Diário da Constituinte [gravação de vídeo] : [programa n. 530 2ª edição]

Mobilização de Governadores de Estado e da Ordem dos Advogados do Brasil (OAB) em prol da realização de eleições presidenciais em 1988. Debate sobre a diferença entre empresa de capital nacional e a empresa de capital estrangeiro. Obstrução da pauta de votação sobre o capítulo Da Ordem Econômica.

Diário da Constituinte [gravação de vídeo] : [programa n. 661 2ª ed.]

PMDB garante que o projeto da Constituinte será votado com ou sem acordo. A Frente Nacional de Ação Ecológica se reuniu com os constituintes com a preocupação com a poluição que vem causando prejuízos à saúde. O projeto sobre o Meio ambiente apresenta

Diário da Constituinte [gravação de vídeo] : [programa n. 676 2ª ed.]

Debate acerca do marco legal sobre a comercialização, transfusão e captação de sangue no País. Contaminação de pacientes hemofílicos pelo vírus HIV. Convocação, pelo Presidente Ulysses Guimarães, dos constituintes para registro de presença em plenário.

Diário da Constituinte [gravação de vídeo] : [programa n. 680 2ª ed.]

Ulysses Guimarães faz apelo para a votação do segundo turno, que deve terminar o Capítulo das Liberdades Individuais e Coletivas, ainda faltam 56 incisos para votação neste capítulo. Já foram aprovados 27 incisos e são dados como certo de aprovação: o habeas data, a defesa do consumidor, racismo, o mandado de injunção e coletivo. Os direitos individuais recebem o apoio de todos os setores. Ulysses Guimarães apela para que os constituintes compareçam para a votação do 2º turno para apreciar 708 destaques.

PP backward elastic scattering between 0.70 and 2.37 GeV/c

̄pp backward elastic scattering has been measured for the cos θ_cm region between – 1.00 and – 0.88 and for the incident ̄p laboratory momentum region between 0.70 and 2.37 GeV/c. These measurements, done in intervals of approximately 0.1 GeV/c, have been performed at the Alternating Gradient Synchrotron at Brookhaven National Laboratory during the winter of 1968. The measured differential cross sections, binned in cos θ_cm intervals of 0.02, have statistical errors of about 10%. Backward dipping exists below 0.95 GeV/c and backward peaking above 0.95 GeV/c. The 180˚ differential cross section extrapolated from our data shows a sharp dip centered at 0.95 GeV/c and a broad hump centered near 1.4 GeV/c. Our data have been interpreted in terms of resonance effects and in terms of diffraction dominance effects.

A study of T=1, T=3/2, and T=2 states in some light nuclei using (He^3,n) reactions

The (He³, n) reactions on B¹¹, N¹⁵, O¹⁶, and O¹⁸ targets have been studied using a pulsed-beam time-of-flight spectrometer. Special emphasis was placed upon the determination of the excitation energies and properties of states with T = 1 (in Ne¹⁸), T = 3/2 (in N¹³ and F¹⁷) and T = 2 (in Ne²⁰). The identification of the T = 3/2 and T = 2 levels is based on the structure of these states as revealed by intensities and shapes of angular distributions. The reactions are interpreted in terms of double stripping theory. Angular distributions have been compared with plane and distorted wave stripping theories. Results for the four reactions are summarized below:

1) O¹⁶ (He³, n). The reaction has been studied at incident energies up to 13.5 MeV and two previously unreported levels in Ne¹⁸ were observed at E_x = 4.55 ± .015 MeV (Γ = 70 ± 30 keV) and E_x = 5.14 ± .018 MeV (Γ = 100 ± 40 keV).

2) B¹¹ (He³, n). The reaction has been studied at incident energies up to 13.5 MeV. Three T = 3/2 levels in N¹³ have been identified at E_x = 15.068 ± .008 MeV (Γ ˂ 15 keV), E_x = 18.44 ± .04, and E_x 18.98 ± .02 MeV (Γ = 40 ± 20 keV).

3) N¹⁵ (He³, n). The reaction has been studied at incident energies up to 11.88 MeV. T = 3/2 levels in F¹⁷ have been identified at E_x = 11.195 ± .007 MeV (Γ ˂ 20 keV), E_x = 12.540 ± .010 MeV (Γ ˂ 25 keV), and E_x = 13.095 ± .009 MeV (Γ ˂ 25 keV).

4) O¹⁸ (He³, n). The reaction has been studied at incident energies up to 9.0 MeV. The excitation energy of the lowest T = 2 level in Ne²⁰ has been found to be 16.730 ± .006 MeV (Γ ˂ 20 keV).

