) and indium(III).

The thermodynamics and kinetics of the binding of Ga(III) and In(III) to two hydroxamic acids, C6H5-C(O)N(OH)H (BHA) and C6H5-C(O)N(OH)C6H5 (PBHA), have been investigated in acidic media. Spectrophotometric titrations in the UV region reveal that, with excess metal, only the chelate ML forms, whereas the concentration of the protonated species, MHL, is negligible. The thermodynamic parameters indicate that the driving force for formation of ML from MOH2+ and HL is mainly enthalpic, with entropic contributions favoring InL2+ and disfavoring GaL2+ formation. The kinetic (stopped-flow) experiments are interpreted on the basis of two parallel reaction paths both involving reaction of the undissociated ligand (HL): (a) M + HL <==> MHL <==> ML + H where MHL is in a steady state and (b) MOH + HL <==> ML + H2O. Whereas gallium binding to BHA and PBHA proceeds mainly through path b, indium binding to PBHA proceeds through both a and b paths. The rates of both the a and b steps are ligand dependent. Two alternative mechanisms are proposed. The first is based on the electronic characteristics of the ligands and is of the Ia type. The second, of the Id type, assumes that a considerable fraction of the ligand is unreactive owing to intramolecular hydrogen bonding (possibly including a water molecule) which blocks the reaction site. The reasons for preferring the former mechanism are discussed.

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Influence of ligand rigidity and ring substitution on the structural and electronic behavior of trivalent iron and gallium complexes with asymmetric tridentate ligands.

Species 1-6 are [M(III)(L)2]ClO4 complexes formed with the PhO--CH=N-CH2-Py imines, (L(I))- and (L(tBuI))-, and PhO--CH2-NH-CH2-Py amines, (L(A))- and (L(tBuA))-, in which PhO- is a phenolate ring and Py is a pyridine ring and the prefix tBu indicates the presence of tertiary butyl groups occupying the positions 4 and 6 of the phenol ring. Monometallic species with d5 high-spin iron (1, 2, 3, 4) and d10 gallium (5, 6) were synthesized and characterized to assess the influence of the ligand rigidity and the presence of tertiary butyl-substituted phenol rings on their steric, electronic, and redox behavior. Characterization by elemental analysis, mass spectrometry, IR, UV-visible, and EPR spectroscopies, and electrochemistry has been performed, and complexes [FeIII(L(tBuI))2]ClO4 (2), [FeIII(L(tBuA))2]ClO4 (4), and [Ga(III)(L(tBuI))2]ClO4 (5) have been characterized by X-ray crystallography. The crystal structures show the imine ligands meridionally coordinated to the metal centers, whereas the amine ligands are coordinate in a facial mode. Cyclic voltammetry shows that the complexes with the ligands (L(tBuI))- and (L(tBuA))- were able to generate ligand-based phenoxyl radicals, whereas unsubstituted ligands displayed ill-defined redox processes. EPR spectroscopy supports high-spin configurations for the iron complexes. UV-visible spectra are dominated by charge-transfer phenomena, and imine compounds exhibit dramatic hyperchromism when compared to equivalent amines. The tertiary butyl groups on the phenolate ring enhance this trend. Detailed B3LYP/6-31G(d)-level calculations have been used to account for the results observed.

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Theoretical investigation of paramagnetic diazabutadiene gallium(III)-pnictogen complexes: insights into the interpretation and simulation of electron paramagnetic resonance spectra.

