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Showing papers in "European Physical Journal C in 1982"


Journal ArticleDOI
W. Furmanski, Roberto Petronzio1
TL;DR: In this article, a summary of QCD formulae describing the effects of scaling violation in leptonhadron processes, with the inclusion of recently derived higher order corrections, is presented, and a comparative analysis of various processes as well as an independent analysis of each of them is possible.
Abstract: We present a summary of QCD formulae describing the effects of scaling violation in leptonhadron processes, with the inclusion of recently derived higher order corrections. Deep inelastic leptoproduction, one-hadron inclusive distributions in leptoproduction and ine + e − annihilation and Drell-Yan processes are discussed in detail. Higher order corrections to parton densities, fragmentation functions and to lepton-parton cross-sections in the above processes are presented in a common factorization scheme, so that a comparative analysis of various processes as well as an independent analysis of each of them is possible. A discussion of the various scheme dependences at next-to-leading level is also included.

303 citations


Journal ArticleDOI
TL;DR: In this article, the relation between the calculus of differential forms and concepts of algebraic topology is shown to be a useful method for a completely analogous treatment of the problems in the continuum and on the lattice.
Abstract: The geometrical description of spinor fields by E. Kahler is used to formulate a consistent lattice approximation of fermions. The relation to free simple Dirac fields as well as to Susskind's description of lattice fermions is clarified. The first steps towards a quantized interacting theory are given. The correspondence between the calculus of differential forms and concepts of algebraic topology is shown to be a useful method for a completely analogous treatment of the problems in the continuum and on the lattice.

205 citations


Journal ArticleDOI
TL;DR: In this paper, an attempt is made to extract the gluon distributionG(x, Q2=4 GeV2) from the observed scaling violations of structure functions.
Abstract: Using recent data on deep inelastic lepton-nucleon scattering an attempt is made to extract the gluon distributionG(x, Q 2=4 GeV2) from the observed scaling violations of structure functions. The accuracy of the data allows only for a rough determination of the gluon distribution. In particular it is found that a hard gluon distributionis consistent with present measurements. Implications of the hard gluon distribution for charm production in the gluon fusion model and for the perturbative contributions to σ L /σ T are further discussed. Finally, analytic parametrizations of the QCDx- andQ 2-dependence of quark and gluon distributions are presented facilitating further possible applications.

174 citations


Journal ArticleDOI
TL;DR: In this article, a large sample of opposite-sign dimuons, produced by the interaction of neutrinos and antineutrinos in iron, is analyzed to provide information on the strength and space-time structure of the charm-producing weak current.
Abstract: A large sample of opposite-sign dimuons, produced by the interaction of neutrinos and antineutrinos in iron, is analysed. The data agree very well with the hypothesis that the extra muon is the product of charm decay. They yield information on the strength and space-time structure of the charmproducing weak current. The strange-sea structure functionxs(x) is determined. The difference between neutrino and antineutrino dimuon production is analysed to provide a value of the Kobayashi-Maskawa weak mixing angleθ2.

158 citations


Journal ArticleDOI
TL;DR: In this paper, the invariant isospin-even πN amplitude D+(ν2,t) to the Cheng-Dashen point, ν=0, t=2μ.
Abstract: Dispersion relations in the (ν2,t) plane along hyperbolas are used in order to extrapolate the invariant isospin-even πN amplitude D+(ν2,t) to the Cheng-Dashen point, ν=0, t=2μ. The fluctuation of the results obtained with different hyperbolas gives a realistic estimate of the errors, except for errors of the partial wave solution and of the ππ $$ - N\bar N$$ amplitudes assumed at t < 4μ2 —If our ππ $$ - N\bar N$$ partial waves are used, which are based on the ππs-wave scattering length a 0 0 =0.28 μ-1, the result for the sigma term is 64±8 MeV, in agreement with earlier determinations.—The discrepancy with the theoretical prediction σπN≈ 30 MeV is smaller by only 8 MeV, if our $$ - N\bar N$$ amplitudes are modified in such a way that the threshold behaviour of the ππs-wave agrees with Weinberg's prediction a 0 0 =0.16 μ-1. Further progress depends on new accurate experimental π±p scattering data in the Coulomb interference region at low energies.

