Practical tools for third order cosmological perturbations

We discuss cosmological perturbation theory at third order, deriving the gauge transformation rules for metric and matter perturbations, and constructing third order gauge invariant quantities. We present the Einstein tensor components, the evolution equations for a perfect fluid, and the Klein-Gordon equation at third order, including scalar, vector and tensor perturbations. In doing so, we also give all second order tensor components and evolution equations in full, exhilarating generality.Comment: 17 pages, revtex4; v2: corresponds to version published in JCA

Anatomia do cone medular aplicada à via epidural de administração de fármacos em macacos-prego ( Sapajus libidinosus )

Resumo: Com este estudo objetivou-se descrever a topografia do cone medular do macaco-prego (Sapajus libidinosus) a fim de fornecer suporte para que a realização de procedimentos anestésicos, bem como exames de mielografia e coleta de líquor, dentre outros procedimentos que utilizam a via epidural. Para tanto foram dissecados oito animais, sendo seis machos e duas fêmeas, de diferentes faixas etárias. Rebateu-se a pele para retirada da musculatura da região dorsal, exposição de toda a coluna vertebral e identificação das vértebras lombares e sacrais. Para estabelecer o final da medula espinhal e medir o comprimento do cone medular, foi aberto todo o canal vertebral lombossacro, seccionando-se lateralmente os arcos vertebrais. Em seguida a duramáter foi seccionada para visualização do cone medular e observação da relação topográfica deste com as vértebras. Todos os animais apresentaram cinco vértebras lombares e três vértebras sacrais. As vértebras se apresentaram, de forma geral, muito próximas e com os processos espinhosos bem desenvolvidos e direcionados em sentido cranial. O cone medular dos macacos-prego situou-se entre as vértebras L2 e L5, com a base localizando-se com maior frequência na altura da vértebra L3, enquanto o ápice em L4. O comprimento corporal (espaço interarcual occiptoatlântico até o espaço interarcual sacrocaudal) variou de 22,9 a 31,8cm, com média de 27,44 ±3,1cm enquanto que comprimento do cone medular variou de 1,70 a 3,51cm, com média de 2,47 ±0,57cm. Não houve correlação entre o tamanho do corpo e o comprimento do cone medular (r = 0,212). Conclui-se que apesar das variações do comprimento e posicionamento do cone medular, o seu ápice não ultrapassa a articulação lombossacral, tornando seguro o acesso ao espaço epidural por esta via

In the social factory? Immaterial labour, precariousness and cultural work

This article introduces a special section concerned with precariousness and cultural work. Its aim is to bring into dialogue three bodies of ideas -- the work of the autonomous Marxist 'Italian laboratory'; activist writings about precariousness and precarity; and the emerging empirical scholarship concerned with the distinctive features of cultural work, at a moment when artists, designers and (new) media workers have taken centre stage as a supposed 'creative class' of model entrepreneurs. The paper is divided into three sections. It starts by introducing the ideas of the autonomous Marxist tradition, highlighting arguments about the autonomy of labour, informational capitalism and the 'factory without walls', as well as key concepts such as multitude and immaterial labour. The impact of these ideas and of Operaismo politics more generally on the precarity movement is then considered in the second section, discussing some of the issues that have animated debate both within and outside this movement, which has often treated cultural workers as exemplifying the experiences of a new 'precariat'. In the third and final section of the paper we turn to the empirical literature about cultural work, pointing to its main features before bringing it into debate with the ideas already discussed. Several points of overlap and critique are elaborated -- focusing in particular on issues of affect, temporality, subjectivity and solidarity

Direct Measurements of DT Fuel Preheat from Hot Electrons in Direct-Drive Inertial Confinement Fusion

Hot electrons generated by laser-plasma instabilities degrade the performance of laser-fusion implosions by preheating the DT fuel and reducing core compression. The hot-electron energy deposition in the DT fuel has been directly measured for the first time by comparing the hard x-ray signals between DT-layered and mass-equivalent ablator-only implosions. The electron energy deposition profile in the fuel is inferred through dedicated experiments using Cu-doped payloads of varying thickness. The measured preheat energy accurately explains the areal-density degradation observed in many OMEGA implosions. This technique can be used to assess the viability of the direct-drive approach to laser fusion with respect to the scaling of hot-electron preheat with laser energy

Direct Measurements of DT Fuel Preheat from Hot Electrons in Direct-Drive Inertial Confinement Fusion

Submitted for publication in Physical Review LettersHot electrons generated by laser-plasma instabilities degrade the performance of laser-fusion implosions by preheating the DT fuel and reducing core compression. The hot-electron energy deposition in the DT fuel has been directly measured for the first time by comparing the hard x-ray signals between DT-layered and mass-equivalent ablator-only implosions. The electron energy deposition profile in the fuel is inferred through dedicated experiments using Cu-doped payloads of varying thickness. The measured preheat energy accurately explains the areal-density degradation observed in many OMEGA implosions. This technique can be used to assess the viability of the direct-drive approach to laser fusion with respect to the scaling of hot-electron preheat with laser energy

Inferences of hot electron preheat and its spatial distribution in OMEGA direct drive implosions

Submitted for publication in Physics of PlasmasHot electrons generated from laser plasma instabilities degrade performance of direct drive implosions by preheating the deuterium and tritium (DT) fuel resulting in early decompression and lower areal densities at stagnation. A technique to quantify the hot electron preheat of the dense DT fuel and connect it to the degradation in areal density is described in detail. Hot electrons are measured primarily from the hard x-rays they emit as they slow down in the target. The DT preheat is inferred from a comparison of the hard x-ray signals between a DT-layered implosion and its mass equivalent ablator only implosion. The preheat energy spatial distribution within the imploding shell is inferred from experiments using high Z payloads of varying thicknesses. It is found that the electrons deposit their energy uniformly throughout the shell material. For typical direct-drive OMEGA implosions driven with an overlapped intensity of ∼9·10^14 W/cm2, approximately ∼0.02%–0.03% of the laser energy is converted into preheat of the stagnated fuel which corresponds to areal density degradations of 10%–20%. The degradations in areal density explain some of the observed discrepancies between the simulated and measured areal densities