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Spinning Strings and Integrable Spin Chains in the AdS/CFT Correspondence Jan Plefka
Spinning Strings and Integrable Spin Chains in the AdS/CFT Correspondence Jan Plefka

... are therefore derived, non-fundamental objects, just as the theory of gravity itself. Ironically though, advances in our understanding of non-perturbative string theory and of D-branes have led to a resurrection of gauge fields as fundamental objects. Namely, it is now generally believed that string ...
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Particle Physics Part III Major Option 2008
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...  Empirically, the strong force is short range and therefore know that the physical gluons are confined. The colour singlet state does not exist in nature ! NOTE: this is not entirely ad hoc. In the context of gauge field theory (see minor option) the strong interaction arises from a fundamental SU( ...
A unification of photons, electrons, and gravitons under qbit
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Lattice QCD

...  Boundary condition is imposed on each field in finite volume: Momentum space is restricted in finite Brillouin zone: Lattice QCD is an Ultra-Violet (UV) finite theory Lattice action is not unique, above action is the simplest one! Many implementations were proposed to reduce the discretization err ...
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... description of the strong interactions is by a gauge theory, called quantumchromodynamics, or QCD for short. Quarks and gluons can be arranged as multiplets of the gauge group of QCD, which is SU(3). The associated charges are called color, and there are three quark colors and three anti-quark color ...
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Gauge fixing



In the physics of gauge theories, gauge fixing (also called choosing a gauge) denotes a mathematical procedure for coping with redundant degrees of freedom in field variables. By definition, a gauge theory represents each physically distinct configuration of the system as an equivalence class of detailed local field configurations. Any two detailed configurations in the same equivalence class are related by a gauge transformation, equivalent to a shear along unphysical axes in configuration space. Most of the quantitative physical predictions of a gauge theory can only be obtained under a coherent prescription for suppressing or ignoring these unphysical degrees of freedom.Although the unphysical axes in the space of detailed configurations are a fundamental property of the physical model, there is no special set of directions ""perpendicular"" to them. Hence there is an enormous amount of freedom involved in taking a ""cross section"" representing each physical configuration by a particular detailed configuration (or even a weighted distribution of them). Judicious gauge fixing can simplify calculations immensely, but becomes progressively harder as the physical model becomes more realistic; its application to quantum field theory is fraught with complications related to renormalization, especially when the computation is continued to higher orders. Historically, the search for logically consistent and computationally tractable gauge fixing procedures, and efforts to demonstrate their equivalence in the face of a bewildering variety of technical difficulties, has been a major driver of mathematical physics from the late nineteenth century to the present.
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