The electronic structures and the spin density distributions of the paramagnetic gallium 1,4-diaza(1,3)butadiene (DAB) model systems [((t)Bu-DAB)Ga(I)[Pn(SiH3)2]]* and the related dipnictogen species [((t)Bu-DAB)Ga[Pn(SiH3)2]2]* (Pn = N, P, As) were studied using density functional theory. The calculations demonstrate that all systems share a qualitatively similar electronic structure and are primarily ligand-centered pi-radicals. The calculated electron paramagnetic resonance (EPR) hyperfine coupling constants (HFCCs) for these model systems were optimized using iterative methods and were used to create accurate spectral simulations of the parent radicals [((t)Bu-DAB)Ga(I)[Pn(SiMe3)2]]* (Pn = N, P, or As) and [((t)Bu-DAB)Ga[Pn(SiMe3)2]2]* (Pn = P or As), the EPR spectra of which had not been simulated previously due to their complexity. Excellent agreement was observed between the calculated HFCCs and the optimum values, which can be considered the actual HFCCs for these systems. The computational results also revealed inconsistencies in the published EPR data of some related paramagnetic group 13-DAB complexes.

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Two new structurally related strontium gallium nitrides: Sr4GaN3O and Sr4GaN3(CN2).

The strontium gallium oxynitride Sr(4)GaN(3)O and nitride-carbodiimide Sr(4)GaN(3)(CN(2)) are reported, synthesized as single crystals from molten sodium at 900 degrees C. Red Sr(4)GaN(3)O crystallizes in space group Pbca (No. 61) with a = 7.4002(1) Angstroms, b = 24.3378(5) Angstroms, c = 7.4038(1) Angstroms, and Z = 8, as determined from single-crystal X-ray diffraction measurements at 150 K. The structure may be viewed as consisting of slabs [Sr(4)GaN(3)](2+) containing double layers of isolated [GaN(3)](6-) triangular anions arranged in a "herringbone" fashion, and these slabs are separated by O(2-) anions. Brown Sr(4)GaN(3)(CN(2)) has a closely related structure in which the oxide anions in the Sr(4)GaN(3)O structure are replaced by almost linear carbodiimide [CN(2)](2-) anions [Sr(4)GaN(3)(CN(2)): space group P2(1)/c (No. 14), a = 13.4778(2) Angstroms, b = 7.4140(1) Angstroms, c = 7.4440(1) Angstroms, beta = 98.233(1) degrees, and Z = 4].

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Synthesis, structural characterization, and theoretical studies of complexes of magnesium and calcium with gallium heterocycles.

The magnesium- and calcium-gallium heterocycle complexes [Mg{Ga[(ArNCH)2]}2(THF)3] and [Ca{Ga[(ArNCR)2]}2(THF)4], R = H or Me, Ar = C6H3Pr(i)2-2,6, have been prepared via the reduction of [I2Ga{(ArNCR)2}] with the group 2 metal in tetrahydrofuran. The mechanisms of the reactions have been elucidated, and the crystal structures of the complexes exhibit the first structurally authenticated Ga-Mg and Ga-Ca bonds in molecular species. Theoretical studies suggest that the heterocycle-group 2 metal interactions have significant ionic character.

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Methanolysis as a route to gallium(III) clusters: synthesis and structural characterization of a decanuclear molecular wheel.

Treatment of a methanolic solution of gallium(III) nitrate with lithium hydroxide in the presence of benzilic acid resulted in the decanuclear cluster [Ga(OMe)2{O2CC(OH)Ph2}]10 (1). The metal and the organic components have assembled to form a cyclic molecule that adopts the structure of a wheel. The 10 Ga(III) ions are approximately coplanar and are coordinated in a distorted octahedral manner by six oxygen atoms. The integrity of the molecular wheel is retained in solution, as evidenced by the 1NMR spectrum of 1 in DMSO-d6, while no signal in the 71Ga NMR could be detected.

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Stereochemical Consequences of the Bismuth Atom Electron Lone Pair, a Comparison between MX(6)E and MX(6) Systems. Crystal and Molecular Structures of Tris[N-(P,P-diphenylphosphinoyl)-P,P-diphenylphosphinimidato]bismuth(III), [Bi{(OPPh(2))(2)N}(3)], -indium(III), [In{(OPPh(2))(2)N}(3)].C(6)H(6), and -gallium(III), [Ga{(OPPh(2))(2)N}(3)].CH(2)Cl(2).

