As a first step towards a strong coupling expansion of Yang-Mills theory, the SU(2) Yang-Mills quantum mechanics of spatially constant gauge fields is investigated in the symmetric gauge, with the six physical fields represented in terms of a positive definite symmetric (3 x 3) matrix S. Representing the eigenvalues of S in terms of elementary symmetric polynomials, the eigenstates of the corresponding harmonic oscillator problem can be calculated analytically and used as orthonormal basis of trial states for a variational calculation of the Yang-Mills quantum mechanics. In this way high precision results are obtained in a very effective way for the lowest eigenstates in the spin-0 sector as well as for higher spin. Furthermore I find, that...
Using the technique of finite field dependent BRST transformations we show that the classical massiv...
We investigate the topological properties of the SU(3) pure gauge theory by performing numerical sim...
Supersymmetric Yang-Mills theory is formulated in six dimensions, without the use of anti-commuting ...
As a first step towards a strong coupling expansion of Yang-Mills theory, the SU(2) Yang-Mills quant...
The smallness of the variation rate of the hamiltonian matrix elements compared to the (square of th...
The motivation and perspectives of numerical simulations of supersymmetric Yang-Mills theories are r...
Recent results obtained within the Hamiltonian approach to continuum Yang-Mills theory in Coulomb ga...
The problem of the pairing interaction is dealt with even Grassmann variables in the hamiltonian fra...
I review theory and phenomenology of (K/2,K/2)*[(1/2,0)+(0,1/2)] states. First I make the case t...
AbstractThe quantum mechanics of spatially constant SU(2) Yang–Mills- and Dirac-fields minimally cou...
We propose a mean-field approach to the Duffing oscillator to construct perturbatively the bounded o...
The free energy in the weak-coupling phase of two-dimensional Yang-Mills theory on a sphere for SO(N...
We discuss the precise relation of the open N=2 string to a self-dual Yang-Mills (SDYM) system in 2+...
Coulomb gauge Yang-Mills theory is considered within the first order formalism. It is shown that the...
The idea of a spin-charge separation of the SU(2) gauge potential is extended to the SU(3) case. It ...
Using the technique of finite field dependent BRST transformations we show that the classical massiv...
We investigate the topological properties of the SU(3) pure gauge theory by performing numerical sim...
Supersymmetric Yang-Mills theory is formulated in six dimensions, without the use of anti-commuting ...
As a first step towards a strong coupling expansion of Yang-Mills theory, the SU(2) Yang-Mills quant...
The smallness of the variation rate of the hamiltonian matrix elements compared to the (square of th...
The motivation and perspectives of numerical simulations of supersymmetric Yang-Mills theories are r...
Recent results obtained within the Hamiltonian approach to continuum Yang-Mills theory in Coulomb ga...
The problem of the pairing interaction is dealt with even Grassmann variables in the hamiltonian fra...
I review theory and phenomenology of (K/2,K/2)*[(1/2,0)+(0,1/2)] states. First I make the case t...
AbstractThe quantum mechanics of spatially constant SU(2) Yang–Mills- and Dirac-fields minimally cou...
We propose a mean-field approach to the Duffing oscillator to construct perturbatively the bounded o...
The free energy in the weak-coupling phase of two-dimensional Yang-Mills theory on a sphere for SO(N...
We discuss the precise relation of the open N=2 string to a self-dual Yang-Mills (SDYM) system in 2+...
Coulomb gauge Yang-Mills theory is considered within the first order formalism. It is shown that the...
The idea of a spin-charge separation of the SU(2) gauge potential is extended to the SU(3) case. It ...
Using the technique of finite field dependent BRST transformations we show that the classical massiv...
We investigate the topological properties of the SU(3) pure gauge theory by performing numerical sim...
Supersymmetric Yang-Mills theory is formulated in six dimensions, without the use of anti-commuting ...