Bobinas de radiofrequência em estudos mamários por ressonância magnética: modelos e qualidade de imagem

Em três equipamentos de Ressonância Magnética [1,5T] avaliaram-se e compararam-se 3 modelos de bobinas dedicadas para estudos mamários. A variável qualidade de imagem foi avaliada quantitativamente através dos indicadores: (i) relação entre o sinal e o ruído (SNR) e (ii) uniformidade do sinal (U). Na avaliação qualitativa consideram-se as variáveis: (iii) conforto proporcionado às voluntárias durante o exame, (iv) acessibilidade à mama para procedimentos de intervenção, (v) manipulação e posicionamento pelos Técnicos de Radiologia, (vi) possibilidade de selecção uni ou bilateral na aquisição da imagem e (vii) orientação da paciente dentro do magneto. Para a obtenção das imagens, 3 mulheres voluntárias, sem história conhecida de patologia mamária que representavam os padrões mamários 1, 2 e 3 da classificação BIRADS (35, 53 e 72 anos) foram submetidas a uma sequência RM utilizando-se a técnica de saturação espectral da gordura (SPIR), em ponderação T2. Procedeu-se a uma análise de variância factorial com cinco factores fixos sem réplicas e verificou-se que existiam diferenças significativas nas imagens relativamente aos valores médios da SNR e U nas três bobinas [SNR (valor-p=0, F=277,193) e U (valor-p=0, F=1487,95)]. A análise das comparações múltiplas de Tukey, permitiu verificar que existem diferenças significativas entre os valores médios da SNR e da U entre todas as combinações de pares de bobinas, sendo a bobina Z a que apresentou os valores médios da SNR e da U significativamente mais elevados [SNR (15,08u.a.) e U (0,58u.a.)] e, por isso, permitindo obter melhores imagens. Quanto à bobina X verificaram-se os valores de (SNR=4,77 e U=0,30u.a.) e para a bobina Y o SNR (2u.a.) e a U (0,06u.a). Verificou-se que a posição da ROI nos procedimentos de medida (correlação de Spearman) não influencia a qualidade da imagem (valor-p≥0 em todas as bobinas). A classificação mais elevada relativamente ao conforto foi atribuída à bobina X, seguindo-se a bobina Z. A escolha do modelo da bobina é importante para promover o aumento da qualidade das imagens, do conforto da paciente e manipulação nas manobras de posicionamento. Este estudo poderá contribuir como regulador dos aspectos financeiros e comerciais desenvolvidos entre marcas concorrentes no mercado.

Risk factors for metabolic bone disease in Crohn's disease patients

Background: The aim was to evaluate the presence of metabolic bone disease (MBD) in patients with Crohn’s disease (CD) and to identify potential etiologic factors. Methods: The case–control study included 99 patients with CD and 56 controls with a similar age and gender distribution. Both groups had dual-energy x-ray absorptionmetry and a nutritional evaluation. Single nucleotide polymorphisms at the IL1, TNF-a, LTa, and IL-6 genes were analyzed in patients only. Statistical analysis was performed using SPSS software. Results: The prevalence of MBD was significantly higher in patients (P ¼ 0.006). CD patients with osteoporosis were older (P < 0.005), small bowel involvement and surgical resections were more frequent (P < 0.005), they more often exhibited a penetrating or stricturing phenotype (P < 0.05), duration of disease over 15 years (P < 0.005), and body mass index (BMI) under 18.5 kg/m2 (P < 0.01) were more often found. No association was found with steroid use. Patients with a Z-score < 2.0 more frequently had chronic active disease (P < 0.05). With regard to diet, low vitamin K intake was more frequent (P ¼ 0.03) and intake of total, monounsaturated, and polyunsaturated fat was higher in patients with Z-score < 2.0 (P < 0.05). With respect to genetics, carriage of the polymorphic allele for LTa252 A/G was associated with a higher risk of osteoporosis (P ¼ 0.02). Regression analysis showed that age over 40 years, chronic active disease, and previous colonic resections were independently associated with the risk of developing MBD. Conclusions: The prevalence of MBD was significantly higher in CD patients. Besides the usual risk factors, we observed that factors related to chronic active and long-lasting disease increased the risk of MBD.

