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Both the genomes of the epsilonproteobacteria Wolinella succinogenes and Campylobacter jejuni contain operons (sdhABE) that encode for so far uncharacterized enzyme complexes annotated as ‘non-classical’ succinate:quinone reductases (SQRs). However, the role of such an enzyme ostensibly involved in aerobic respiration in an anaerobic organism such as W. succinogenes has hitherto been unknown. We have established the first genetic system for the manipulation and production of a member of the non-classical succinate:quinone oxidoreductase family. Biochemical characterization of the W. succinogenes enzyme reveals that the putative SQR is in fact a novel methylmenaquinol:fumarate reductase (MFR) with no detectable succinate oxidation activity, clearly indicative of its involvement in anaerobic metabolism. We demonstrate that the hydrophilic subunits of the MFR complex are, in contrast to all other previously characterized members of the superfamily, exported into the periplasm via the twin-arginine translocation (tat)-pathway. Furthermore we show that a single amino acid exchange (Ala86→His) in the flavoprotein of that enzyme complex is the only additional requirement for the covalent binding of the otherwise non-covalently bound FAD. Our results provide an explanation for the previously published puzzling observation that the C. jejuni sdhABE operon is upregulated in an oxygen-limited environment as compared with microaerophilic laboratory conditions.
Perturbation theory for non-abelian gauge theories at finite temperature is plagued by infrared
divergences which are caused by magnetic soft modes ~ g2T, corresponding to gluon fields of
a 3d Yang-Mills theory. While the divergences can be regulated by a dynamically generated
magnetic mass on that scale, the gauge coupling drops out of the effective expansion parameter
requiring summation of all loop orders for the calculation of observables. Some gauge invariant
possibilities to implement such infrared-safe resummations are reviewed. We use a scheme based
on the non-linear sigma model to estimate some of the contributions ~ g6 of the soft magnetic
modes to the QCD pressure through two loops. The NLO contribution amounts to ~ 10% of the
LO, suggestive of a reasonable convergence of the series.
The so-called sign problem of lattice QCD prohibits Monte Carlo simulations at finite baryon
density by means of importance sampling. Over the last few years, methods have been developed
which are able to circumvent this problem as long as the quark chemical potential is m=T <~1.
After a brief review of these methods, their application to a first principles determination of the
QCD phase diagram for small baryon densities is summarised. The location and curvature of the
pseudo-critical line of the quark hardon transition is under control and extrapolations to physical
quark masses and the continuum are feasible in the near future. No definite conclusions can as
yet be drawn regarding the existence of a critical end point, which turns out to be extremely quark
mass and cut-off sensitive. Investigations with different methods on coarse lattices show the lightmass
chiral phase transition to weaken when a chemical potential is switched on. If persisting on
finer lattices, this would imply that there is no chiral critical point or phase transition for physical
QCD. Any critical structure would then be related to physics other than chiral symmetry breaking.
The chiral critical surface is a surface of second order phase transitions bounding the region of
first order chiral phase transitions for small quark masses in the fmu;d;ms;mg parameter space.
The potential critical endpoint of the QCD (T;m)-phase diagram is widely expected to be part of
this surface. Since for m = 0 with physical quark masses QCD is known to exhibit an analytic
crossover, this expectation requires the region of chiral transitions to expand with m for a chiral
critical endpoint to exist. Instead, on coarse Nt = 4 lattices, we find the area of chiral transitions
to shrink with m, which excludes a chiral critical point for QCD at moderate chemical potentials
mB < 500 MeV. First results on finer Nt = 6 lattices indicate a curvature of the critical surface
consistent with zero and unchanged conclusions. We also comment on the interplay of phase
diagrams between the Nf = 2 and Nf = 2+1 theories and its consequences for physical QCD.
