The Anatomy of the Thoracic Spinal Canal Investigated with Magnetic Resonance Imaging

BACKGROUND: We investigated, with magnetic resonance imaging, the distance of the dura mater to the spinal cord in patients without spinal or medullar disease at the 2nd, 5th, and 10th thoracic segments.METHODS: Fifty patients in the supine position underwent magnetic resonance imaging. Medial sagittal slices of the 2nd, 5th, and 10th thoracic segments were measured for the relative distances using the 1.5-T superconducting system (Gyroscan Intera, Philips Medical Systems, Best, the Netherlands). In 10 patients, the angles relative to the tangent at the insertion point on the skin were measured.RESULTS: The posterior dural-spinal cord distance is significantly greater at the midthoracic region (5th thoracic = 5.8 +/- 0.8 mm) than at the upper (2nd thoracic = 3.9 +/- 0.8 mm) and lower thoracic levels (10th thoracic = 4.1 +/- 1.0 mm) (P < 0.015). There were no differences between interspaces T2 and 110. There was no correlation between age and the measured distance between the dura mater and the spinal cord. The entry angle of the needle at T2 was 9.0 degrees +/- 2.5 degrees; at T5, 45.0 degrees +/- 7.4 degrees; and at T10, 9.50 degrees +/- 4.2 degrees.CONCLUSIONS: This study demonstrated that there is greater depth of the posterior subarachnoid space at the T2, T5, and T10 levels. The greater distance was found at T5. (Anesth Analg 2010;110:1494-5)

Two phase transitions in (s+id)-wave Bardeen-Cooper-Schrieffer superconductivity

We establish universal behaviour in the temperature dependencies of some observables in (s + id)-wave BCS superconductivity in the presence of a weak a wave. We find also a second second-order phase transition. As temperature is lowered-past the usual critical temperature T-c, a less ordered superconducting phase is created in the d wave, which changes to a more ordered phase in a (s + id) wave at T-c1 (

Cutoff-independent regularization of four-fermion interactions for color superconductivity

We implement a cutoff-independent regularization of four-fermion interactions to calculate the color-superconducting gap parameter in quark matter. The traditional cutoff regularization has difficulties for chemical potentials mu of the order of the cutoff Lambda, predicting in particular a vanishing gap at mu similar to Lambda. The proposed cutoff-independent regularization predicts a finite gap at high densities and indicates a smooth matching with the weak coupling QCD prediction for the gap at asymptotically high densities.

Two phase transitions in (d(x2-y2)+is)-wave superconductors

We study numerically the temperature dependencies of specific heat, susceptibility, penetration depth, and thermal conductivity of a coupled (d(x2-y2) + is)-wave Bardeen-Cooper-Schrieffer (BCS) superconductor in the presence of a weak s-wave component (1) on square lattice and (2) on a lattice with orthorhombic distortion. As the temperature is lowered past the critical temperature T-c, a less ordered superconducting phase is created in d(x2-y2) wave, which changes to a more ordered phase in (d(x2-y2) + is) wave at T-c1. This manifests in two second-order phase transitions. The two phase transitions are identified by two jumps in specific heat at T-c and T-c1. The temperature dependencies of the superconducting observables exhibit a change from power-law to exponential behavior as temperature is lowered below T-c1 and confirm the new phase transition. (C) 1999 Elsevier B.V. B.V. All rights reserved.

Critical temperature for first-order phase transitions in confined systems

We consider the Euclidean D-dimensional -lambda vertical bar phi vertical bar(4)+eta vertical bar rho vertical bar(6) (lambda,eta > 0) model with d (d <= D) compactified dimensions. Introducing temperature by means of the Ginzburg-Landau prescription in the mass term of the Hamiltonian, this model can be interpreted as describing a first-order phase transition for a system in a region of the D-dimensional space, limited by d pairs of parallel planes, orthogonal to the coordinates axis x(1), x(2),..., x(d). The planes in each pair are separated by distances L-1, L-2, ... , L-d. We obtain an expression for the transition temperature as a function of the size of the system, T-c({L-i}), i = 1, 2, ..., d. For D = 3 we particularize this formula, taking L-1 = L-2 = ... = L-d = L for the physically interesting cases d = 1 (a film), d = 2 (an infinitely long wire having a square cross-section), and for d = 3 (a cube). For completeness, the corresponding formulas for second-order transitions are also presented. Comparison with experimental data for superconducting films and wires shows qualitative agreement with our theoretical expressions.

