498 research outputs found

    Effective Action of Composite Fields for General Gauge Theories in BLT-Covariant Formalism

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    The gauge dependence of the effective action of composite fields for general gauge theories in the framework of the quantization method by Batalin, Lavrov and Tyutin is studied. The corresponding Ward identities are obtained. The variation of composite fields effective action is found in terms of new set of operators depending on composite field. The theorem of the on-shell gauge fixing independence for the effective action of composite fields in such formalism is proved. brief discussion of gravitational-vector induced interaction for Maxwell theory with composite fields is given.Comment: Typos corrected. Latex fil

    Superfield extended BRST quantization in general coordinates

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    We propose a superfield formalism of Lagrangian BRST-antiBRST quantization of arbitrary gauge theories in general coordinates with the base manifold of fields and antifields desribed in terms of both bosonic and fermionic variables.Comment: LaTex, 10 page

    More on the Subtraction Algorithm

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    We go on in the program of investigating the removal of divergences of a generical quantum gauge field theory, in the context of the Batalin-Vilkovisky formalism. We extend to open gauge-algebrae a recently formulated algorithm, based on redefinitions δλ\delta\lambda of the parameters λ\lambda of the classical Lagrangian and canonical transformations, by generalizing a well- known conjecture on the form of the divergent terms. We also show that it is possible to reach a complete control on the effects of the subtraction algorithm on the space Mgf{\cal M}_{gf} of the gauge-fixing parameters. A principal fiber bundle EMgf{\cal E}\rightarrow {\cal M}_{gf} with a connection ω1\omega_1 is defined, such that the canonical transformations are gauge transformations for ω1\omega_1. This provides an intuitive geometrical description of the fact the on shell physical amplitudes cannot depend on Mgf{\cal M}_{gf}. A geometrical description of the effect of the subtraction algorithm on the space Mph{\cal M}_{ph} of the physical parameters λ\lambda is also proposed. At the end, the full subtraction algorithm can be described as a series of diffeomorphisms on Mph{\cal M}_{ph}, orthogonal to Mgf{\cal M}_{gf} (under which the action transforms as a scalar), and gauge transformations on E{\cal E}. In this geometrical context, a suitable concept of predictivity is formulated. We give some examples of (unphysical) toy models that satisfy this requirement, though being neither power counting renormalizable, nor finite.Comment: LaTeX file, 37 pages, preprint SISSA/ISAS 90/94/E

    Resistive Transition and Upper Critical Field in Underdoped YBa_2Cu_3O_{6+x} Single Crystals

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    A superconducting transition in the temperature dependence of the ab-plane resistivity of underdoped YBa_2Cu_3O_{6+x} crystals in the range T_c<30 K has been investigated. Unlike the case of samples with the optimal level of doping, the transition width increased insignificantly with magnetic field, and in the range T_c<13 K it decreased with increasing magnetic field. The transition point T_c(B) was determined by analyzing the fluctuation conductivity. The curves of B_{c2}(T) measured in the region T/T_c>0.1 did not show a tendency to saturation and had a positive second derivative everywhere, including the immediate neighborhood of T_c. The only difference among the curves of B_{c2}(T) for different crystal states is the scales of T and B, so they can be described in terms of a universal function, which fairly closely follows Alexandrov's model of boson superconductivity.Comment: 10 Revtex pages, 6 figures, uses psfig.st

    Optimal values of rovibronic energy levels for triplet electronic states of molecular deuterium

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    Optimal set of 1050 rovibronic energy levels for 35 triplet electronic states of D2D_2 has been obtained by means of a statistical analysis of all available wavenumbers of triplet-triplet rovibronic transitions studied in emission, absorption, laser and anticrossing spectroscopic experiments of various authors. We used a new method of the analysis (Lavrov, Ryazanov, JETP Letters, 2005), which does not need any \it a priory \rm assumptions concerning the molecular structure being based on only two fundamental principles: Rydberg-Ritz and maximum likelihood. The method provides the opportunity to obtain the RMS estimates for uncertainties of the experimental wavenumbers independent from those presented in original papers. 234 from 3822 published wavenumber values were found to be spurious, while the remaining set of the data may be divided into 20 subsets (samples) of uniformly precise data having close to normal distributions of random errors within the samples. New experimental wavenumber values of 125 questionable lines were obtained in the present work. Optimal values of the rovibronic levels were obtained from the experimental data set consisting of 3713 wavenumber values (3588 old and 125 new). The unknown shift between levels of ortho- and para- deuterium was found by least squares analysis of the a3Σg+a^3\Sigma_g^+, v=0v = 0, N=0÷18N = 0 \div 18 rovibronic levels with odd and even values of NN. All the energy levels were obtained relative to the lowest vibro-rotational level (v=0v = 0, N=0N = 0) of the a3Σg+a^3\Sigma_g^+ electronic state, and presented in tabular form together with the standard deviations of the empirical determination. New energy level values differ significantly from those available in literature.Comment: 46 pages, 9 picture

    Is soft breaking of BRST symmetry consistent?

