Infrared degrees of freedom of Yang-Mills theory in the Schrodinger representation

We set up a new calculational framework for the Yang-Mills vacuum transition amplitude in the Schrodinger representation. After integrating out hard-mode contributions perturbatively and performing a gauge-invariant gradient expansion of the ensuing soft-mode action, a manageable saddle-point expansion for the vacuum overlap can be formulated. In combination with the squeezed approximation to the vacuum wave functional this allows for an essentially analytical treatment of physical amplitudes. Moreover, it leads to the identification of dominant and gauge-invariant classes of gauge field orbits which play the role of gluonic infrared (IR) degrees of freedom. The latter emerge as a diverse set of saddle-point solutions and are represented by unitary matrix fields. We discuss their scale stability, the associated virial theorem and other general properties including topological quantum numbers and action bounds. We then find important saddle-point solutions (most of them solitons) explicitly and examine their physical impact. While some are related to tunneling solutions of the classical Yang-Mills equation, i.e. to instantons and merons, others appear to play unprecedented roles. A remarkable new class of IR degrees of freedom consists of Faddeev-Niemi type link and knot solutions, potentially related to glueballs.

Superstring in a pp-wave background at finite temperature. TFD approach

A thermodynamical analysis for the type IIB superstring in a pp-wave background is considered. The thermal Fock space is built and the temperature SUSY breaking appears naturally by analyzing the thermal vacuum. All the thermodynamical quantities are derived by evaluating matrix elements of operators in the thermal Fock space. This approach seems to be suitable to study thermal effects in the BMN correspondence context. (C) 2004 Elsevier B.V. All rights reserved.

THE CRYSTAL-STRUCTURE OF BENZOYL-HISTIDINE MONOHYDRATE

The crystal structure of benzoyl-histidine monohydrate (BYLH hereafter), C-13H-12N-3O-3. H2O was determined from three dimensional data of 3012 independent reflections measured on a Enraf-Nonius (CAD4) single crystal diffractometer. The compound crystallizes in the orthorhombic space group P2(1)2(1)2(1) with cell dimensions alpha = 7.102(1) angstrom, b = 13.783(3) angstrom, c = 14.160(4) angstrom, V = 1385.92 angstrom-3, F.W. = 277.28, F(000) = 584 Q(calc) = 1.32 g cm-3 and Z = 4.The structure was solved with direct methods. All positional and anisotropic thermal parameters were refined by full-matrix least-squares calculations. The final reliability factor was R = 0.040, while the weighted one was Rw = 0.034. The H atoms found in the difference Fourier map were refined isotropically.The compound consists of a histidine molecule bound to a benzoyl group. There is also a cocrystallized water molecule stabilized through a hydrogen bridge.The 5-membered ring of the histidine has its tautomeric form, after the transfer of the H atom from the N(delta) to the N(epsilon) atom of the ring. There is an sp2 conformation around C6 while the conformation around C3 is that of sp3. The histidine ring forms with the benzene ring a dihedral angle of 109.8(1)-degree.All angle values and bond distances agree very well with the expected values in the literature.

Physico-chemical parameter correlations in the [RuCl2(CO)(L)(PPh3)2] complexes (L = N-heterocycles)

Fourteen complexes in the series [RuCl2(CO)(L)(PPh3)2] (where L = N-heterocycles) have been prepared and characterized by IR and NMR spectroscopies, and cyclic voltammetry. A good correlation is found between observed and calculated electrochemical potentials; E1/2 vs pKa or (Gp, σm for a series of similar ligands. It is now reported that the carbonyl stretching frequency, νCO, and the 13C and 31P NMR signals do not correlate well with any of the physico-chemical parameters used (E1/2, Taft's and Hammett's parameters). This behaviour is probably due to the characteristics of the Ru(II) species, which does not transmit the steric and electron donor/acceptor properties of the ligands to the carbonyl group, or because the measurements are not able to detect the effect induced by the changes in the ligand L. Indeed, good correlations are obtained when the measurements directly involve the metal centre, as is the case in the E1/2 measurements. Crystals of o[RuCl2(CO)(4-pic)(PPh3)2] are monoclinic, space group P21/n, a = 12.019(2), b = 13.825(3) and c = 22.253(3) . The structure was solved by the Patterson method and was refined by full-matrix least-squares procedure to R = 0.054 and Rw = 0.055, for 2114 reflections with I > 3σ(I). For L = 2-acetylpyridine and 2-methylimidazole, complexes with formulae [RuCl2(CO)(L)(PPh3)] · L and [RuCl2(CO)(L)2 (PPh3)], respectively, were obtained. © 1998 Elsevier Science Ltd. All rights reserved.

Crystal structures and magnetic properties of CuX2(pdmp)2 complexes (X = Br, Cl)

We report the synthesis and the structural and magnetic characterization of two new compounds: dibromobis-(pdmp)copper(II), CuBr2C22H24N4 (1), and dichlorobis(pdmp)copper(II), CuCl2C22H24N4 (2), where pdmp = 1-phenyl-3,5-dimethylpyrazole. The structures were refined by full-matrix least-squares techniques to R1 = 0.0620 and 0.0777, respectively. Compound 1 belongs to the space group P21/n with a = 8.165(5) Å, b = 10.432(3) Å, c = 13.385(4) Å, β = 100.12(4)̊, and Z = 2. Compound 2 belongs to the space group P21/c with a = 8.379(2) Å, b = 22.630(2) Å, c = 12.256(2) Å, β= 98.43(3)°, and Z = 4. It has the same molecular formula as a compound reported previously but a different crystal structure. Detailed single-crystal EPR measurements were performed for single-crystal samples of 1 and 2 at 9 and 35 GHz and at room temperature. The positions and line widths of the EPR lines were measured as a function of the magnetic field orientation in three orthogonal planes. The data were used to study the electronic properties of the copper ions and to evaluate the exchange interactions between them. Our results are discussed in terms of the electronic pathways for superexchange between copper ions, which are provided by the stacking of pyrazole and phenyl rings of neighboring molecules and by hydrogen-halogen bonds. © 1999 American Chemical Society.