115 citations


Journal ArticleDOI
TL;DR: In this article, the analytic calculation of the Sterman-Weinberg type 3-jet cross section to order αs was presented, and the fit to recent PLUTO data gave αs which corresponds to Λ=0.24 GeV in the 1-loop approximation.
Abstract: We present in detail the analytic calculation of the Sterman-Weinberg type 3-jet cross section to order αs2 The fit to recent PLUTO data gives in the\({MS}\) scheme αs which corresponds to Λ=0.24 GeV in the 1-loop approximation.

111 citations


Journal ArticleDOI
R. Cahn1
TL;DR: In this paper, the problem of extracting the phase of the hadronic proton-proton scattering amplitude from its interference with the Coulombic amplitude near the forward direction was re-examined using an eikonal model.
Abstract: The problem of extracting the phase of the hadronic proton-proton scattering amplitude from its interference with the Coulombic amplitude near the forward direction is re-examined using an eikonal model. The results are in accord with the Feynman diagrammatic calculation of West and Yennie, with some small corrections. An especially compact forms is derived for the electromagnetic shift in the hadronic amplitude's phase, which includes the effect of the electromagnetic form factor. The largest modification of the previous results comes from the effect of the form factor on the phase of the electromagnetic amplitude itself.

88 citations


Journal ArticleDOI
TL;DR: In this article, simple relations among intercepts and slopes of Regge trajectories based on the topological expansion and the string picture of hadrons are derived, and the corresponding mass relations for bosons with different quark content are satisfied with a very high accuracy.
Abstract: Simple relations among intercepts and slopes of Regge trajectories based on the topological expansion and\(q\bar q\)-string picture of hadrons are derived. It is shown that the corresponding mass relations for bosons with different quark content are satisfied with a very high accuracy.

78 citations


Journal ArticleDOI
TL;DR: In this article, it was shown that γγ into hadrons is a rather effective means of searching for four-quark states from (9.0+) to (4.5+).
Abstract: It is shown that the reactions γγ into hadrons is a rather effective means of searching for fourquark states. We predict the suppression ofS *(980,0+) and δ(980,0+) in γγ→ππ and γγ→π0 η respectively, if they are four-quark states from (9.0+). The well-known anomaly in γγ→ρ 0 ρ 0 is interpreted as the production of the tensor four-quark resonances with the isospin 0 and 2. We predict the absence of similar enhancement in γγ→ρ + ρ −. The bright anomalies are predicted near thresholds of γγ→ρ 0 ω and γγ→ρ 0 ϕ

76 citations


Journal ArticleDOI
TL;DR: In this article, the influence of coherence in a soft parton bremsstrahlung on hadron spectra in jets is discussed and a simple functional method for calculation of different inclusive parton distributions in the “plateau” region is presented.
Abstract: The influence of coherence in a soft parton bremsstrahlung on hadron spectra in jets is discussed. We present a simple functional method for calculation of different inclusive parton distributions in the “plateau” region. Inclusive parton cross sections, spectra, multiplicities, energy and angular correlations, etc. are derived in the Double Logarithmic approximation.

61 citations


Journal ArticleDOI
TL;DR: In this paper, the renormalization of the three pseudoscalar gauge invariant operators which appear in the Adler-Bell-Jackiw anomaly is studied in the back ground field gauge, where it is simplest.
Abstract: The renormalization of the three pseudoscalar gauge invariant operators which appear in the Adler-Bell-Jackiw anomaly is studied in the back-ground field gauge, where it is simplest. We analyse questions concerning renormalization-group invariance, mixing, the γ5-perscription inD dimensions, as well as the meaning of the nonrenormalization of the axial anomaly in the context of the renormalization of composite operators.

Journal ArticleDOI
TL;DR: In this paper, the direct photon signal relative to neutral-pion production increases with the number of collisions at the CERN ISR and shows little dependence on the transverse moment.
Abstract: Direct photon and neutral-pion production have been measured inpp collisions at the CERN ISR for 30< $$\sqrt s $$ <63 GeV and transverse momenta up to 12 GeV/c. The direct photon signal relative to neutral-pion production increases withp T and shows little $$\sqrt s $$ -dependence. Results are reported from a variety of running conditions, and details are given on the method of analysis and on the evaluation of systematic errors for the inclusive cross-section of single-photon and neutral-pion production.