The tetraphenylimidodiphosphinate [N-(P,P-diphenylphosphinoyl)-P,P-diphenylphosphinimidate] ion forms stable tris-chelates with the Bi(III), In(III), and Ga(III) cations. The crystal and molecular structures of [M{(OPPh(2))(2)N}(3)] (M = Ga, In, Bi) were determined by X-ray diffractometry. The geometry around the bismuth atom in compound 3 displays an approximately C(3)(v)() symmetry. This arrangement suggests the presence of a stereoactive lone pair of electrons, which is located in one of the triangular octahedral faces. Derivative 3 crystallizes in the triclinic space group P&onemacr; with Z = 2, a = 14.006(6) Å, b = 14.185(4) Å, c = 17.609(8) Å, alpha = 88.45(2) degrees, beta = 79.34(2) degrees, and gamma = 78.23(2) degrees. The structures of the gallium(III) and indium(III) tris-chelate oxygen-based complexes (1 and 2, respectively) were compared with the bismuth analogue in order to determine the ligand steric bulk influence on the coordination sphere in the absence of the electron lone pair. Complex 1 crystallizes as the [Ga{(OPPh(2))(2)N}(3)].CH(2)Cl(2) solvate in the triclinic space group P&onemacr;; Z = 2, a = 13.534(4) Å, b = 13.855(4) Å, c = 18.732(7) Å, alpha = 95.48(2) degrees, beta = 98.26(2) degrees, and gamma = 97.84(2) degrees. Crystal data for the benzene solvate of 2, [In{(OPPh(2))(2)N}(3)].C(6)H(6): triclinic space group P&onemacr;, Z = 2, a = 13.542(9) Å, b = 15.622(3) Å, c = 18.063(5) Å, alpha = 98.21(1) degrees, beta = 104.77(0) degrees, and gamma = 92.260(0) degrees.

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Gallium and Indium Complexes of Bis(amino thiol) (N(2)S(2)) Ligands.

Three methods have been developed to prepare gallium and indium complexes of three tetradentate N(2)S(2) ligands of the general formula M(N(2)S(2))R (M = Ga, In; R = Cl, Br, SCN, O(2)CC(6)H(5)-O,O'). The ancillary ligand (Cl, SCN, O(2)CC(6)H(5)-O,O') was varied with the tetradentate ligand BAT-TM. X-ray crystallography shows that the coordination geometry about the d(10) metal ion is influenced by the steric requirements of the ligands. X-ray crystallography of four molecules results in the following data: GaCl(BAT-TM) (1), formula = C(10)H(22)ClGaN(2)S(2), space group = Pnma, a = 12.387(4) Å, b = 21.116(6) Å, c = 5.986(2) Å, V = 1565.8(9) Å(3), Z = 4; InCl(BAT-TM) (2), formula = C(10)H(22)ClInN(2)S(2), space group = Pnma, a = 12.968(9) Å, b = 29.29(1) Å, c = 5.866(2) Å, V = 1620(2) Å(3), Z = 4; InNCS(BAT-TM) (3), formula = C(11)H(24)ClInN(3)S(3), space group = Pbca, a = 11.812(3) Å, b = 11.679(3) Å, c = 24.238(9) Å, V = 3449.7 (17) Å(3), Z = 8; In(O,O'-O(2)CC(6)H(5))(BAT-TM) (4), formula = C(19)H(29)O(2)InN(2)S(2), space group = P2(1)/n, a = 10.783(2) Å, b = 18.708(4) Å, c = 12.335(4) Å, V = 2321.7(9) Å(3), Z = 4. Proton NMR studies show that the complexes are stable in solution; in polar solvents such as acetonitrile, for certain molecules, two metal-ligand complexes are observed. Similarly, two metal-ligand complexes are seen in NMR data taken in 80% acetonitrile/20% D(2)O (pD = 4.6) mixture. HPLC studies (acetonitrile/50 mM sodium acetate, pH = 4.6) show that the lipophilicity of the ligand determines the retention time of the complex.