Robust control applications for smart truss structure

A finite element modeling of an intelligent truss structure with piezoelectric stack actuators for the purpose of active damping and structural vibration attenuation is presented. This paper concerns with the following issues aspects: the design of intelligent truss structure considering electro-mechanical coupling between the host structure and piezoelectric stack actuators; the H 2 norm approach to search for optimal placement of actuators and sensors; and finally some aspects in robust control techniques. The electro-mechanical behavior of piezoelectric elements is directly related to the successful application of the actuators in truss structures. In order to achieve the desired damping in the interested bandwidth frequency it is used the H ∞ output feedback solved by convex optimization. The constraints to be reached are written by linear matrix inequalities (LMI). The paper concludes with a numerical example, using Matlab and Simulink, in a cantilevered, 2-bay space truss structure. The results demonstrated the approach applicability.

Global optimization for the ℋ∞-norm model reduction problem

A branch and bound algorithm is proposed to solve the [image omitted]-norm model reduction problem for continuous and discrete-time linear systems, with convergence to the global optimum in a finite time. The lower and upper bounds in the optimization procedure are described by linear matrix inequalities (LMI). Also proposed are two methods with which to reduce the convergence time of the branch and bound algorithm: the first one uses the Hankel singular values as a sufficient condition to stop the algorithm, providing to the method a fast convergence to the global optimum. The second one assumes that the reduced model is in the controllable or observable canonical form. The [image omitted]-norm of the error between the original model and the reduced model is considered. Examples illustrate the application of the proposed method.

Controle ótimo H 'INFINITO' e H2 com a locação de pólos e modificação de zeros para rastreamento de sinais e rejeição de distúrbios em sistemas de controle usando LMIs

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Daspu e a redefinição da representação social da prostituta nos meios de comunicação de massa do Brasil

Pós-graduação em Comunicação - FAAC

Educação e relações raciais: percepções de alunos e professores de uma escola pública de São Carlos

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

As novas tecnologias e os limites da formação: uma abordagem a partir da Teoria Crítica

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Controle ativo de vibração de rotores com mancais magnéticos: influência da flexibilidade dos rotores

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Controle ativo de vibrações de rotores com mancais magnéticos: influência dos parâmetros do controlador PID

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)

Efeito de instruções sobre a demonstração de equivalência entre posições

A maioria dos trabalhos sobre equivalência com participantes humanos resultou na formação de classes de equivalência independentemente das características dos estímulos empregados. Entretanto, uma série de estudos recentes utilizando a posição como dimensão relevante de estímulo mostrou resultados negativos, em sua maioria. O presente estudo pretendeu verificar se instruções que tornassem mais clara a tarefa dos participantes resultaria em melhor desempenho na formação de três classes de equivalência formadas pela posição relativa de nove quadrados compondo uma matriz três por três. Dez estudantes universitários que participaram do experimento receberam instruções mínimas. Onze outros receberam instruções adicionais instando-os a levar em conta nas próximas tentativas (tentativas de teste) o que aprenderam no decorrer do experimento (tentativas de linha de base). Dez participantes que receberam instruções adicionais e cinco que receberam instruções mínimas formaram as três classes equivalentes de posição. Deste modo parece evidente que as instruções adicionais facilitaram a formação de equivalência. Entretanto, o presente trabalho também difere dos anteriores em mais dois aspectos: 1) na utilização de uma cor diferente para cada classe, e 2) na permissão de um maior número de testes antes de concluir-se pela não formação de equivalência, favorecendo deste modo, mais extinção de respostas incompatíveis com as contingências programadas.

Análise do enxofre corrosivo em óleo mineral isolante e remoção do dibenzil dissulfeto com nanotubos de carbono baseados em matriz metálica

Falhas inesperadas em transformadores levaram a identificação da formação de sulfeto de cobre, depositado sobre os condutores, avaliando-se da presença qualitativa de enxofre corrosivo resultando na alteração da norma brasileira ABNT NBR 10505, que avalia a presença de enxofre corrosivo em óleo mineral, alterando-se o tempo e a temperatura de ensaio para 150 °C por 48 horas. Realizando-se a especiação química de compostos organosulfurados via cromatografia gasosa acoplada a espectrometria de massas, onde foram encontrados 13 compostos sulfurados no óleo Nynas e 9 compostos no óleo da Petrobras, sendo o dibenzil dissulfeto (DBDS) o de maior concentração, encontrado apenas no óleo Nynas. Para realizar a determinação da presença do DBDS em óleo mineral isolante foi desenvolvido um método através de cromatografia gasosa acoplada a espectrometria de massas, e por este método foi possível quantificar o teor de DBDS em amostras de OMI oriundas de transformadores de potência. Foi avaliado o processo de passivação do cobre por benzotriazol e tolutriazol, utilizados como aditivos anticorrosivos no núcleo dos equipamentos elétricos, verificando-se que o efeito da adição agente de passivação torna-se ineficaz com o passar do tempo. A solução para a remoção de DBDS em óleo mineral foi a utilização de nanotubo de carbono baseado em matriz metálica (NTC/Al) como agente de remoção do DBDS. Verificou-se que o agente de adsorção foi capaz de efetuar a remoção total do DBDS do OMI até um volume de 4000 mL de óleo contaminado com DBDS.