Alvará com força de Lei, pelo qual Vossa Alteza Real he servido crear hum Conselho Supremo Militar, e de Justiça, na forma acima declarada : para Vossa Alteza Real ver / João Alvares de Miranda Varejão o fez

Variação de Título: Criação do Conselho Supremo Militar

Alvará, por que V. Magestade he servido declarar que a todos os Ministtros, e Officiaes de Justiça, Fazenda, ou Guerra he permitido negocear por meio da Companhia Geral do Grão Pará, e Maranhão, e de quaesquer outras por V. Magestade confirmadas, e que não possão ser dados de suspeitos nas causas, e dependencias civeis, ou crimes respectivas às ditas Companhias, com o pretexto de terem acçoens nellas ; tudo na forma acima declarada : para Vossa Magestade ver / Filippe Joseph da Gama o fez

Ao alto do título: Sebastião Joseph de Carvalho e Mello.

Alvará, porque V. Magestade he servido declarar o parágrafo dezoito da Instituição da Companhia Geral do Grão Pará, e Maranhão : na forma, que nelle se contém : para V. Magestade ver : Filippe Joseph da Gama o fez

Ao alto do título: Sebastião Joseph de Carvalho e Mello.

Alvará com força de Lei, porque Vossa Magestade he servido declarar, que a graça concedida á Companhia Geral do Graõ Pará, e do Maranhaõ, em quanto isenta as madeiras de Siza, sómente se deve entender daquellas, que vierem destinadas pra se venderem nestes Reinos; e quanto ás madeiras, que vierem por conta, e risco dos moradores de Lisboa, ou de quaesquer outros Vassallos destes Reinos, para o gasto das suas obras, e que tiverem proporção com o consumo dellas, sem excesso, nem dólo, sejaõ isentas de todos os direitos, e pensoens, da mesma fórma, que pelo Regimento do Paço da Madeira, o foraõ sempre comfórme o paragrapho segundo do capitulo onze : para Vossa Magestade ver

Ao alto do titulo: Sebastião Joseph de Carvalho e Mello.

Alvará em forma de Ley, pelo qual V. Magestade he servido declarar as assignaturas, e emolumentos, que devem haver os Ouvidores, Juizes, e seus Officiaes das Comarcas das Minas Geraes, Cuyabá, Mato Grosso, S. Paulo, e Goyaz, e nas que ficão no Continente do Governo da Bahia, e todas as mais, que se descobrirem nos mesmos, ou diversos Governos ; e tudo na forma, que acima se declara : para Vossa Magestade ver

Ao alto do título : Diogo de Mendonça Corte-Real.

Alvará com força de Ley, porque V. Magestade he servido ordenar, que todo Official, que constar haver constrangido, ou sugerido as pessoas, que se apresentarem nas Casas de Fundição com ouro, para nellas se fundir, que o manifestem em nome diverso, do ue ellas voluntariamente quizerem declarar, perca o valor do officio, que servir, e fique desde logo suspenso, sendo executores da suspensão os Governadores das respectivas Capitanias, na fôrma que acima se declara : para Vossa Magestade ver

Ao alto do título : Thomé Joaquim da Costa Corte-Real.

Alvará, por que Vossa Alteza Real he servido ampliar, e declarar o outro alvará de vinte e hum de janeiro de mil oitocentos e nove, comprehendendo nos privilegios conferidos aos proprietarios dos engenhos de assucar, e lavradores de canas, as dividas, e execuções fiscaes ; na forma acima declarada : para Vossa Alteza Real ver

Variação do título : Extensão de isenção de penhoras dos engenhos de açúcar.

Inter-stage line ratio of He- and Li-like Ti emissions for the electron temperature measurement

Under coronal conditions, the steady state rate-equations are used to calculate the inter-stage line ratios between Li-like Is(2)2p(P-2(3/2))-> 1s(2)2s -> ((2) S-1/2) and He-like 1s2p (P-1(1))-> 1s(2) (S-1(0)) transitions for Ti in the electronic temperature ranges from 0.1 keV to 20 keV. The results show that the. temperature sensitivities are higher at the electronic temperature less than 5000 eV and the temperature sensitivities will decrease with the increase of electronic temperature.

Single attosecond pulse generation in He+ by controlling the instant ionization rate using attosecond pulse trains combined with an intense laser pulse

High-order harmonics and single attosecond pulse generation by using an infrared laser pulse combined with attosecond pulse trains (APT) interacting with He+ have been investigated. We show that the ionization for different instant time intervals can be controlled by altering the time delay between the APT and the infrared pulse. Consequently, APT can be used as a tool to control the efficiency of high-order harmonics emitted at different times. By choosing appropriate APT and time delay, the driving pulse width for single attosecond pulse generation can be extended up to six optical cycles. (c) 2007 Optical Society of America.

Origin of the double-peak structure in longitudinal momentum distributions for single ionization of an He atom in strong laser field

The single ionization of an He atom by intense linearly polarized laser field in the tunneling regime is studied by S- matrix theory. When only the first term of the expansion of the S matrix is considered and time, spatial distribution, and fluctuation of the laser pulse are taken into account, the obtained momentum distribution in the polarization direction of laser field is consistent with the semiclassical calculation, which only considers tunneling and the interaction between the free electron and external field. When the second term, which includes the interaction between the core and the free electron, is considered, the momentum distribution shows a complex multipeak structure with the central minimum and the positions of some peaks are independent of the intensity in some intensity regime, which is consistent with the recent experimental result. Based on our analysis, we found that the structures observed in the momentum distribution of an He atom are attributed to the " soft" collision of the tunneled electron with the core.

An investigation of the three-body reaction He^3(He^3, 2p)He^4

Reactions produced by the He³ bombardment of the He³ have been investigated for bombarding energies from 1 to 20 MeV using a tandem Van de Graaff accelerator. Proton spectra from the three-body reaction He³(He³, 2p)He⁴ have been measured with a counter telescope at 13 angles for 9 bombarding energies between 3 and 18 MeV. The results are compared with a model for the reaction which includes a strong p-He⁴ final-state interaction. Alpha-particle spectra have been obtained at 12 and 18 MeV for forward angles with a magnetic spectrometer. These spectra indicate a strongly forward-peaked mechanism involving the ¹S₀ p-p interaction in addition to the p-He⁴ interaction. Measurements of p-He⁴ and p-p coincidence spectra at 10 MeV confirm these features of the reaction mechanism. Deuteron spectra from the reaction of He³(He³, d)pHe³ have been measured at 18 MeV. A triton spectrum from the reaction He³(He³, t)3p at 20 MeV and 4⁰ is interpreted in terms of a sequential decay through an excited state of the alpha particle at 20.0 MeV. No effects are observed which would indicate an interaction in the residual (3p) system. Below 3 MeV the He³(He³, 2p)He⁴ reaction mechanism is observed to be changing and further measurements are suggested in view of the importance of this reaction in stellar interiors.

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.