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Ring Systems Containing Anionic and Cationic Gallium Centers: Structural and Bonding Considerations.

The metathetical reaction of 2-(dimethylamino)benzyllithium (Bz(N)Li) with GaCl(3) afforded the salt [Bz(N)(2)Ga][GaCl(4)] (4), the X-ray crystal structure of which revealed a four-coordinate cationic gallium center featuring two Ga-C sigma-bonds and two N-->Ga dative bonds. (Crystal data for 4: monoclinic, space group P2(1)/n, a = 11.519(2) Å, b = 18.254(4) Å, c = 12.506(3) Å, beta = 117.40(3) degrees, V = 2334.6(9) Å(3), Z = 4, R = 0.545). Two Ga.Cl interionic contacts, while somewhat long, are sufficiently strong to render the geometry of 4(+)() roughly midway between tetrahedral and octahedral. Treatment of 1,4-di-tert-butyl-1,4-diazabutadiene (DAB) with 2 equiv of GaCl(3) afforded [(DAB)GaCl(2)][GaCl(4)] (7), which, by means of X-ray analysis, was shown to possess a cation (7(+)()) with localized C=N bonds and N-->Ga dative interactions with a [GaCl(2)](+) moiety. (Crystal data for 7: orthorhombic, space group Pbca, a = 11.882(2) Å, b = 17.289(3) Å, c = 20.424(4) Å, V = 4195.5(11) Å(3), Z = 8, R = 0.460). The structure of 7(+)() is relevant to discussions of the bonding in both neutral DAB complexes of the group 13 elements and the skeletally isoelectronic anion [Me(4)C(4)GaCl(2)](-) (9(-)()). The structure of the [NEt(4)](+) salt of the latter (9) has been determined by X-ray diffraction. (Crystal data for 9: monoclinic, space group P2(1)/n, a = 9.967(1) Å, b = 13.073(2) Å, c = 15.345(2) Å, beta = 96.76(1) degrees, V = 1985.5(4) Å(3), Z = 4, R = 0.721).

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Effect of Pyridyl Donors in the Chelation of Aluminum(III), Gallium(III), and Indium(III).

A new preparation of N,N'-bis(2-pyridylmethyl)ethylenediamine-N,N'-diacetic acid (H(2)bped) is reported, and its properties of complexation with Al(III), Ga(III), In(III), and Co(III) are investigated. The molecular structure of the cobalt(III) complex [Co(bped)]PF(6).CH(3)CN.H(2)O (C(20)H(25)CoF(6)N(5)O(5)P) has been solved by X-ray methods; the complex crystallizes in the triclinic space group P&onemacr;, with a = 10.611(2) Å, b = 12.720(2) Å, c = 9.868(1) Å, alpha = 102.70(1) degrees, beta =93.60(1) degrees, gamma = 106.96(1) degrees, and Z = 2. The structure was solved by direct methods and was refined by full-matrix least-squares procedures to R = 0.041 (R(w) = 0.038) for 4312 reflections with I > 3sigma(I). The Co(III) ion is coordinated in a distorted octahedral geometry with an N(4)O(2) donor atom set. The carboxylato oxygen atoms are coordinated trans, while the pyridyl nitrogen atoms are coordinated cis. The largest distortion from octahedral geometry is the N(pyridyl)-Co-N(pyridyl) angle of 107 degrees. Complex formation constants have been measured at 25 degrees C (&mgr; = 0.16 M (NaCl)). log K([M(bped)](+)) (log K([M(bped)(OH)])): M = Al, 10.85 (6.37); M = Ga, 19.89 (15.62); M = In, 22.6 (15.44). A protonated complex was also detected, [Ga(Hbped)](2+), log K = 21.79. The order of stability is In(III) > Ga(III) > Al(III) for the binary species, [M(bped)](+). The solution structures of the complexes have been probed in multinuclear NMR ((1)H, (13)C, (27)Al) studies, and these solution structures are compared with the solid state structure of the cobalt(III) complex. The complexes [In(bped)](+) and [In(bped)(OH)] are proposed to contain 7-coordinate In(III) with water and hydroxide completing the respective coordination spheres. The gallium complexes are proposed to be 6-coordinate: the [Ga(Hbped)](2+) complex contains a nondeprotonated carboxylic acid group which is not coordinated, and [Ga(bped)(OH)] contains a coordinated hydroxide which displaces a carboxylato donor. The [Al(bped)(OH)] complex may be 5-coordinate on the basis of its downfield (27)Al NMR chemical shift, 54 ppm.

