Tromboflebite plantar: achados em ressonância magnética

OBJETIVO: Demonstrar os achados em ressonância magnética (RM) da tromboflebite plantar. MÉTODOS: Revisão retrospectiva de 20 pacientes com dor na região plantar nos quais os achados de ressonância magnética indicaram tromboflebite plantar. RESULTADOS: Foram avaliados 14 homens e seis mulheres, com idade média de 46,7 anos. Oito desses pacientes também foram submetidos à ultrassonografia com doppler, que confirmaram a tromboflebite. As imagens de ressonância magnética foram avaliadas em consenso por dois radiologistas com experiência em radiologia do sistema musculoesquelético (mais de 10 anos cada um), demonstrando edema perivascular em todos os 20 pacientes (100%) e edema muscular em 19 dos 20 pacientes (95%). Todos os 20 pacientes apresentavam intensidade de sinal intermediária intraluminal em T2 (100%) e ectasia venosa estava presente em 17 dos 20 casos (85%). Veias colaterais foram visualizadas em um dos 20 pacientes (5%). Todos os 14 casos (100%), nos quais o contraste intravenoso foi administrado, apresentavam realce dos tecidos perivenulares e defeito de enchimento intraluminal. Ectasia venosa, perda da compressibilidade e ausência de fluxo na ultrassonografia com doppler também foram observados em todos os oito casos examinados pelo método. CONCLUSÕES: A RM é um método sensível na avaliação de tromboflebite plantar em pacientes com dor plantar.

Monitoramento por imagem de ressonância magnética do crescimento tumoral no modelo C6 de glioblastoma com perspectivas de avaliação da terapia de magnetohipertemia

Objetivo: Estabelecer um padrão de crescimento tumoral (volume) em ratos Wistar submetidos ao modelo C6 de glioblastoma multiforme por meio de imagens de ressonância magnética para posterior verificação de redução de volume tumoral com a terapia de magnetohipertermia. Métodos: Para o modelo C6, utilizamos ratos Wistar, machos, jovens, pesando entre 250 e 300 g. Após anestesiados (cetamina 55 mg/kg e xilazina 11 mg/kg) foram injetadas estereotaxicamente células tumorigênicas linhagem C6 suspensas em meio de cultura (105 células em 10 µL) no córtex frontal direito (coordenadas a partir do bregma: anteroposterior = 2,0 mm; látero-lateral = 3,0 mm; profundidade = 2,5 mm) com uma seringa Hamilton. No Grupo Controle, houve a injeção do meio de cultura sem as células. Posteriormente, foram feitas imagens mediante a técnica de imagem por ressonância magnética em 14, 21 e 28 dias após a injeção em um escâner de imagem por ressonância magnética 2.0 T (Bruker BioSpec, Germany). Para o exame, os animais foram anestesiados com cetamina 55 mg/kg e xilazina 11 mg/kg. Multifatias coronais foram adquiridas utilizando uma sequência spin-echo padrão com os seguintes parâmetros: TR/TE = 4,000 ms/67,1 ms, FOV = 3,50, Matrix 192, slice thickness = 0,4 mm e slice separation = 0 mm. Resultados: A análise das imagens de ressonância magnética do tumor possibilitou a clara visualização da massa tumoral, sendo possível ainda estabelecer parâmetros de volume tumoral nos diferentes dias analisados. O volume de 14 dias após a indução do foi de 13,7 ± 2,5 mm3 . Aos 21 dias, o volume alcançado foi de 31,7 ± 6,5 mm3 e, aos 28 dias, a massa tumoral atingiu 122,1 ± 11,8 mm3 . Conclusão: Estes resultados mostraram a possiblidade de avaliação do volume tumoral no modelo C6 em ratos, o que possibilitará, no futuro, a aplicação da terapia de magnetohipertermia bem como verificação de seus resultados.

Monitoramento in vivo por imagem por ressonância magnética de células C6 de glioma marcadas com nanopartículas superparamagnéticas de óxido de ferro

OBJECTIVE: The aim of the current study was to monitor the migration of superparamagnetic iron oxide nanoparticle (SPION)-labeled C6 cells, which were used to induce glioblastoma tumor growth in an animal model, over time using magnetic resonance imaging (MRI), with the goal of aiding in tumor prognosis and therapy. METHODS: Two groups of male Wistar rats were used for the tumor induction model. In the first group (n=3), the tumors were induced via the injection of SPION-labeled C6 cells. In the second group (n=3), the tumors were induced via the injection of unlabeled C6 cells. Prussian Blue staining was performed to analyze the SPION distribution within the C6 cells in vitro. Tumor-inducing C6 cells were injected into the right frontal cortex, and subsequent tumor monitoring and SPION detection were performed using T2- and T2*-weighted MRI at a 2T field strength. In addition, cancerous tissue was histologically analyzed after performing the MRI studies. RESULTS: The in vitro qualitative evaluation demonstrated adequate distribution and satisfactory cell labeling of the SPIONs. At 14 or 21 days after C6 injection, a SPION-induced T2- and T2*-weighted MRI signal reduction was observed within the lesion located in the left frontal lobe on parasagittal topography. Moreover, histological staining of the tumor tissue with Prussian Blue revealed a broad distribution of SPIONs within the C6 cells. CONCLUSION: MRI analyses exhibit potential for monitoring the tumor growth of C6 cells efficiently labeled with SPIONs.