Commissioning and performance of the CMS silicon strip tracker with cosmic ray muons

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

The CMS experiment at the CERN LHC

The Compact Muon Solenoid (CMS) detector is described. The detector operates at the Large Hadron Collider (LHC) at CERN. It was conceived to study proton-proton (and lead-lead) collisions at a centre-of-mass energy of 14 TeV (5.5 TeV nucleon-nucleon) and at luminosities up to 10(34)cm(-2)s(-1) (10(27)cm(-2)s(-1)). At the core of the CMS detector sits a high-magnetic-field and large-bore superconducting solenoid surrounding an all-silicon pixel and strip tracker, a lead-tungstate scintillating-crystals electromagnetic calorimeter, and a brass-scintillator sampling hadron calorimeter. The iron yoke of the flux-return is instrumented with four stations of muon detectors covering most of the 4 pi solid angle. Forward sampling calorimeters extend the pseudo-rapidity coverage to high values (vertical bar eta vertical bar <= 5) assuring very good hermeticity. The overall dimensions of the CMS detector are a length of 21.6 m, a diameter of 14.6 m and a total weight of 12500 t.

Gravity, antigravity and gravitational shielding in (2+1) dimensions

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Planejamento e produção de um criostato de baixo custo para caracterização elétrica de materiais

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Avaliação da limpeza de CDtrodo construídos a partir de CD de ouro gravável/fita adesiva de galvanoplastia

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Correção e prevenção da deformidade em flexão da articulação antebraquiocárpica em cães, decorrente do alongamento do antebraço pelo método de Ilizarov

O objetivo do estudo foi comparar os resultados dos tratamentos cirúrgico e preventivo da deformidade em flexão da articulação antebraquiocárpica, decorrentes do alongamento simultâneo do rádio e ulna pelo método de Ilizarov. Foram utilizados 12 cães, sem raça definida, adultos, com peso entre 19 e 28kg, divididos em quatro grupos segundo os tratamentos: A - alongamento ósseo, B - alongamento ósseo e posterior alongamento tendíneo, C - alongamento ósseo e estabilização da articulação antebraquiocárpica, D - sem alongamento. O fixador básico empregado em todos os grupos foi composto por dois anéis e quatro hastes telescópicas, porém no grupo C foi incluído um semi-anel distal fixando a articulação antebraquiocárpica. Os animais dos grupos A, B e C foram submetidos a 28 dias de alongamento, 60 dias de fase neutra com fixador e 45 dias sem o fixador. Os cães do grupo D, considerados como controle, foram submetidos à fixação e osteotomia e não foram alongados. Mesmo com o emprego de exercícios passivos alternados com esparadrapo estendendo-se dos coxins à porção cranial do anel, os animais dos grupos A e B desenvolveram, durante o período de distração, gradual e progressiva contratura em flexão da articulação antebraquiocárpica, que persistiu mesmo após a remoção do fixador. Nos cães do grupo B, ao término do período sem fixador, efetuaram-se alongamento dos tendões flexores, secção dos tecidos periarticulares e capsulotomia. Eles foram observados por mais 45 dias. O tratamento cirúrgico, tecnicamente difícil de ser feito, permitiu a correção da contratura. No grupo C, o tratamento preventivo com o semi-anel distal evitou a contratura, mas durante a fase de alongamento houve tendência à flexão dos dígitos. Os cães do grupo D não desenvolveram contratura. Foi possível concluir que medidas preventivas, como o emprego do semi-anel nos metacarpianos, são importantes para evitar o desenvolvimento de contratura durante o alongamento do antebraço em cães.