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Synthesis and Structure of One-, Two-, and Three-Dimensional Alkaline Earth Metal Gallium Nitrides: Sr(3)Ga(2)N(4), Ca(3)Ga(2)N(4), and Sr(3)Ga(3)N(5).

We report the structures of three new alkaline earth metal gallium nitrides synthesized as crystals from the elements in sealed Nb tubes at 760 degrees C using Na/Sr and Na/Ca melts as growth media. The materials are all transparent insulators. Yellow Sr(3)Ga(2)N(4) is isostructural with the previously reported Ba(3)Ga(2)N(4) and Sr(3)Al(2)N(4). It crystallizes in Pnna (No. 52) with a = 5.9552(6) Å, b = 10.2753(8) Å, c = 9.5595(9) Å, and Z = 4. It contains infinite chains, [GaN(4/2)(3)(-)], of trans-edge-shared tetrahedra extending along the b axis. Colorless Ca(3)Ga(2)N(4) is isostructural with Ca(3)Al(2)As(4) and gamma-Ca(3)Al(2)N(4). It crystallizes in C2/c (No. 15) with a = 10.6901(11) Å, b = 8.3655(7) Å, c = 5.5701(4) Å, beta = 91.194(6) degrees, and Z = 4. It contains infinite sheets, [GaN(4/2)(3)(-)], of edge- and corner-sharing tetrahedra in the bc plane. Orange-yellow Sr(3)Ga(3)N(5) has a new structure; it crystallizes in P&onemacr; (No. 2) with a = 5.9358(6) Å, b = 7.2383(8) Å, c = 8.6853(12) Å, alpha = 108.332(10) degrees, beta = 103.783(9) degrees, gamma = 95.326(8) degrees, and Z = 2. It is one of the few materials prepared from Na melts which has an infinite three-dimensional framework structure. It contains a [Ga(3)N(5)(6)(-)] framework of edge- and corner-sharing GaN(4) tetrahedra.

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Cyclic Metalloporphyrin Trimers: (1)H NMR Identification of Trimeric Heterometallic (Iron(III), Gallium(III), Manganese(III)) 2-Hydroxy-5,10,15,20-tetraphenylporphyrins and X-ray Crystal Structure of the Iron(III) 2-Hydroxy-5,10,15,20-tetra-p-tolylporphyrin Trimer(1).