Journal ArticleDOI
TL;DR: In this article, a cross section for the production of mesons and particles in proton-proton interactions at the full phase space is presented, and a strong energy dependence of the production cross sections is observed.
Abstract: The inclusive cross section for the production ofK 0 mesons, Λ and $$\bar \Lambda$$ particles in proton-proton interactions at $$\sqrt s = 63$$ GeV is presented. The produced particles have been detected in the full phase space. Behaviour of the longitudinal and transversal depandences of the cross sections are discussed. The total production cross sections for 0 mesons and Λ particles was determined to $$\sigma _{{\rm K}_S^0 } = (25.5 \pm 1.4)$$ mb andσ Λ =(7.8±1.2) mb respectively. A strong energy dependence of the production cross sections is observed.

Journal ArticleDOI
TL;DR: In this paper, the complicated Lagrangians for massless as well as massive Yang-Mills fields and their BRS and anti-BRS transformations were simplified by the help of an auxiliary field.
Abstract: The complicated Lagrangians for massless as well as massive Yang-Mills fields and their BRS and anti-BRS transformations proposed by Curci and Ferrari are simplified by the help of an auxiliary field. In the massive non-Abelian case, the mechanism of the breakdown of physicalS-matrix unitarity is clarified and contrasted to the situation in the Abelian case.

Journal ArticleDOI
TL;DR: In this paper, the observed scaling violations of the nucleon structure function were analyzed in the framework of perturbative QCD to determine the shape and magnitude of the gluon distribution.
Abstract: The observed scaling violations of the nucleon structure functionF 2 and $$\bar q$$ have been analysed in the framework of perturbative QCD to determine the shape and magnitude of the gluon distribution. The data are in good agreement with leading order QCD, and the simultaneous use ofF 2 and $$\bar q$$ structure functions permits, for the first time, a reliable determination of the gluon structure function.

Journal ArticleDOI
TL;DR: In this paper, the αs corrections to quark vacuum condensate contributions to various types of current correlation functions are discussed and their relevance to the first Weinberg sum rule is discussed.
Abstract: We present the αs corrections to quark vacuum condensate contributions to various types of current correlation functions. Their relevance to the first Weinberg sum rule is discussed. A new derivation of the relation between theA1-mass and the ϱ-mass is presented. The higher order corrections to the socalled non-perturbative quark mass are also discussed.

Journal ArticleDOI
TL;DR: In this paper, the angular distribution of the low energy jet axis with respect to the high-energy jet axis in an abelian gluon model (QED) and a phase space model (PS) is calculated.
Abstract: We consider the reactionse+e−→γ*→4 jets andZo→4 jets with the 4 jets coming in two pairs of essentially back to back jets of high and low energy. We calculate the angular distribution of the low energy jet axis with respect to the high energy jet axis in QCD, in an abelian gluon model “QED” and a phase space model (PS). Using simple helicity arguments we show that our angular distribution is very sensitive to the triple gluon coupling in QCD. This is then confirmed by a complete calculation. Our correlation offers, therefore, a direct test for QCD as a non-abelian gauge theory.

Journal ArticleDOI
TL;DR: The standard SU(2) lattice theory model without fermions may be considered as a Z2 model with monopoles and fluctuating coupling constants as mentioned in this paper, and at low temperatures β−1 (= small bare coupling constant) the monopoles are confined.
Abstract: The standardSU(2) lattice gauge theory model without fermions may be considered as aZ2 model with monopoles and fluctuating coupling constants. At low temperatures β−1 (=small bare coupling constant) the monopoles are confined.