Percepção de professores de educação infantil sobre a inclusão da criança com deficiência

A educação infantil é importante para o desenvolvimento da criança com necessidades especiais. Nesse processo educacional, o professor e sua percepção de educação inclusiva são fatores primordiais. Este trabalho objetivou analisar a percepção de professores de educação infantil, que quanto à prática educativa atual, diferem em relação à presença de alunos com deficiências em seus ambientes de trabalho, sobre a educação da criança com deficiência na faixa etária de 3 a 6 anos. Foram sujeitos da pesquisa 12 professores de educação infantil divididos eqüitativamente em três grupos: de escolas especiais; de escolas comuns que trabalham com crianças com deficiências inseridas em suas classes e de escolas comuns que não possuem em suas classes crianças com deficiências. A coleta de dados foi realizada através de entrevistas semi-estruturadas, gravadas em fita cassete. Foi realizada análise de conteúdo e os dados mostraram que os professores vêem como a principal contribuição do processo de inclusão a socialização da criança com deficiências, restringindo-o, porém, a crianças com possibilidades de independência. Quanto à aprendizagem, acreditam que a criança com deficiência mental é a que encontra maiores dificuldades, contrariamente à com deficiência física. Ressaltam problemas com o espaço físico, recursos materiais e humanos e relativos à formação do professor. Pôde se concluir que é preciso possibilitar aos professores uma formação que abranja conhecimentos sobre as diferentes deficiências e as necessidades educacionais relativas a estas, propiciar a adequação do espaço físico e dos recursos materiais, além de assistência técnica específica.

Addition of Ca-compounds nanoparticles in melt-textured Bi : 2212

Superconducting BSCCO samples made by melt-texturing process were prepared with the addition of calcium zirconate and calcium silicate nanoparticles. Bi:2212 melt-textured composites prepared with I wt.% of either addition showed different behavior for the critical current density as a function of the applied field, indicating that for each additional compound the improvement can be associated to different enhancement mechanisms, such as the creation of pinning centers and the increase on the connectivity of the grains. The estimated pinning forces indicated higher values for the calcium compound containing samples. (c) 2007 Elsevier B.V. All rights reserved.

Processing and properties of Ag/BSCCO PIT tapes containing different proportions of silver metal powder

Monofilamentary tapes (150 pm thickness) were prepared by swaging and rolling silver tubes containing the Bi:2212 ceramic (granulation below 20 mum) and the silver powder (about 0.8 mum). The study has been made, among other samples, on tapes with nominal proportions of 0, 10 and 20 wt.% of silver. The samples were characterized by SEM, and by electrical measurements under varying applied magnetic field. The measurements of J(c) showed that the addition of 10 wt.% silver powder is very beneficent to this property, doubling the obtained values at 60 K, while the 20 wt.% tape presented very low J(c). The tape with no silver content showed to have a J(c) as high as 2.2 x 10(5) A/cm(2), at 4.2 K, zero applied magnetic field. (C) 2004 Elsevier B.V. All rights reserved.

Vortices in superconductors with a columnar defect: Finite size effects

In the present work we investigate the behavior of a vortex in a long superconducting cylinder near to a columnar defect at the center. The derivations of the local magnetic field distribution and the Gibbs free energy will be carried out for a cylinder and a cavity of arbitrary sizes. From the general expressions, it is considered two particular limits: one in which the radius of the cavity is very small but the radius of the superconducting cylinder is kept finite; and one in which the radius of the superconducting cylinder is taken very large (infinite) but the radius of the cavity is kept finite. In both cases the maximum number of vortices which are allowed in the cavity is determined. In addition, the surface barrier field for flux entrance into the cavity is calculated. (c) 2005 Elsevier B.V. All rights reserved.