Cobalt complexes with pyrazole ligands as catalyst precursors for the peroxidative oxidation of cyclohexane: Z-ray absorption spectroscopy studies and biological applications

[CoCl(-Cl)(Hpz(Ph))(3)](2) (1) and [CoCl2(Hpz(Ph))(4)] (2) were obtained by reaction of CoCl2 with HC(pz(Ph))(3) and Hpz(Ph), respectively (Hpz(Ph)=3-phenylpyrazole). The compounds were isolated as air-stable solids and fully characterized by IR and far-IR spectroscopy, MS(ESI+/-), elemental analysis, cyclic voltammetry (CV), controlled potential electrolysis, and single-crystal X-ray diffraction. Electrochemical studies showed that 1 and 2 undergo single-electron irreversible (CoCoIII)-Co-II oxidations and (CoCoI)-Co-II reductions at potentials measured by CV, which also allowed, in the case of dinuclear complex 1, the detection of electronic communication between the Co centers through the chloride bridging ligands. The electrochemical behavior of models of 1 and 2 were also investigated by density functional theory (DFT) methods, which indicated that the vertical oxidation of 1 and 2 (that before structural relaxation) affects mostly the chloride and pyrazolyl ligands, whereas adiabatic oxidation (that after the geometry relaxation) and reduction are mostly metal centered. Compounds 1 and 2 and, for comparative purposes, other related scorpionate and pyrazole cobalt complexes, exhibit catalytic activity for the peroxidative oxidation of cyclohexane to cyclohexanol and cyclohexanone under mild conditions (room temperature, aqueous H2O2). Insitu X-ray absorption spectroscopy studies indicated that the species derived from complexes 1 and 2 during the oxidation of cyclohexane (i.e., Ox-1 and Ox-2, respectively) are analogous and contain a Co-III site. Complex 2 showed low invitro cytotoxicity toward the HCT116 colorectal carcinoma and MCF7 breast adenocarcinoma cell lines.

Reappraisal of the wrong-sign HBB¯ coupling and the study of h→Zγ

It has been pointed out recently that current experiments still allow for a two Higgs doublet model where the hbb¯ coupling (kDmb/v) is negative; a sign opposite to that of the Standard Model. Due to the importance of delayed decoupling in the hH+H− coupling, h→γγ improved measurements will have a strong impact on this issue. For the same reason, measurements or even bounds on h→Zγ are potentially interesting. In this article, we revisit this problem, highlighting the crucial importance of h→VV, which can be understood with simple arguments. We show that the impacts on kD<0 models of both h→bb¯ and h→τ+τ− are very sensitive to input values for the gluon fusion production mechanism; in contrast, h→γγ and h→Zγ are not. We also inquire if the search for h→Zγ and its interplay with h→γγ will impact the sign of the hbb¯ coupling. Finally, we study these issues in the context of the flipped two Higgs doublet model.

Determinação dos valores de referência da excursão sistólica do plano do anel tricúspide (TAPSE) em crianças saudáveis

Mestrado em Tecnologia de Diagnóstico e Intervenção Cardiovascular - Área de especialização: Ultrassonografia cardiovascular

Two-loop stability of a complex singlet extended Standard Model

Motivated by the dark matter and the baryon asymmetry problems, we analyze a complex singlet extension of the Standard Model with a Z(2) symmetry (which provides a dark matter candidate). After a detailed two-loop calculation of the renormalization group equations for the new scalar sector, we study the radiative stability of the model up to a high energy scale (with the constraint that the 126 GeV Higgs boson found at the LHC is in the spectrum) and find it requires the existence of a new scalar state mixing with the Higgs with a mass larger than 140 GeV. This bound is not very sensitive to the cutoff scale as long as the latter is larger than 10(10) GeV. We then include all experimental and observational constraints/measurements from collider data, from dark matter direct detection experiments, and from the Planck satellite and in addition force stability at least up to the grand unified theory scale, to find that the lower bound is raised to about 170 GeV, while the dark matter particle must be heavier than about 50 GeV.