Synthesis and structural analysis of the copper(II) complexes of N2-(2-pyridylmethyl)-2-pyridinecarboxamide.

Previous investigations of the potential of metal-organic compounds as inhibitors of human immunodeficiency virus type I protease (HIV-1 PR) showed that the copper(II) complex diaqua [bis(2-pyridylcarbonyl)amido] copper(II) nitrate dihydrate and the complex bis[N2-(2,3,6-trimethoxybenzyl)-4-2-pyridinecarboxamide] copper(II) behaved as inhibitors of HIV-1 PR. In a search for similar readily accessible ligands, we synthesised and studied the structural properties of N2-(2-pyridylmethyl)-2-pyridinecarboxamide (L) copper(II) complexes. Three different crystal structures were obtained. Two were found to contain ligand L simultaneously in a tridentate and bidentate conformation [Cu(L(tri)L(bi))]. The other contained two symmetry-related ligands, coordinated through the pyridine nitrogen and the amide oxygen atoms [Cu(L(bi))(2)]. A search of the Cambridge Structural Database indicated that L(tri) resulting from nitrogen bound amide hydrogen metal substitution is favoured over chelation through the amide oxygen atom. In our case, we calculated that the conformation of L(tri) is 11 kcal/mol more favourable than that of L(bi). ESI-MS experiments showed that the Cu(L(bi))(2) structure could not be observed in solution, while Cu(L(tri)L(bi))-related complexes were indeed present. The lack of protease inhibition of the pyridine carboxamide copper(II) complexes was explained by the fact that the Cu(L(bi)L(tri)) complex could not fit into the HIV-1 active site.

Structural and photomagnetic studies of two compounds in the system Cu(2+)/Mo(CN8)(4-): from trinuclear molecule to infinite network.

The syntheses and structural and physical characterization of the compounds [Cu(bipy)(2)](2)[Mo(CN)(8)].5H(2)O. CH(3)OH (1) with bipy = 2,2'-bipyridine and M(II)(2)[Mo(IV)(CN)(8)].xH(2)O (2 with M = Cu, x = 7.5; 3 with M = Mn, x = 9.5) are presented. 1 crystallizes in the triclinic space group P1; (a = 11.3006(4) A, b = 12.0886(5) A, c = 22.9589(9) A, alpha = 81.799(2) degrees, beta = 79.787(2) degrees, gamma = 62.873(2) degrees, Z = 2). The structure of 1 consists of neutral trinuclear molecules in which a central [Mo(CN8)](4-) anion is linked to two [Cu(bipy)2](2+) cations through two cyanide bridges. 2 crystallizes poorly, and hence, structural information has been obtained from the wide-angle X-ray scattering (WAXS) technique, by comparison with 3 and Fe(II)(2)(H(2)O)(4)[Mo(IV)(CN)(8)].4H(2)O whose X-ray structure has been previously solved. 2, 3, and Fe(II)(2)(H(2)O)(4)[Mo(IV)(CN)(8)].4H(2)O form extended networks with all the cyano groups acting as bridges. The magnetic properties have shown that 1 and 2 behave as paramagnets. Under irradiation with light, they exhibit important modifications of their magnetic properties, with the appearance at low temperature of magnetic interactions. For 1 the modifications are irreversible, whereas they are reversible for 2 after cycling in temperature. These photomagnetic effects are thought to be caused by the conversion of Mo(IV) (diamagnetic) to Mo(V)(paramagnetic) through a photooxidation mechanism for 1 and a photoinduced electron transfer in 2. These results have been correlated with the structural features.

Chemistry and physics of supramolecular magnetic materials.

The building of multidimensional magnetic materials obtained with the molecular precursor [Cu(opba)](2-) is described. The reaction with other paramagnetic species (3d or 4f metal ions, organic radicals) yielded one-dimensional, two-dimensional, and interlocked networks. The magnetic properties of these systems are reviewed using polarized neutron diffraction and magnetic measurements. It is shown that the spin density maps give a precise description of the ground state of such molecular magnetic species. Moreover, different long-range magnetic orderings (antiferro-, ferri-, and ferromagnetic) have been obtained.