Correlação das imagens da ressonância magnética e observação intra operatória nas lesões traumáticas da coluna vertebral

OBJETIVO: Avaliar a acurácia e a reprodutibilidade das imagens da ressonância magnética (RM) nas lesões ligamentares traumáticas da coluna vertebral. MÉTODOS: Estudo retrospectivo para avaliação das imagens da RM de 32 pacientes com lesões traumáticas da coluna vertebral submetidos a tratamento cirúrgico. A avaliação das lesões do complexo ligamentar posterior (CLP) por imagens da RM foi realizada independentemente por dois radiologistas. Um grupo de pacientes tinha exames com inclusão de sequência com supressão de gordura sensível ao líquido (STIR ou SPAIR T2), além das imagens de rotina e no outro grupo os exames de RM não incluíam imagens com a supressão da gordura. As avaliações dos exames de imagem foram comparadas com as observações obtidas durante o ato cirúrgico. Foi realizada a analise de reprodutibilidade intra e interobservador entre os dois radiologistas pelo cálculo do coeficiente Kappa. RESULTADOS: Foi observada lesão do CLP em 21/32 pacientes. De forma geral a sensibilidade da RM para lesões do CLP variou entre 88,9% a 100% e a especificidade entre 0 e 50%. A concordância entre a avaliação dos radiologistas foi maior nos exames de ressonância magnética sem a supressão da gordura (Κ=0,6) do que nos exames que incluíram sequências com supressão (Κ=0,34). CONCLUSÃO: A avaliação de lesões dos ligamentos posteriores por meio da RM pelos radiologistas resultou em boa sensibilidade em relação aos achados cirúrgicos, porém com baixa especificidade, reproduzindo resultados da literatura. Na casuística atual a utilização do sinal de edema presente nas sequências com supressão de gordura diminuiu a concordância interobservador.

Pressure Dependence of N-15 Chemical Shifts in Model Peptides Ac-Gly-Gly-X-Ala-NH2

High pressure NMR spectroscopy has developed into an important tool for studying conformational equilibria of proteins in solution. We have studied the amide proton and nitrogen chemical shifts of the 20 canonical amino acids X in the random-coil model peptide Ac-Gly-Gly-X-Ala-NH2, in a pressure range from 0.1 to 200 MPa, at a proton resonance frequency of 800 MHz. The obtained data allowed the determination of first and second order pressure coefficients with high accuracy at 283 K and pH 6.7. The mean first and second order pressure coefficients <B-1(15N)> and <B-2(15N)> for nitrogen are 2.91 ppm/GPa and -2.32 ppm/GPa(2), respectively. The corresponding values <B-1(1H)> and <B-2(1H)> for the amide protons are 0.52 ppm/GPa and -0.41 ppm/GPa(2). Residual dependent (1)J(1H15N)-coupling constants are shown.

(18O,16O) Two-neutron transfer reactions for spectroscopic studies.

A systematic study of the response of different nuclei to the (18O, 16O) two-neutron transfer reaction at 84 MeV incident energy was pursued at the INFN-LNS in Catania (Italy). The experiments were performed using several solid targets from light (9Bc, 11 B, 12,13C, 16O, 28Si) to heavier ones (58,64Ni, 120Sn, 208Pb). The 16O ejectiles were detected at forward angles by the MAGNEX magnetic spectrometer and identified without the need of time of flight measurements. Exploiting the large momentum (≈ 25%) and angular (50 msr) acceptance of the spectrometer, energy spectra were obtained with a relevant yield up to about 20 MeV excitation energy. A common feature of the light nuclei spectra is the strong population of states with well known configuration of two-particle over a core and the appearance of unknown resonant structures in the continuum. These latter can reveal the excitation of a collective mode connected with the transfer of a pair. For the heavier nuclei as 66Ni a completely different behaviour is observed indicating the presence of more dissipative processes in the reaction mechanisms that hide the spectroscopic information.

Quasi-bound alpha resonant states populated by the 12C(6Li,d) reaction.