Oligomerization of a mixture of monomeric iron(III) 2-hydroxy-5,10,15,20-tetraphenylporphyrin, (2-OH-TPP)Fe(III)Cl, manganese(III) 2-hydroxy-5,10,15,20-tetraphenylporphyrin, (2-OH-TPP)Mn(III)Cl, and gallium(III) 2-hydroxy-5,10,15,20-tetraphenylporphyrin, (2-OH-TPP)Ga(III)Cl, complexes affords the series of heterometallic cyclic trimeric species of the general formula {[(2-O-TPP)Ga(III)](n)()[(2-O-TPP)Fe(III)](3)(-)(n)()}, {[(2-O-TPP)Ga(III)](n)()[(2-O-TPP)Mn(III)](3)(-)(n)()}, and {[(2-O-TPP)Fe(III)](n)()[(2-O-TPP)Mn(III)](3)(-)(n)()} (n = 0-3). The (1)H NMR spectroscopic and mass spectrometric investigations indicate that these compounds have a head-to-tail cyclic trimeric structure. In the (1)H NMR spectra the interactions between paramagnetic, weakly coupled centers are reflected by marked variations of chemical shifts and line widths of pyrrole resonances. The characteristic upfield positions of the 3-H pyrrole resonances are diagnostic for the trimeric motifs. The structure of the prototypical molecule, [(2-O-TTP)Fe(III)](3), has been determined by X-ray crystallography. [(2-O-TTP)Fe(III)](3).3n-octane crystallizes in the monoclinic space groupP2(1)/n with a = 16.729(6) Å, b = 43.671(13) Å, c = 19.564(7) Å, beta = 105.83(3) degrees, and Z = 4 at 130 K. The refinement of 1612 parameters and 5072 reflections yields R(1)( )()= 0.089 and wR(2) = 0.1848. The trimeric iron(III) complex has a head-to-tail cyclic arrangement with the pyrrolic alkoxide groups forming bridges from one macrocycle to the metal in adjacent macrocycle. The three iron(III) porphyrin subunits are not equivalent but have typical geometry for high-spin five-coordinate iron(III) porphyrin complexes. The porphyrin skeleton of [(2-O-TTP)Fe(III)](3) is expected to be representative of the structures of the homometallic and heterometallic trimeric complexes of 2-hydroxytetraarylporphyrin with M(III) ions.

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Cs(8)Ga(11), a New Isolated Cluster in a Binary Gallium Compound. A Family of Valence Analogues A(8)Tr(11)X: A = Cs, Rb; Tr = Ga, In, Tl; X = Cl, Br, I.

Fusion of the elements, and alkali-metal halide when appropriate, in stoichiometric amounts in Ta containers followed by slow cooling results in high yields of the title compounds. X-ray structures refined for rhombohedral Cs(8)Ga(11) (R&thremacr;c, Z = 6, a = 9.9962(5) Å, c = 50.839(6) Å) and Cs(8)Ga(11)Cl (R&thremacr;&thremacr;c, Z = 6, a = 10.0111(7) Å, c = 50.504(6) Å) reveal isolated clusters of pentacapped, trigonal prismatic gallium anions, Ga(11)(7)(-), the former compound being isostructural with K(8)In(11) and A(8)Tl(11) (A = K, Rb, Cs). The clusters are arranged in pseudo-ccp layers separated by double layers of cesium atoms. The halide in Cs(8)Ga(11)Cl is bound in a preformed cavity within the cesium double layers where it is surrounded by eight cations. Of the nine examples reported for A(8)Tr(11)X, three chlorides occur in systems in which the binary A(8)Tr(11) do not form, Rb-Ga, Rb-In, and Cs-In. These halides are the first examples of Tr(11)(7)(-) compounds that are valence phases and do not contain an extra alkali-metal cation and electron. Magnetic susceptibility data indicate an apparently localized electron in paramagnetic Cs(8)Ga(11) and diamagnetism for Cs(8)Ga(11)Cl.

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Time-resolved electron spin resonance of gallium and germanium porphyrins in the excited triplet state.

Gallium and germanium porphyrin complexes in the lowest excited triplet (T1) state have been studied by time-resolved electron spin resonance (TRESR). It is found that for Ge(TPP)(OH)2 (TPP = dianion of tetraphenylporphyrin) intersystem crossing (ISC) from the lowest excited singlet (S1) state to the T1x and T1y sublevels is faster than that to the T1z sublevel (T1x, T1y, and T1z are sublevels of the T1 state), while the ISC of ZnTPP and Ga(TPP)(OH) is selective to the T1z sublevel. This is interpreted by a weak interaction between the dpi orbital of germanium and LUMO (eg) of the porphyrin ligand, resulting in small spin-orbit coupling (SOC). The interpretation is supported by molecular orbital calculations. The ISC of Ge(OEP)(OH)2 (OEP = dianion of octaethylporphyrin) and Ge(Pc)(OH)2 (Pc = dianion of tetra-tert-butylphthalocyanine) is found to be selective to the T1z sublevel in contrast to Ge(TPP)(OH)2. This dependence on the porphyrin ligand is reasonably explained by a difference between the 3(a(1u)eg) (the OEP and Pc complexes) and 3(a(2u)eg) (the TPP complex) configurations. This is the first observation of a difference in selective ISC between the 3(a(1u)eg) and 3(a(2u)eg) configurations. The TRESR spectrum of Ge(TPP)Br2 is different from those of Ge(TPP)Cl2 and Ge(TPP)(OH)2, and is interpreted by SOC between the T1 and T2 states. From ESR parameters the square of the coefficient of the eg orbital on bromine is evaluated as 0.018 in the T1 state.

