Polimorfismo genético de citocinas na população do Rio de Janeiro

Citocinas são moléculas que controlam e modulam a atividade de numerosas células por se ligarem a seus receptores específicos. As diferenças observadas na produção de citocinas entre indivíduos podem ser, pelo menos em parte, explicadas pelos polimorfismos genéticos como o polimorfismo de um único nucleotídeo (SNP). Em 181 indivíduos saudáveis não-aparentados da cidade do Rio de Janeiro (região Sudeste - Brasil), nós analisamos os polimorfismos de citocinas em genes que codificam para Fator de Necrose Tumoral-alfa (TNF-a), Fator de Crescimento Transformante-beta (TGF-b), Interleucina-10, Interleucina-6 e Interferon-gama (IFN-g). Reação em cadeia da polimerase utilizando-se iniciadores sequencia-específicos foi realizada com auxílio do kit comercial CytGen (One Lambda Inc. Canoga Park, CA, USA). Ao todo, 8 polimorfismos foram analisados: TNF-a (-308G/A); TGF-b (códon 10C/T, códon 25C/G); IL-10 (-1082A/G, -819T/C, -592A/C); IL-6 (-174C/G) e IFN-g (+874T/A). Os dados observados foram comparados a três grupos de população de diferentes regiões do Brasil (São Paulo, Paraná e Bahia) e a três populações de outros continentes (Itália, Eslováquia e Negros Norte-Americanos). O teste qui-quadrado foi utilizado para as comparações. Nossa análise da população do Rio de Janeiro mostrou que os as freqüências alélicas em IL-10, IL-6 e IFN-g são desigualmente distribuídos entre Brancos, Mulatos e Negros (p<0,05). A comparação com populações de outras regiões do Brasil revelou que Rio de Janeiro e Bahia possuem freqüências alélicas e genotípicas de TGF-b (códon 25) estatisticamente diferentes (p=0,004 e p=0,002, respectivamente). Ainda, a freqüência alélica na população do Rio de Janeiro é significativamente diferente quando comparada à população da Itália [IL-6 (-174), p=0,0092; e IFN-g (+874) p=0,0418)]; Eslováquia [IL-10(-1082), p=0,006; IL-6(-174), p=0,0002; e IFN-g(+874), p=0,0335]; e Afro-Americanos [IL-10(-819), p=0,0446; IL-6(-174), p<0,0001; e IFN-g(+874), p<0,0001]. Adicionalmente, observamos que a diferença na distribuição dos haplótipos em IL-10 (-1082/-819/-592) na população do Rio de Janeiro em comparação com a da Itália (p=0,0293) e Afro-Americanos (p=0,0025) é significativa. Portanto, concluímos que os polimorfismos em IL-10, IL-6 e IFN-g estão distribuídos de acordo com a etnia na população do Rio de Janeiro. A população do Rio de Janeiro possui freqüências de polimorfismos diferentes das populações de Bahia, Itália, Eslováquia e Afro-Americanos, mas semelhantes à população de São Paulo/Paraná. Nossas observações poderão ser úteis para futuros estudos e associação entre polimorfismos genéticos de citocinas e doenças na população do Rio de Janeiro.

Observational constraints on the unified dark matter and dark energy model based on the quark bag model

In this work we investigate if a small fraction of quarks and gluons, which escaped hadronization and survived as a uniformly spread perfect fluid, can play the role of both dark matter and dark energy. This fluid, as developed in [1], is characterized by two main parameters: beta, related to the amount of quarks and gluons which act as dark matter; and gamma, acting as the cosmological constant. We explore the feasibility of this model at cosmological scales using data from type Ia Supernovae (SNeIa), Long Gamma-Ray Bursts (LGRB) and direct observational Hubble data. We find that: (i) in general, beta cannot be constrained by SNeIa data nor by LGRB or H(z) data; (ii) gamma can be constrained quite well by all three data sets, contributing with approximate to 78% to the energy matter content; (iii) when a strong prior on (only) baryonic matter is assumed, the two parameters of the model are constrained successfully. (C) 2014 The Authors. Published by Elsevier B.V.

A novel optical subdivision method for dual-frequency interferometer

The theory of optical subdivision techniques of dual-frequency laser interferometers is stated. And a novel optical subdivision technique is proposed originally to enhance resolution of a commercial interferometer by adding some corner-cubes. Then the performance of the interferometer is tested. The interferometer resolution of 1.24 nm and the average error of below 2 nm are achieved by using the technique. The most novel of the optical subdivision technique is without lambda/4 plates. It is less sensitive to environmental changes, it has prodigious potential to improve resolution farther and it can reduce polarization mixing error. (C) 2007 Elsevier GmbH. All rights reserved.