Several narrow alpha resonant 16O states were detected through the 12C(6Li,d) reaction, in the range of 12 to 17 MeV of excitation energy. The reaction was measured at a bombarding energy of 25.5 MeV employing the São Paulo Pelletron-Enge-Spectrograph facility and the nuclear emulsion technique. Experimental angular distributions associated with four natural parity quasi-bound states ncar the 4α threshold are presented and compared to DWBA predictions.

Spin coherent states in NMR quadrupolar system: experimental and theoretical applications

Working with nuclear magnetic resonance (NMR) in quadrupolar spin systems, in this paper we transfer the concept of atomic coherent state to the nuclear spin context, where it is referred to as pseudonuclear spin coherent state (pseudo-NSCS). Experimentally, we discuss the initialization of the pseudo- NSCSs and also their quantum control, implemented by polar and azimuthal rotations. Theoretically, we compute the geometric phases acquired by an initial pseudo-NSCS on undergoing three distinct cyclic evolutions: (i) the free evolution of the NMR quadrupolar system and, by analogy with the evolution of the NMR quadrupolar system, that of (ii) single-mode and (iii) two-mode Bose-Einstein Condensate like system. By means of these analogies, we derive, through spin angular momentum operators, results equivalent to those presented in the literature for orbital angular momentum operators. The pseudo-NSCS description is a starting point to introduce the spin squeezed state and quantum metrology into nuclear spin systems of liquid crystal or solid matter.

Classical bifurcation in a quadrupolar NMR system

The Josephson junction model is applied to the experimental implementation of classical bifurcation in a quadrupolar nuclear magnetic resonance system. There are two regimes, one linear and one nonlinear, which are implemented by the radio-frequency and the quadrupolar terms of the Hamiltonian of a spin system, respectively. These terms provide an explanation of the symmetry breaking due to bifurcation. Bifurcation depends on the coexistence of both regimes at the same time in different proportions. The experiment is performed on a lyotropic liquid crystal sample of an ordered ensemble of 133Cs nuclei with spin I = 7/2 at room temperature. Our experimental results confirm that bifurcation happens independently of the spin value and of the physical system. With this experimental spin scenario, we confirm that a quadrupolar nuclei system could be described analogously to a symmetric two-mode Bose-Einstein condensate.

Molecular dynamics of poly(Ethylene Glycol) intercalated in clay, studied using 13C solid-state NMR

In this study, Cross-Polarization Magic-angle Spinning CP/MAS, 2D Exchange, Centerband-Only Detection of Exchange (CODEX), and Separated-Local-Field (SLF) NMR experiments were used to study the molecular dynamics of poly(ethylene glycol) (PEG) inside Hectorite/PEG intercalation compounds in both single- and double-layer configurations. The results revealed that the overall amplitude of the motions of the PEG chain in the single-layer configuration is considerably smaller than that observed for the double-layer intercalation compound. This result indicates that the effect of having the polymer chain interacting with both clay platelets is to produce a substantial decrease in the motional amplitudes of those chains. The presence of these dynamically restricted segments might be explained by the presence of anchoring points between the clay platelets and the PEG oxygen atoms, which was induced by the Na+ cations. By comparing the PEG motional amplitudes of the double-layered nanocomposites composed of polymers with different molecular weights, a decrease in the motional amplitude for the smaller PEG chain was observed, which might also be understood using the presence of anchoring points.

ScPdZn and ScPtZn with YAlGe type structure: group-subgroup relation and 45Sc solid state NMR spectroscopy

The intermetallic compounds ScPdZn and ScPtZn were prepared from the elements by high-frequency melting in sealed tantalum ampoules. Both structures were refined from single crystal X-ray diffractometer data: YAlGe type, Cmcm, a = 429.53(8), b = 907.7(1), c = 527.86(1) pm, wR2 = 0.0375, 231 F2 values, for ScPdZn and a = 425.3(1), b = 918.4(2), c = 523.3(1) pm, wR2 = 0.0399, 213 F2 values for ScPtZn with 14 variables per refinement. The structures are orthorhombically distorted variants of the AlB2 type. The scandium and palladium (platinum atoms) build up ordered networks Sc3Pd3 and Sc3Pt3 (boron networks) which are slightly shifted with respect to each other. These networks are penetrated by chains of zinc atoms (262 pm in ScPtZn) which correspond to the aluminum positions, i.e. Zn(ScPd) and Zn(ScPt). The corresponding group-subgroup scheme and the differences in chemical bonding with respect to other AlB2-derived REPdZn and REPtZn compounds are discussed. 45Sc solid state NMR spectra confirm the single crystallographic scandium sites. From electronic band structure calculations the two compounds are found metallic with free electron like behavior at the Fermi level. A larger cohesive energy for ScPtZn suggests a more strongly bonded intermetallic than ScPdZn. Electron localization and overlap population analyses identify the largest bonding for scandium with the transition metal (Pd, Pt).