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    A definition of soft breaking of BRST symmetry in the field-antifield formalism is proposed, valid for general gauge theories and arbitrary gauge fixing. The Ward identities for the generating functionals of Green's functions are derived, and their gauge dependence is investigated. We discuss the Gribov-Zwanziger action for the one-parameter family of R_xi gauges. It is argued that gauge theories with a soft breaking of BRST symmetry are inconsistent.Comment: 1+16 pages; v2: example of section 5 changed to R_xi gauges; v3: small corrections to section 5, one reference added, published versio

    Anomalously large oxygen-ordering contribution to the thermal expansion of untwinned YBa2Cu3O6.95 single crystals: a glass-like transition near room temperature

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    We present high-resolution capacitance dilatometry studies from 5 - 500 K of untwinned YBa2Cu3Ox (Y123) single crystals for x ~ 6.95 and x = 7.0. Large contributions to the thermal expansivities due to O-ordering are found for x ~ 6.95, which disappear below a kinetic glass-like transition near room temperature. The kinetics at this glass transition is governed by an energy barrier of 0.98 +- 0.07 eV, in very good agreement with other O-ordering studies. Using thermodynamic arguments, we show that O-ordering in the Y123 system is particularly sensitive to uniaxial pressure (stress) along the chain axis and that the lack of well-ordered chains in Nd123 and La123 is most likely a consequence of a chemical-pressure effect.Comment: 4 pages, 3 figures, submitted to PR

    Simulation method of the low-Re flows in the packed bed technological equipment

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    The paper shows the semiempirical method of a numerical simulation of the low-Re flows in the packed bed technological apparatus. The proposed method is based on the Navier-Stokes equations modification by the linear momentum sources equations in the packed bed zones. It is found that the simulation error of the proposed method is not more than 6.2% for low-density finite element meshes. The average value of the simulation error is about 3.0% for all shown cases. It was found that the proposed method simulation error almost independents on the mesh density. In the main, the simulation error is determined by the linear momentum sources equations approximation error. © Published under licence by IOP Publishing Ltd

    Collisional kinetics of non-uniform electric field, low-pressure, direct-current discharges in H2_{2}

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    A model of the collisional kinetics of energetic hydrogen atoms, molecules, and ions in pure H2_2 discharges is used to predict Hα_\alpha emission profiles and spatial distributions of emission from the cathode regions of low-pressure, weakly-ionized discharges for comparison with a wide variety of experiments. Positive and negative ion energy distributions are also predicted. The model developed for spatially uniform electric fields and current densities less than 10310^{-3} A/m2^2 is extended to non-uniform electric fields, current densities of 10310^{3} A/m2^2, and electric field to gas density ratios E/N=1.3E/N = 1.3 MTd at 0.002 to 5 Torr pressure. (1 Td = 102110^{-21} V m2^2 and 1 Torr = 133 Pa) The observed far-wing Doppler broadening and spatial distribution of the Hα_\alpha emission is consistent with reactions among H+^+, H2+_2^+, H3+_3^+, and HH^-H ions, fast H atoms, and fast H2_2 molecules, and with reflection, excitation, and attachment to fast H atoms at surfaces. The Hα_\alpha excitation and H^- formation occur principally by collisions of fast H, fast H2_2, and H+^+ with H2_2. Simplifications include using a one-dimensional geometry, a multi-beam transport model, and the average cathode-fall electric field. The Hα_\alpha emission is linear with current density over eight orders of magnitude. The calculated ion energy distributions agree satisfactorily with experiment for H2+_2^+ and H3+_3^+, but are only in qualitative agreement for H+^+ and H^-. The experiments successfully modeled range from short-gap, parallel-plane glow discharges to beam-like, electrostatic-confinement discharges.Comment: Submitted to Plasmas Sources Science and Technology 8/18/201
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