Infrared (1.2-1.6 mu m) luminescence in Yb, Cr : YAG with 940 nm diode pumping

Infrared (1.2-1.6 mum) luminescence in a yttrium aluminium garnet (YAG) crystal, co-doped with Yb (10 at.%) and Cr (0.05 at.%) ions, was investigated under CW laser diode pumping (lambda = 940 nm). The Cr4+ emission band was observed with its peak at 1.35 mum and measured to be about 6% with respect to Yb3+ IR luminescence (lambda = 1.03 mum). Analysis of the crystal absorption and luminescence spectra allows one to conclude that Yb3+-Cr4+ energy transfer is a mechanism responsible for the B-3(2)(T-3(2))-B-3(1)((3)A(2)) emission of Cr4+ ions. This crystal is promising as an efficient source of the near infrared emission. (C) 2004 Elsevier B.V. All rights reserved.

Infrared (1.2-1.6 mu m) luminescence in Cr4+: Yb3Al5O12 single crystal with 940 nm diode pumping

Infrared (1.2-1.6 mu m) luminescence in a ytterbium aluminium garnet (YbAG) crystal, doped with Cr (0.05 at.%) ions, was investigated under CW laser diode pumping (lambda = 940 nm). The Cr4+ emission band was observed with its peak at 1.34 mu m and measured to be about 1.3 times with respect to Yb3+ IR luminescence (lambda = 1.03 mu m). We demonstrate that for the excitation wavelength of 940 nm Yb3+ ions act as sensitizers of the B-3(2)(T-3(2))-B-3(1)((3)A(2)) emission of Cr4+ ions. This crystal is promising as a high-efficient system for tunable laser (1.2-1.6 mu m) output. (c) 2004 Elsevier B.V. All rights reserved.

Cr4+在Al2O3多晶体中的光谱性能研究

Transparent polycrystalline Cr:Al2O3 ceramics were synthesized by conventional pressureless synthesis processing. The absorption and emission spectra of Cr:Al2O3 ceramics specimens before and after annealing were measured at room temperature. It was discovered that the emission spectra of Cr4+ in Al2O3 octahedral coordination site is in infrared wavelength range of 1100-1600 nm. The emission peak of Cr4+ is centered at 1223 nm, which is similar to that of Cr4+ in tetrahedral site. Al2O3 has smaller lattice constant, resulting in the larger crystal field strength, so there is a blue shift in the peak of Cr4+:Al2O3 ceramics compared to those of other Cr4+-doped crystals. And the emission band is much narrower with full width at half maximum Delta lambda 37 nm.

高浓度掺Er^3＋铌酸锂晶体的光谱参数计算

用提拉法成功地生长了6mol％的高浓度掺铒铌酸锂晶体。测量了晶体的两个非偏振方向（X和Z）以及两个偏振方向（π和δ）的吸收光谱。高浓度掺铒铌酸锂晶体的吸收系数高，有利于提高泵浦效率。根据所测的吸收光谱用Judd-Ofelt理论拟合出了Er^3＋离子的强度参数Ωλ。所得的均方差结果显示偏振拟合的误差要小于非偏振拟合。利用偏振吸收数据计算了各能级跃迁的自发辐射跃迁几率（AJJ’）、辐射寿命（τ）、荧光分支比（β）和积分发射截面（σp）等参数，对计算结果进行了讨论并与其他文献的报道结果进行了比较。

Effects of CO2 laser conditioning of the antireflection Y2O3/SiO2 coatings at 351 nm

Y2O3/SiO2 coatings were deposited on fused silica by electron beam evaporation. A continuous wave CO2 laser was used to condition parts of the prepared samples at different scanning speeds in the air. LAMBDA 900 spectrometer was used to investigate the changes of the transmittance and residual reflection spectrum. A Nomarski microscope under dark field was used to examine the changes of the micro defect density. The changes of the surface roughness and the microstructure of the film before and after conditioning were investigated by AFM and X-ray diffraction, respectively. We found that laser-induced damage threshold (LIDT) of the films conditioning at 30 mm/s scanning speed was increased by more than a factor of 3 over the thresholds of the as-deposited films. The conditioning effect was correlated with an irradiation-induced decrease of the defect density and absorption of the films. (c) 2005 Elsevier B.V. All rights reserved.

Stress, absorptance and laser-induced damage threshold properties of 355-nm HR coatings

A number of 355-nm Al2O3/MgF2 high-reflectance (HR) coatings were prepared by electron-beam evaporation. The influences of the number of coating layers and deposition temperature on the 355-nm Al2O3/MgF2 HR coatings were investigated. The stress was measured by viewing the substrate deformation before and after coating deposition using an optical interferometer. The laser-induced damage threshold (LIDT) of the samples was measured by a 355-nm Nd:YAG laser with a pulse width of 8 ns. Transmittance and reflectance of the samples were measured by a Lambda 900 spectrometer. It was found that absorptance was the main reason to result in a low LIDT of 355-nm Al2O3/MgF2 HR coatings. The stress in Al2O3/MgF2 HR coatings played an unimportant role in the LIDT, although MgF2 is known to have high tensile stress.