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Novel gallium phosphate framework encapsulating trinuclear Mn3(H2O)6O8 cluster: hydrothermal synthesis and characterization of Mn3(H2O)6Ga4(PO4)6.

A new manganese gallium phosphate, Mn3(H2O)6Ga4(PO4)6, has been synthesized under hydrothermal conditions at 150 degrees C and characterized by single-crystal X-ray diffraction, thermogravimetric analysis, magnetic susceptibility, and electron paramagnetic resonance (EPR) spectroscopy. It crystallized in the monoclinic space group, P2(1)/n, with a = 8.9468(4) A, b = 10.148(5) A, c = 13.5540(7) A, beta = 108.249(1) degrees, and Z = 2. The compound is unusual in that it is not only the first nonoranically templated MnGaPO phase but also the first instance where edge-shared trinuclear manganese-oxygen clusters are encapsulated in a metal phosphate lattice. The trimer involves a central Mn(H2O)4O2 octahedron, which links to two Mn (H2O)2O4 octahedra at trans edges. The Mn3(H2O)6O8 clusters reside in tunnels built from GaO5 trigonal bipyramids and PO4 tetrahedra. Our magnetic study revealed that superexchange interactions occurred between the neighboring MnII centers. A good fit of the magnetic susceptibility data for the isolated trimers was obtained by using a derived expression based on Van Vleck's equation. Unlike all existing linear trinuclear MnII complexes, the chi MT product in the range 8-4 K remains at a constant value corresponding to one spin S = 5/2 per three MnII centers. The Curie behavior at such low temperatures has been confirmed by EPR data. According to the thermogravimetric analysis/differential thermal analysis (TGA/DTA) results, the title compound is thermally stable up to ca. 200 degrees C.

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Layered rare-earth gallium antimonides REGaSb(2) (RE = La--Nd, Sm).

The ternary rare-earth gallium antimonides, REGaSb(2) (RE = La--Nd, Sm), have been synthesized through reaction of the elements. The structures of SmGaSb(2) (orthorhombic, space group D(5)(2)-C222(1), Z = 4, a = 4.3087(5) A, b = 22.093(4) A, c = 4.3319(4) A) and NdGaSb(2) (tetragonal, space group D(19)(4h)-I4(1)/amd, Z = 8, a = 4.3486(3) A, c = 44.579(8) A) have been determined by single-crystal X-ray diffraction. The SmGaSb(2)-type structure is adopted for RE = La and Sm, whereas the NdGaSb(2)-type structure is adopted for RE = Ce--Nd. The layered SmGaSb(2) and NdGaSb(2) structures are stacking variants of each other. In both structures, two-dimensional layers of composition (2)(infinity)[GaSb] are separated from square nets of Sb atoms [Sb] by RE atoms. Alternatively, the structures may be considered as resulting from the insertion of zigzag Ga chains between (2)(infinity)[RE Sb(2)] slabs. In SmGaSb(2), all of the Ga chains are parallel and the (2)(infinity)[SmSb(2)] layers are stacked in a ZrSi(2)-type arrangement. In NdGaSb(2), the Ga chains alternate in direction, resulting in a doubling of the long axis relative to SmGaSb(2), and the (2)(infinity)[NdSb(2)] layers are stacked in a Zr(3)Al(4)Si(5)-type arrangement. Extended Hückel band structure calculations are used to explain the bonding in the [GaSb(2)](3-) substructure.