Photomagnetic properties in a series of spin crossover compounds

The spin crossover (SC) compounds [Fe(PM-AzA)2(NCX)2] and [Fe(PM-FIA)2(NCX)2] (with PM-AzA = N-2'-pyridylmethylene-4-(phe-nylazo)aniline, PM-FIA = N-2'-pyridylmethylene-4-(2-amino)fluorene, and X = S, Se) have been prepared. The SC regimes have been deduced from variable-temperature magnetic susceptibility data. The enthalpy and entropy changes associated with the SC have been evaluated from DSC measurements. A cooperativity factor, C, has been defined, and its values for the different compounds have been deduced from the spin crossover curves. At 10 K, the light-induced excited spin state trapping (LIESST) effect has been observed within the cavity of the SQUID magnetometer. The critical temperatures Tc(LIESST) have been determined for [Fe(PM-AzA)2(NCS)2] and [Fe(PM-F1A)2(NCX)2], and the role of cooperativity has been analyzed. A linear correlation has been found between the Tc(LIESST) and C values. The kinetics of HS-->LS relaxation have been investigated; a thermally activated mechanism at elevated temperatures and a nearly temperature independent relaxation behavior at low temperatures have been found. Finally, the magnetic behavior recorded under light irradiation in the warming and cooling modes has revealed the occurrence of the light-induced thermal hysteresis (LITH) effect.

Single-crystal polarized optical absorption spectroscopy of the one-dimensional ferrimagnet MnIICuII(pba)(H2O)3.2H2O (pba = 1,3-propylenebis(oxamato)).

Powder and single-crystal optical absorption of the ferrimagnet MnIICuII(pba)(H2O)(3).2H2O (denoted MnCu) and the Mn-doped compound Mn0.1Mg0.9Cu(pba)(H2O)(3).2H2O (denoted Mn0.1Mg0.9Cu) with pba standing for 1,3-propylenebis(oxamato) was investigated in the 10-300 K range. The crystal structure of MnCu was previously reported, and consists of bimetallic chains with octahedral MnII and square pyramidal CuII ions linked by oxamato bridges, MnCu and Mn0.1Mg0.9Cu being isostructural. The spectra of both MnCu and Mn0.1Mg0.9Cu show an important dichroism along the chain direction, due to the strong polarization of the CuII band at around 16,000 cm-1 in this direction. They exhibit narrow and intense spin-forbidden MnII transitions in the 24,000-25,000 cm-1 range, which are activated by an exchange mechanism. The polarization and thermal dependence of the 6A1g-->4A1g, 4Eg(G) MnII transitions were recorded. The polarization along the chain axis was interpreted in the framework of the pair mechanism first introduced by Tanabe and co-workers. A theoretical expression for the thermal dependence of the intensity was derived by considering the CuII spin as a quantum spin and the MnII spin as a classical spin, and compared with the experimental data. The interaction parameter between the local ground states has been found to be J = -25 cm-1 using the spin Hamiltonian H = -J sigma i(SMn,iSCu,i + SMn,i+1SCu,i). The spectra of Mn0.1Mg0.9Cu showed cold and hot bands, whose energy difference is directly related to J and the interaction parameter J* between the CuII ion in its ground state and the MnII ion in its spin-flip excited state. J* has been estimated to be +40 cm-1. These results have been compared to those obtained with other MnIICuII compounds. The complementarity between optical and magnetic properties has been discussed.

Ferromagnetism in an extended three-dimensional, diamond-like copper(II) network: a new copper(II)/1-hydroxybenzotriazolato complex exhibiting soft-magnet properties and two transitions at 6.4 and 4.4 K.

The use of the substituted benzotriazole ligand btaOH (1-hydroxybenzotriazole) in copper(II) chemistry has yielded a structurally and magnetically very interesting complex. The [Cu2(O2CMe)4(H2O)2]/btaOH.H2O/aqueous NH3 (1:4:4, 1:3:3, 1:2:2) reaction system in MeOH gives dark brown-green [Cu(btaO)2(MeOH)]n (4) in approximately 80% yield. 4 crystallizes in the tetragonal space group P4(3)2(1)2 with (at 25 degrees C) a = 9.915(1) A, b = 9.915(1) A, c = 14.715(2) A, and Z = 4. The structure consists of a 3D, diamond-like copper(II) lattice. The CuII atom has a square pyramidal geometry with four btaO- ligands at the basal plane. The btaO- ion functions as a bidentate bridging ligand, with N(3) and the deprotonated oxygen being the ligating atoms. Dc and ac magnetic susceptibility measurements, together with low-field (10 G) and high-field (up to 5000 G) magnetization data, are consistent with ferromagnetic interactions on the scale of the crystal lattice with two critical temperatures: 6.4 and 4.4 K. The former critical temperature could correspond to a transition from a paramagnetic to a ferromagnetic state; the latter one, to a transition from a ferromagnetically ordered state to its 3D ordering. The magnetic data, along with the field dependence of the magnetization and the EPR data, are also in line with a soft magnet. Moreover, the EPR studies performed on 4 reveal unique features reported for the first time in the field of molecular magnetism.