Journal ArticleDOI
TL;DR: In this paper, an analysis of ωρ0ρ0 ω invariant mass range from 1.2 to 2.0 GeV is presented, where the authors exclude a dominant contribution from JP=0− or 2− states.
Abstract: We present an analysis ofρ0ρ0 production by two photons in theρ0ρ0 invariant mass range from 1.2 to 2.0 GeV. From a study of the angular correlations in the process γγ→ρ0ρ0→π−π+π− we exclude a dominant contribution fromJP=0− or 2− states. The data indicate sizeable contributions fromJP=0+ for four pion massesM4π 1.7 GeV. The data are also well described by a model with isotropic production and uncorrelated isotropic decay of theρ0,s. The cross section stays high below the nominalρ0ρ0 threshold, i.e.M4π<1.5 GeV. The matrix element forρ0ρ0 production is found to decrease steeply with increasingM4π. Upper limits for the couplings of the ι(1440) and Θ(1640) to γγ andρ0ρ0 are given:Γ(ι→γγ)·B(ι→ρ0ρ0)<1.0 keV andΓ(Θ→γγ)

Journal ArticleDOI
L. Bergström1
TL;DR: In this article, the rare electromagnetic decay of a neutral pseudoscalar meson into a lepton pair was calculated in a bound state quark model, where the leading QCD diagram was argued to be dominant allowing higher order QCD corrections to be neglected.
Abstract: The rare electromagnetic decay of a neutral pseudoscalar meson into a lepton pair is calculated in a bound state quark model. For heavy mesons, the leading QCD diagram is argued to be dominant allowing higher order QCD corrections to be neglected for the branching ratio of this decay to the two-photon decay. The experimentally interesting case of pion decay is treated separately, and the rates for competing processes (weak neutral currents, axions, technicolour ...) are estimated. We conclude that existing data may well allow for such contributions.

Journal ArticleDOI
TL;DR: Spin-spin asymmetries have been calculated in the inclusive process in this paper with reference to photon gluon events only and are relatively insensitive to the exact form of the structure functions used.
Abstract: Spin-spin asymmetries have been calculated in the inclusive process\(\mu ^ + p \to \mu c\bar cX\) with reference to photon gluon events only. The resulting asymmetries are small and relatively insensitive to the exact form of the structure functions used.

Journal ArticleDOI
TL;DR: In this paper, the bulk of data from deep inelasticep, eD, μp, μN, νp and νN scattering is fitted with a new diquark model of nucleons.
Abstract: The bulk of data from deep inelasticep, eD, μp, μN, νp and νN scattering is fitted with a new diquark model of nucleons. The proton is found to be mostly in au(ud)0 state, where the (ud)0 diquark has spin and isospin zero. There is hence no trace ofSU(6) symmetry among diquarks in nucleons.

Journal ArticleDOI
TL;DR: In this paper, the Weinberg type sum rules were analyzed in the light of the Laplace transform sum rule and including the leading nonperturbative effects, and bounds on the pseudoscalar decay amplitudes and the gluon component of the meson mass were derived.
Abstract: We reanalyse the Weinberg type sum rules in the light of the Laplace transform sum rule and including the leading non-perturbative effects. We then estimate the light quark invariant masses\(\hat m_s /\hat m_d ,\hat m_u \hat m_d \); the pion decay amplitudefπ and theA1 coupling and mass. Using other type of sum rules, we derive bounds on the pseudoscalar decay amplitudesf p (P≡π, K, D, F) as well as on the gluon component of theU(1) A meson mass. Our main results are summarized in Sect. 4.

Journal ArticleDOI
TL;DR: In this paper, the jet character of the hadronic final states produced ine+e− annihilations is studied in terms of jet measures such as thrust, sphericity, jet opening angle and jet masses, in the energy range 7.7 to 31.6 GeV.
Abstract: The jet character of the hadronic final states produced ine+e− annihilations is studied in terms of jet measures such as thrust, sphericity, jet opening angle and jet masses, in the energy range 7.7 to 31.6 GeV. All distributions and averages have been corrected for detector effects and initial state radiation. The energy dependence of the averages of these jet quantities is used to estimate the contributions due to perturbative QCD and fragmentation effects. Correlations between the jet measures and the multiplicity of charged hadrons are also presented.