Study of Al2O3/MgF2 HR coatings at 355 nm

With the present work we tried to study the effective methods to improve the laser-induced damage threshold (LIDT) and reflectance of HR coatings at 355 nm. The work presented in this paper wits part of an ongoing study about vacuum annealing. It was dedicated to study the effects Of Vacuum annealing with different temperature gradients on the structure, optical properties and laser-induced damage threshold (LIDT) of 355nm Al2O3/MgF2HR coatings. A number of samples were prepared by electron beam evaporation using the same deposition process with an optimal deposition temperature of 280 degrees C. After deposition, samples were annealed in the coating chamber for 3 h with different temperature gradients. Morphologies of the samples were observed by Leica-DMRXE. Microscope, Structure of the samples had been characterized by X-ray diffraction (XRD). Transmittance and reflectance of the samples were measured by Lambda 900 Spectrometer, The LIDT of the samples was measured by a 355 nm Nd:YAG laser with a pulse width of 8 ns. It was found that the temperature gradient of vacuum annealing had significant effects on the morphology, structure, absorption, and LIDT of the samples, (c) 2005 Elsevier Ltd. All rights reserved.

Overcoat dependence of laser-induced damage threshold of 355 nm HR coatings

A series of HR coatings, with and without overcoat, were prepared by electron beam evaporation using the same deposition process. The laser-induced damage threshold (LIDT) was measured by a 355 nm Nd:YAG laser with a pulse width of 8 ns. Damage morphologies of samples were observed by Leica-DMRXE Microscope. The stress was measured by viewing the substrate deformation before and after coatings deposition using an optical interferometer. Reflectance of the samples was measured by Lambda 900 Spectrometer. The theoretical results of electric field distributions of the samples were calculate by thin film design software (TFCalc). It was found that SiO2 overcoat had improved the LIDT greatly, while MgF2 overcoat had little effect on the LIDT because of its high stress in the HR coatings. The damage morphologies were different among HR coatings with and without overcoats. (c) 2005 Elsevier B.V. All rights reserved.

离子束溅射沉积不同厚度铜膜的光学常数研究

利用Lambda-900分光光度计对离子束溅射沉积不同厚度Cu膜测定的反射率和透射率，运用哈德雷方程，并考虑基片后表面的影响，对离子束溅射沉积的Cu膜光学常数进行了计算。结果表明，在同一波长情况下，膜厚小于100nm的纳米Cu膜光学常数随膜厚变化明显；膜厚大于100nm后，Cu膜的光学常数趋于一定值。Cu膜不连续时的光学常数与连续膜时的光学常数随波长变化规律不同；不同厚度的连续膜的光学常数随波长变化规律相同，但大小随膜厚变化而变化。

Cu膜的光学特性尺寸效应及最小连续膜厚研究

采用离子束溅射在K9玻璃基底上沉积了不同厚度的Cu膜，利用Lambda-900分光光度计，测量了波长为310nm到1300nm范围内Cu膜的反射率和透射率．选定波长为310、350、400、430、550、632、800、1200nm时对薄膜的反射率、透射率和吸收率随膜厚变化的关系进行研究．同时，对Cu膜的光学常量也进行了讨论．结果显示，Cu膜的光学特性都有明显的尺寸效应．将波长为550nm时的反射率和透射率随Cu膜厚度变化关系的交点对应厚度作为特征厚度，该厚度可认为是金属Cu膜生长从不连续膜进入连续膜的

1064nm倍频波长分离膜的制备与性能研究

通过对主膜系添加匹配层并借助计算机对膜系进行优化，设计出结构规整、性能优良的1064ilm倍频波长分离膜。用电子束蒸发及光电极值监控技术在K9玻璃基底上沉积薄膜，将样品置于空气中在260℃温度下进行3h热退火处理。然后用Lambda 900分光光度计测量了样品的光谱性能；用表面热透镜(STL)技术测量了样品的弱吸收值；用调Q脉冲激光装置测试了样品的抗激光损伤阈值(LIDT)。实验结果发现，样品的实验光谱性能与理论光谱性能有很好的一致性。退火前后其光谱性能几乎没有发生温漂，说明薄膜的温度稳定性好；同时退火使

纳米Mo膜的光学特性及最小连续膜厚研究

利用Lambda-900分光光度计，在波长为310～1250nm范围内测量了离子束溅射沉积不同厚度纳米Mo膜的反射率和透射率。选定波长为310nm，350nm，400nm，500nm，550nm，632nm，800nm，1200nm时对薄膜的反射率、透射率和吸收率随膜厚变化的关系进行了讨论。实验结果显示，纳米Mo膜的光学特性有明显的尺寸效应。提出将薄膜对光波长为550nm时的反射率和透射率随Mo膜厚度变化关系的交点对应的厚度作为特征厚度，该厚度可认为是纳米Mo膜生长从不连续膜进入连续膜的最小连续膜厚。利用