Deposits of clastic carbonate-dominated (calciclastic) sedimentary slope systems in the rock record have been identified mostly as linearly-consistent carbonate apron deposits, even though most ancient clastic carbonate slope deposits fit the submarine fan systems better. Calciclastic submarine fans are consequently rarely described and are poorly understood. Subsequently, very little is known especially in mud-dominated calciclastic submarine fan systems. Presented in this study are a sedimentological core and petrographic characterisation of samples from eleven boreholes from the Lower Carboniferous of Bowland Basin (Northwest England) that reveals a >250 m thick calciturbidite complex deposited in a calciclastic submarine fan setting. Seven facies are recognised from core and thin section characterisation and are grouped into three carbonate turbidite sequences. They include: 1) Calciturbidites, comprising mostly of highto low-density, wavy-laminated bioclast-rich facies; 2) low-density densite mudstones which are characterised by planar laminated and unlaminated muddominated facies; and 3) Calcidebrites which are muddy or hyper-concentrated debrisflow deposits occurring as poorly-sorted, chaotic, mud-supported floatstones. These

Phd by thesis

To say that this is the best book on the quantum theory of fields is no praise, since to my knowledge it is the only book on this subject But it is a very good and most useful book The original was written in German and appeared in 1942 This is a translation with some minor changes A few remarks have been added, concerning meson theory and nuclear forces, also footnotes referring to modern work in this field, and finally an appendix on the symmetrization of the energy momentum tensor according to Belinfante Quantum Theory of Fields Prof Gregor Wentzel Translated from the German by Charlotte Houtermans and J M Jauch Pp ix + 224, (New York and London: Interscience Publishers, Inc, 1949) 36s

Quantum Theory of Fields

Tables of integrals

The Three-loop splitting functions in QCD: The Singlet case

http://cds.cern.ch/record/257993/files/9401310.pdf

QCD phenomenology based on a chiral effective Lagrangian

Effective hadron theory of QCD

The Yang-Mills Schr\"odinger equation is solved in Coulomb gauge for the vacuum by the variational principle using an Ansatz for the wave functional, which is strongly peaked at the Gribov horizon. A coupled set of Schwinger-Dyson equations for the gluon and ghost propagators in the Yang-Mills vacuum as well as for the curvature of gauge orbit space is derived and solved in one-loop approximation. We find an infrared suppressed gluon propagator, an infrared singular ghost propagator, and an almost linearly rising confinement potential.

http://export.arxiv.org/pdf/hep-th/0408236

Variational solution of the Yang-Mills Schrödinger equation in Coulomb gauge

Extended NJL model for light and heavy mesons without q-q thresholds

Baryons as chiral solitons in the nambu-jona-lasinio model

We solve a truncated system of coupled Dyson-Schwinger equations for the gluon and ghost propagators in $\mathrm{SU}{(N}_{c})$ Yang-Mills theories in Faddeev-Popov quantization on a four-torus. This compact space-time manifold provides an efficient mean to solve the gluon and ghost Dyson-Schwinger equations without any angular approximations. We verify that analytically two powerlike solutions in the very far infrared seem possible. However, only one of these solutions can be matched to a numerical solution for nonvanishing momenta. For a bare ghost-gluon vertex this implies that the gluon propagator is only weakly infrared vanishing, ${D}_{\mathrm{gl}}{(k}^{2})\ensuremath{\propto}{(k}^{2}{)}^{2\ensuremath{\kappa}\ensuremath{-}1},$ $\ensuremath{\kappa}\ensuremath{\approx}0.595,$ and the ghost propagator is infrared singular, ${D}_{\mathrm{gh}}{(k}^{2})\ensuremath{\propto}{(k}^{2}{)}^{\ensuremath{-}\ensuremath{\kappa}\ensuremath{-}1}.$ For nonvanishing momenta our solutions are in agreement with the results of recent SU(2) Monte Carlo lattice calculations. The running coupling possesses an infrared fixed point. We obtain $\ensuremath{\alpha}{(0)=8.92/N}_{c}$ for all gauge groups $\mathrm{SU}{(N}_{c}).$ Above one GeV the running coupling rapidly approaches its perturbative form.

Hugo Reinhardt

Papers

Effective hadron theory of QCD

Variational solution of the Yang-Mills Schrödinger equation in Coulomb gauge

Extended NJL model for light and heavy mesons without q-q thresholds

Baryons as chiral solitons in the nambu-jona-lasinio model

The Elusiveness of infrared critical exponents in Landau gauge Yang-Mills theories