Journal ArticleDOI
TL;DR: In this paper, the results of an experiment to study elastic photoproduction were presented, and the results showed that the photon ϕ coupling constant was consistent with the observed photon energy and over a wide range of momentum transfer.
Abstract: The results of an experiment to study elasticK + K − photoproduction are presented. Differential cross sections and spin density matrix elements for ϕ(1.019) production are stddied as a function of incident photon energy and over a wide range of momentum transfer,t (t min >t>−1.5(GeV/c)2). Helicity conserving amplitudes are observed to dominate ϕ production throughout this range and the differential cross sections exhibit a forward diffractive peak which cannot be understood in terms of a simple exponential dependence. A new value of the photon ϕ coupling constant is determined and shown to be consistent withe + e − annihilation measurements. A detailed study of the energy dependence of the differential cross sections is made, including other experimental data, and the extracted effective Regge trajectory compared with other diffractive processes. A study of the dependence of theK + K − decay angular distribution on invariant mass reveals evidence for ans wave contribution interfering with thep wave ϕ which may be attributable to theS * meson.

Journal ArticleDOI
F. M. Renard1
TL;DR: In this paper, the physical interest of γγ collisions is examined and a basic formalism is established for γ collisions with general couplings and polarization states, and crosssections are computed with generalized couplings.
Abstract: The physical interest ofγe ± collisions is examined. A basic formalism is established. Crosssections are computed with general couplings and polarization states. Illustrations are given for QED tests, Z0 andW ± production, various electro-weak processes including γγ collisions and the search for new currents and particles.

Journal ArticleDOI
TL;DR: In this paper, the Callan-Symanzik γ-function is studied in the large number of lepton (in QED) or flavour (in qCD) limit.
Abstract: The Callan-Symanzik γ-function is studied in the large number of lepton (in QED) or flavour (in QCD) limit. We have computed analytically 7 terms and they show a striking factorization. We have computed numerically 19 terms and they show a large radius of convergence and two unambiguous zeros within the region of convergence.

Journal ArticleDOI
TL;DR: In this paper, the authors considered the gauge invariance constraints in Hamiltonian lattice gauge theories, focusing mainly on pure SU(2) Yang-Mills theory in 2+1 dimensions.
Abstract: We consider in detail the gauge invariance constraints in Hamiltonian lattice gauge theories, focusing mainly on pureSU(2) Yang-Mills theory in 2+1 dimensions. We present matrix and partial differential representations of the Hamiltonian in which all gauge constraints have been taken fully into account. The applicability of this formulation is demonstrated on small lattices.

Journal ArticleDOI
TL;DR: In this paper, a new K*\(\bar K\)+c.c. resonance with a mass of 1.526±6 MeV, a width of (107±15) MeV and quantum numbers IPC=01++ was presented.
Abstract: Evidence is presented for a newK*\(\bar K\)+c.c. resonance with a mass of (1,526±6) MeV, a width of (107±15) MeV and quantum numbersIJPC=01++. We call itD′ meson. Initially it is observed as aK*\(\bar K\)+c.c. enhancement in the reactionsK−p→(K s 0 K±π∓)Λ at 4.2 GeV/c. The isospin assignmentI=0 comes from its further observation in the reactionsK−p→(K s 0 K±π∓)Σ0 andK−p→(K s 0 K±π∓)Σ(1,385)0 but not inK−p→(K+K−π−)Σ+ orK−p→(K s 0 K±π∓)Σ(1,385)+. A maximum likelihood analysis of the (K\(\bar K\)π) decay Dalitz plots in the reactionsK−p→(K s 0 K±π∓) determines theJPC of theD′ meson to be 1++. A satisfactorySU(3) fit is obtained to a 1++ nonet composed of theI-1A1, theI=1/2QA with theD(1,285) and theD′(1,526) as theI=0 members having a mixing angle close to the magic one.

Journal ArticleDOI
TL;DR: In this paper, the authors compared the rate of muon pairs produced from thermalized quark-gluon matter to that of pairs produced via the usual Drell-Yan mechanism.
Abstract: Characteristics of muon pair production in very high energy nucleus-nucleus collisions are discussed. Particular attention is given to comparing the rate of muon pairs produced from thermalized quark-gluon matter to that of pairs produced via the usual Drell-Yan mechanism. The thermal rate is at least of the same order of magnitude as the direct Drell-Yan rate and will certainly dominate whenxF for the pair approaches 1. BeyondxF=1 the thermal rate is also substantial. This region is particularly easily accessible in fixed target experiments.