Synthesis, crystal structure, EXAFS, and magnetic properties of catena [mu-tris(1,2-bis(tetrazol-1-yl)propane-N1,N1')iron(II)] bis(perchlorate). First crystal structure of an iron(II) spin-crossover chain compound.

[Fe(btzp)3](ClO4)2 (btzp = 1,2-bis(tetrazol-1-yl)propane) represents the first structurally characterized Fe(II) linear chain compound exhibiting thermal spin crossover. It shows a very gradual spin transition (T1/2 = 130 K) which has been followed by magnetic susceptibility measurements and 57Fe Mössbauer spectroscopy. The structure has been solved at 200 and 100 K by single-crystal X-ray analysis. It crystallizes in the trigonal space group P3c1 with Z = 2 Fe(II) units at both temperatures. The molecular structure consists of chains running along the c axis in which the Fe(II) ions are linked by three N4,N4' coordinating bis(tetrazole) ligands. The main difference between the two forms appears to be in the Fe-N bond lengths, which are 2.164(4) A at 200 K and 2.038(4) A at 100 K. The Fe-Fe separations are 7.422(1) A at 200 K and 7.273(1) A at 100 K. The EXAFS results are consistent with the crystal structure. In both spin states, the FeN6 octahedron is almost regular within the EXAFS resolution. The Fe-N distance is found as 2.16(2) A at 300 K and 2.00(2) A at 40 K. The absence of the "7 A peak" in the EXAFS spectra of [Fe(btzp)3](ClO4)2, in contrast with what has been observed for the [Fe(4-R-1,2,4-triazole)3]-(anion)2 chain compounds, confirms that this peak can be used as the signature of a metal alignment only when it involves a strongly enhanced multiple scattering M-M-M path, with M-M spacing less than 4 A. Irradiation with green light at 5 K has led to the population of the metastable high-spin state for the iron(II) ion. The nature of the spin-crossover behavior has been discussed on the basis of the structural features.

A Mixed-Valence and Mixed-Spin Molecular Magnetic Material:

Long-range ferromagnetic ordering at 3 K is observed for the title compound, which may be considered as a fully localized mixed-valence species (Mo(3+) and Mo(4+)) as well as a mixed-spin species (low-spin and high-spin Mn(2+) ions). Its two-dimensional structure consists of heart-shaped 48-membered rings, and each ring contains 16 metal centers (see picture).

Celiac sprue, idiopathic thrombocytopenic purpura, and hepatic granulomatous disease. An autoimmune linkage?

We report the case of a patient with celiac sprue in whom idiopathic thrombocytopenic purpura and associated hepatic granulomatous disease developed. We suggest that the three processes are linked through autoimmune mechanisms.

Complications of colonoscopy and flexible sigmoidoscopy.

Complications can occur during both diagnostic and therapeutic endoscopy. Most statistics concerning complications are based on reports generated when colonoscopy was in its infancy. This article examines the diagnosis and treatment of complications that arise during the course of both colonoscopy and polypectomy. Surgery may not be required in all cases. The criteria for operative or nonoperative treatment are presented.

A molecular-based magnet with a fully interlocked three-dimensional structure.

A compound has been synthesized with the formula (rad)(2)Mn(2)[Cu(opba)](3)(DMSO)(2).2H(2)O, where rad(+) is 2-(4-N-methylpyridinium)-4,4,5,5-tetramethylimidazoline-1-oxyl-3-oxide, opba is orthophenylenebis(oxamato), and DMSO is dimethyl sulfoxide. It consists of two nearly perpendicular graphite-like networks with edge-sharing Mn(II)(6)Cu(II)(6) hexagons. The two networks are fully interlocked with the same topological relationship as that between adjacent rings of a necklace. The compound has three kinds of spin carriers: Mn(II) and Cu(II) ions, antiferromagnetically coupled through oxamato bridges, and rad(+) radical cations, bridging the Cu(II) ions through the nitronyl nitroxide groups and forming Cu-rad chains. The temperature dependence of the magnetization reveals that below 22.5 K, the compound behaves as a magnet.

Emission tomography in embolic lung disease: angiographic correlations.

The data from 84 patients with suspected embolic lung disease who underwent radionuclide section scanning of the chest is reported. All underwent additional conventional planar imaging; specific angiographic evidence of embolic disease was available in 12 cases. A good correlation between the section scans and angiography was obtained. Greater sensitivity in lesion detection was obtained by multiplane section imaging, which should reduce the number of diagnostic uncertainties in embolic lung disease.