Abstract
A few basic facts concerning the geometry of classical gauge fields are summarized; in particular, it is asserted that a principal bundle with connection can be characterized uniquely by its “Wilson loops”. The quantization of gauge fields is then shown to consist of converting the Wilson loops into “random fields” on a manifold of oriented loops, a problem in “random geometry”. Other examples in random geometry are briefly sketched. A general theorem permitting to reconstruct quantized Wilson loops from a sequence of Schwinger functionals is stated, the quark-antiquark potential is introduced, and “disorder fields” are discussed in general terms. The status of the construction of quantized gauge fields in the continuum limit is indicated, and some random-geometrical arguments are applied to lattice gauge theories and used to derive estimates on the expectation of the Wilson loop, resp. the disorder field.
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Fröhlich, J. (1980). Some Results and Comments on Quantized Gauge Fields. In: Hooft, G., et al. Recent Developments in Gauge Theories. NATO Advanced Study Institutes Series, vol 59. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-7571-5_5
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DOI: https://doi.org/10.1007/978-1-4684-7571-5_5
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