Angular distributions of the transitions leading to the above higher isospin states are well described by double stripping theory. Analog correspondences are established by comparing the present results with recent studies (t, p) and (He³, p) reactions on the same targets.

Blue Marlin, Makaira nigricans, Movements in the Western North Atlantic Ocean: Results of a Cooperative Game Fish Tagging Program, 1954-88

Blue marlin, Makaira nigricans, tag and recapture data are summarized for 1954-1988. During this period, 8,447 fish have been tagged and only 30 (0.35 percent) have been returned. Results of the tagging program indicate that blue marlin not only travel considerable distances (7,OOO km from the U. S. Virgin Islands to the Ivory Coast of West Africa), but have remained at large for up to 8 years. Seasonal movements, however, are difficult to determine accurately.

Purification, characterization and cytokine release function of a novel Arg-49 phospholipase A(2) from the venom of Protobothrops mucrosquamatus

Group IIA phospholipase A(2) (PLA(2)) are major components in Viperidae/Crotalidae venom. In the present study, a novel PLA(2) named promutoxin with Arg at the site 49 has been purified from the venom of Protobothrops muerosquamatus by chromatography. It

Technological aspects of preservation and processing of edible shell fish 2. Influence of season on the chemical composition of crab (Scylla serrata)

The purpose of this communication is to bring out the influence of season on the chemical composition of crab, covering a period of 2 years. Changes in moisture, protein, water extractable nitrogen, non-protein nitrogen, glycogen, lactic acid, fat and free amino acid composition of crab meat have been reported on a monthly basis.

8×8重排无阻塞型SOI热光波导开关阵列

设计并制作了一种重排无阻塞型的8×8 SOI热光波导开关阵列。开关单元采用了MM I-MZI结构的2×2光开关。整个器件的开关时间约为2μs。器件中开关单元功耗小于240mW。消光比在17~22dB范围内变化。功耗和开关速度都明显优于SiO2基和聚合物基的开关阵列。

Study of the νi13/2－1 band in 189Pt

High-spin levels of 189Pt have been studied with the in-beam γ-spectroscopy method via the 176Yb(18O,5n) reaction at the beam energies of 88 and 95 MeV. The previously known νi-131/2 band has been confirmed, and its unfavored signature branch extended up to the 13/2+ state. Within the framework of the triaxial particle-rotor model, the νi-113/2 band is suggested to be associated with the 11/2[615] configuration, and to have triaxial deformation.

8×8单元CsI(Tl)探测阵列研制；Development of 88 CsI(Tl) array detector

描述了1个8×8单元CsI(Tl)探测阵列的结构和工作原理。探测阵列的每个单元是由1块前表面21 mm×21 mm、后表面23.1 mm×23.1 mm、高50 mm的CsI(Tl)棱台、1块光导和光电倍增管组成。在兰州放射性次级束流线(RIBLL)上对探测阵列进行测试,得到探测阵列对30 MeV质子的能量分辨可达2.7%,对170 MeV7Be可达1.5%,可很好地用于放射性束物理实验中带电粒子的鉴别。

8×8单元CsI(Tl)阵列探测器的研制

近二十年，世界上各大实验室相继建立了各具特色的放射性束流装置，放射性束物理得到了长足的发展，在实验上要求对反应产物进行全运动学测量且具有较高的精度，为实验探测装置提出了更高的要求。我们研制了8×8单元CsI(Tl)阵列探测器，主要用于测量核反应产物的能量和角分布、进行粒子的关联测量以及对粒子的鉴别。脉冲形状甄别（PSD）技术是一种重要的鉴别粒子的方法，已经从原来直接利用电子学硬件的方法发展到先采集到脉冲波形，进而进行离线分析，甚至利用现代数字信号处理(DSP)技术的在线分析。我们对该技术进行了一些初步的研究，为以后利用DSP技术研制PSD系统奠定了重要的基础。本论文工作的主要内容有：（1）探测器的研制和性能测试。该探测器由64块CsI(Tl)晶体组成,每块晶体由光电倍增管单独读出。该探测器覆盖较大的立体角，具有较好的能量分辨和粒子鉴别能力。本文对探测器的探测原理，结构及性能进行较详细的说明。（2）系统地对两部分比较法(Qfast/Qslow，Qfast/Qtotal，Qslow/Qtotal)进行了模拟计算，定性的分析了两部分的积分门的延迟和宽度，为实验提供了有效的指导。分别采集到α源和宇宙线(m子)两种脉冲波形，使用两部分比较、平均时间、确定幅度和确定时间四种方法进行离线分析，对四种分析方法进行比较，以选择甄别效果最好的分析方法。最后，对关于进一步工作的方向进行了简要的讨论