The authors report an odderon Regge trajectory emerging from a field theoretical Coulomb gauge QCD model for the odd signature J{sup PC} (P = C = -1) glueball states (oddballs). The trajectory intercept is clearly smaller than the pomeron and even the {omega} trajectory's intercept which provides an explanation for the nonobservation of the odderon in high energy scattering data. To further support this result we compare to glueball lattice data and also perform calculations with an alternative model based upon an exact Hamiltonian diagonalization for three constituent gluons
The bound state of two massive constituent gluons is studied in the potential approach. The relativi...
Abstract We develop a formalism where the hard and soft pomeron contributions to high energy scatter...
AbstractIn this work we propose a modified holographic softwall model, analytically solvable, to cal...
We perform lattice calculations of the lightest J=0,2,4,6 glueball masses in the D=3+1 SU(3) gauge t...
AbstractIn this work we use gauge/string dualities and a dynamical model that takes into account dyn...
AbstractWe perform lattice calculations of the lightest J=0,2,4,6 glueball masses in the D=3+1 SU(3)...
The Coulomb gauge Hamiltonian model is used to calculate masses for selected JPC states consisting o...
We compute glueball masses for even spins ranging from 0 to 6, in the D = 2 + 1 SU(2) lattice gauge ...
In this work we use the holographic soft-wall AdS/QCD model with anomalous dimension contributions c...
This thesis comprises two investigations, both connected with the attempt to understand Regge theory...
Theoretical developments and applications of an effective QCD Hamiltonian in the Coulomb gauge are s...
In this paper we extend our recent non perturbative functional renormalization group analysis of Reg...
The Confinement 8 proceedings will be published in the journal “Proceedings of Science” (PoS) organi...
In this work we propose a modified holographic softwall model, analytically solvable, to calculate t...
We reinterpret the JIMWLK/KLWMIJ evolution equation as the QCD Reggeon field theory (RFT). The basic...
The bound state of two massive constituent gluons is studied in the potential approach. The relativi...
Abstract We develop a formalism where the hard and soft pomeron contributions to high energy scatter...
AbstractIn this work we propose a modified holographic softwall model, analytically solvable, to cal...
We perform lattice calculations of the lightest J=0,2,4,6 glueball masses in the D=3+1 SU(3) gauge t...
AbstractIn this work we use gauge/string dualities and a dynamical model that takes into account dyn...
AbstractWe perform lattice calculations of the lightest J=0,2,4,6 glueball masses in the D=3+1 SU(3)...
The Coulomb gauge Hamiltonian model is used to calculate masses for selected JPC states consisting o...
We compute glueball masses for even spins ranging from 0 to 6, in the D = 2 + 1 SU(2) lattice gauge ...
In this work we use the holographic soft-wall AdS/QCD model with anomalous dimension contributions c...
This thesis comprises two investigations, both connected with the attempt to understand Regge theory...
Theoretical developments and applications of an effective QCD Hamiltonian in the Coulomb gauge are s...
In this paper we extend our recent non perturbative functional renormalization group analysis of Reg...
The Confinement 8 proceedings will be published in the journal “Proceedings of Science” (PoS) organi...
In this work we propose a modified holographic softwall model, analytically solvable, to calculate t...
We reinterpret the JIMWLK/KLWMIJ evolution equation as the QCD Reggeon field theory (RFT). The basic...
The bound state of two massive constituent gluons is studied in the potential approach. The relativi...
Abstract We develop a formalism where the hard and soft pomeron contributions to high energy scatter...
AbstractIn this work we propose a modified holographic softwall model, analytically solvable, to cal...