Parafusos pediculares: estruturas anatômicas em risco no tratamento da escoliose idiopática

OBJETIVO: Avaliar a posição das estruturas anatômicas em risco durante a inserção de parafusos pediculares na coluna torácica e sua relação com a variação do ângulo de Cobb. MÉTODOS: Os parâmetros estudados foram: a medida do ângulo de Cobb nas radiografias e a posição da medula espinhal, da cavidade pleural e aorta na ressonância nuclear magnética em relação a uma linha de 40mm criada para simular o parafuso pedicular nas cinco vértebras apicais. RESULTADOS: A distância da aorta ao corpo vertebral e o ângulo de segurança do lado convexo apresentaram diferença estatística quando relacionados com a variação do ângulo de Cobb medido. CONCLUSÃO: Os resultados apresentados sugerem maior risco de lesão da artéria aorta com o aumento do ângulo de Cobb e aumento do risco na inserção de parafusos pediculares no lado convexo da curvatura, quando se considera o ângulo de segurança.

Alpha cluster structure in 16O.

The alpha cluster phenomenon in the light nuclei structure has been the subject of a longtime investigation since the proposal of the Ikeda diagrams, however the mechanism of the cluster formation is still not completely understood. In fact, if the clusters have a fairly rigid crystal-like or a gas-like structure remains an open question. The interpretation of the Hoyle state as an α condensate brought a renewed interest to this subject, in particular to resonances analogous to the Hoyle state. In this context the study of the experimental evolution of the α-cluster phenomenon through (6Li,d) transfer reactions has been performed in São Paulo. Particularly important are the regions around the nα thresholds where the α-cluster structure states are predicted. The resonant states around the 4α threshold in the nucleus 16O are the focus of the present contribution. The 12C(6Li,d)16O reaction was measured at a bombarding energy of 25.5 MeV employing the São Paulo Pelletron-Enge-Spectrograph facility and the nuclear emulsion detection technique. Resonant states above the α threshold were measured and an energy resolution of 15-30 keV allows to define states previously unresolved. The angular distributions of the absolute cross sections were determined in a range of 4-40 degree in the center of mass system and up to 17 MeV excitation energy. The upper limit for the resonance widths in the crucial region of the 4α threshold was obtained. These values revealed to be at least a factor three smaller than the ones previously reported in the literature, indicating that the α cluster structure information on this region should be revised.

Remarkable coordination behavior of alkyl isocyanides toward unsaturated vicinal frustrated P/B Lewis pairs

The conjugated frustrated phosphane/borane Lewis pairs formed by 1,1-carboboration of a substituted diphenylphosphino acetylene, undergo a synergistic 1,1-addition reaction to n-butyl isocyanide with formation of new B-C and P-C bonds to the former isonitrile carbon atom. Using tert-butyl isocyanide dynamic behaviour between the isocyanide-[B] adduct and the 1,1-addition product formation was observed in solution. The different modes of isocyanide binding to the FLPs in the solid state were characterized using X-ray crystal structure analyses and comprehensive 11B and 31P solid-state magicangle- spinning (MAS-) NMR experiments. The free FLP, the Lewis adduct at the borane group, and the cyclic product resulting from isocyanide addition to both reaction centers, can be differentiated via 11B and 31P isotropic chemical shifts, 11B nuclear electric quadrupole coupling constants, isotropic indirect 11B-31P spin-spin coupling constants, and 11B...31P internuclear distances measured by rotational echo double resonance.

Molecular origin of charge traps in polyfluorene-based semiconductors

The comprehensive control of morphology and structure is of extreme importance in semiconducting polymers when used as active layers in optoelectronic devices. In the work reported here, a systematic investigation of the structural and dynamical properties of poly(9,9-di-n-octyl-fluorene-alt-benzothiadiazole), known as F8BT, and their correlation with electrical properties is presented when the material is used as an active layer in optoelectronic devices. By means of X-ray diffraction, one observes that in thick layer films (thickness of about 4 μm) grown by drop-cast deposition, a solvent induced crystalline phase exists which evolves to a stable phase as the temperature is raised. This was not observed in thin films (thickness of about 250 nm) prepared by spin-coating within the investigated temperature range. By modeling the current-voltages characteristics of both thick and thin film devices, important information on the influence of crystallization on the trapping states could be drawn. Furthermore, the temperature dependence of the charge carrier mobility was found to be closely related to that of the molecular relaxation processes. The understanding of the nature of such molecular relaxations, measured by solid-state nuclear magnetic resonance methods, allows one to understand the importance of molecular relaxations and microstructure changes on the trap states of the system.