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Formation and characterization of the gallium and indium subhydride molecules Ga2H2 and In2H2: a matrix isolation study.

Ga2 reacts spontaneously with H2 in solid Ar matrixes at 12 K to form the cyclic molecule Ga(mu-H)2Ga. In2 does not react with H2 under similar conditions, but irradiation at wavelengths near 365 nm induces the formation of the corresponding indium hydride, In(mu-H)2In. The molecules have been identified and characterized by the IR spectra displayed by matrixes containing the metal and H2, D2, HD, or H2 + D2; they each have planar, dihydrido-bridged structures with D2h symmetry, as endorsed by comparison of the measured spectra (i) with the properties forecast by quantum chemical calculations and (ii) with the spectra of known gallium and indium hydrides. Both are photolabile under visible light (lambda > 450 nm): green light (lambda = ca. 546 nm) causes Ga(mu-H)2Ga to isomerize to a mixture of HGaGaH and H2GaGa, whereas broad-band visible irradiation (lambda > 450 nm) of In(mu-H)2In gives rise to the isomer HInInH, together with InH. The isomerization can be reversed by UV photolysis (lambda = ca. 365 nm) of HGaGaH, H2GaGa, and HInInH or by near-IR photolysis (lambda > 700 nm) of HGaGaH and H2GaGa.

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1,4-dioxobenzene compounds of gallium: reversible binding of pyridines to [[((t)Bu)(2)Ga](2)(mu-OC(6)H(4)O)](n) in the solid state.

The gallium aryloxide polymer, [[((t)Bu)(2)Ga](2)(mu-OC(6)H(4)O)](n)(1) is synthesized by the addition of Ga((t)()Bu)(3) with hydroquinone in a noncoordinating solvent, and reacts with pyridines to yield the yellow compound [((t)()Bu)(2)Ga(L)](2)(mu-OC(6)H(4)O) [L = py (2), 4-Mepy (3), and 3,5-Me(2)py (4)] via cleavage of the Ga(2)O(2) dimeric core. The analogous formation of Ga((t)()Bu)(2)(OPh)(py) (5) occurs by dissolution of [((t)Bu)(2)Ga(mu-OPh)](2) in pyridine. In solution, 2-4 undergo dissociation of one of the pyridine ligands to yield [((t)()Bu)(2)Ga(L)(mu-OC(6)H(4)O)Ga((t)Bu)(2)](2), for which the DeltaH and DeltaS have been determined. Thermolysis of compounds 2-4 in the solid-state results in the loss of the Lewis base and the formation of 1. The reaction of 1 or [((t)Bu)(2)Ga(mu-OPh)](2) with the vapor of the appropriate ligand results in the solid state formation of 2-4 or 5, respectively. The deltaH and deltaS for both ligand dissociation and association for the solid-vapor reactions have been determined. The interconversion of 1 into 2-4, as well as [((t)Bu)(2)Ga(mu-OPh)](2) into 5, and their reverse reactions, have been followed by (13)C CPMAS NMR spectroscopy, TG/DTA, SEM, EDX, and powder XRD. Insight into this solid-state polycondensation polymerization reaction may be gained from the single-crystal X-ray crystallographic packing diagrams of 2-5. The crystal packing for compounds 2, 3, and 5 involve a head-to-head arrangement that is maintained through repeated ligand dissociation and association cycles. In contrast, when compound 4 is crystallized from solution a head-to-tail packing arrangement is formed, but during reintroduction of 3,5-Me(2)py in the solid state-vapor reaction of compound 1, a head-to-head polymorph is postulated to account for the alteration in the deltaH of subsequent ligand dissociation reactions. Thus, the deltaH for the condensation polymerization reaction is dependent on the crystal packing; however, the subsequent reversibility of the reaction is dependent on the polymorph.

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