We perform a two-flavor dynamical lattice computation of the Isgur-Wise functions t1/2 and t3/2
at zero recoil in the static limit. We find t1/2(1) = 0.297(26) and t3/2(1) = 0.528(23) fulfilling
Uraltsev’s sum rule by around 80%. We also comment on a persistent conflict between theory and
experiment regarding semileptonic decays of B mesons into orbitally excited P wave D mesons,
the so-called “1/2 versus 3/2 puzzle”, and we discuss the relevance of lattice results in this
context.
We present a lattice QCD calculation of the heavy-light decay constants fB and fBs performed with Nf = 2 maximally twisted Wilson fermions, at four values of the lattice spacing. The decay constants have been also computed in the static limit and the results are used to interpolate the observables between the charmand the infinite-mass sectors, thus obtaining the value of the decay constants at the physical b quark mass. Our preliminary results are fB = 191(14)MeV, fBs = 243(14)MeV, fBs/ fB = 1.27(5). They are in good agreement with those obtained with a novel approach, recently proposed by our Collaboration (ETMC), based on the use of suitable ratios having an exactly known static limit.
We present first results from runs performed with Nf = 2+1+1 flavours of dynamical twisted mass fermions at maximal twist: a degenerate light doublet and a mass split heavy doublet. An overview of the input parameters and tuning status of our ensembles is given, together with a comparison with results obtained with Nf = 2 flavours. The problem of extracting the mass of the K- and D-mesons is discussed, and the tuning of the strange and charm quark masses examined. Finally we compare two methods of extracting the lattice spacings to check the consistency of our data and we present some first results of cPT fits in the light meson sector.
"Entre direitos iguais, a força decide", proferiu karl marx ao descrever a antinomia do direito em situações antagônicas das relações de produção capitalistas, em que "o direito [oferece resistência] ao direito" nesse ponto, marx aborda uma questão que se situa no centro de todas as teorias jurídicas críticas: que tipo de violência é velada por meio do mecanismo de ocultação denominado "direito"? Para responder a esta questão, tentar-se-á, a seguir, tornar a teoria da hegemonia de antonio gramsci e seu modelo de direito hegemônico produtivos para o campo da teoria do direito. Tal tarefa tem de lidar com a dupla dificuldade de que, por um lado, gramsci não foi um teórico do direito no sentido mais estrito, razão pela qual o potencial de sua teoria para uma análise do direito raramente foi utilizada. Por outro lado, sua abordagem só pode ser empregada por meio de uma crítica às restrições relacionadas a seu tempo. isso se aplica especialmente à sua concepção de economia como a base e a núcleo essencialista oculto (laclau; mouffe, 2001:69), assim como à sua ideia de 'classismo' sob a forma de um enfoque unilateral das classes, em que há preferencialmente mais de um "pluralismo de poder" e inúmeras lutas (litowitz, 2000: 536). Recuperar-se-á, consequentemente, argumentos-chave, ampliando-os pela utilização das recentes descobertas feitas pelas abordagens feminista e neomaterialista da teoria jurídica, bem como as análises de foucault acerca das tecnologias de poder. por fim, uma interpretação da teoria sistêmica das autonomizações comunicativas.
O 11 de setembro acelerou o desenvolvimento de uma arquitetura transnacional de segurança que intervém profundamente nas liberdades civis individuais, tanto nos direitos básicos dos cidadãos dos Estados como nos direitos humanos dos cidadãos mundiais. O artigo delineia essa arquitetura, mostra como ela dissolve as categorias jurídicas tradicionais que preservam a liberdade e discute por que hoje se aceita amplamente a prioridade da segurança sobre a liberdade.
Os limites da tolerância
(2009)
Este artigo apresenta os elementos constitutivos do conceito de tolerância e discute duas concepções diferentes do termo, como permissão e como respeito moral, que expressam modos diversos de demarcar os limites da tolerância. A tolerância é apresentada como um conceito que, para ganhar algum conteúdo, depende normativamente de um direito à justificação baseado na idéia de um uso público da razão segundo o qual as práticas e as instituições político-jurídicas que determinam a vida social dos cidadãos devem ser justificáveis à luz de normas que eles não podem recíproca e genericamente rejeitar.