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This graduate-level book is a coherent and self-contained introduction to quantum field theory (QFT), with a distinctive focus on geometric and nonperturbative aspects. The opening part covers quantum fields and the Euclidean path integral, Yang–Mills field theories, and Wilsonian renormalization. Wilson's notion of the effective field theory and its heavy implication for the QFT framework itself are given particular attention. Next, geometric and topological aspects are thoroughly treated, accompanied by a healthy dose of underlying mathematics. Anomalies—quantum failures of classical symmetries—follow as crucial litmus tests for self-consistency, which are delineated in unprecedented detail, spanning decades of development. In the final part, the book asks how relativistic gravity, known to resist standard quantization schemes, may be reconciled with the quantum world. This question is approached by invoking the d = 2 Weyl anomaly, Hawking effects, black hole partition functions, and the renormalization of fundamental strings, with a view toward superstring theory.
We explore several foundational facts about quantum field theories, starting with the well-known conversion of Schrödinger mechanics to a path integral formulation. Path integral accommodates the natural time-ordering of the operator formulation without any tweak, which leads to how the causal Green’s function replaces its classical counterpart and motivates the Wick rotation of the path integral into Euclidean time, setting the stage for the rest of the volume. Along the way, we pay some attention to the real-space version of various Green’s functions. After a brief exploration of fermionic mechanics and the following spinor fields, we turn to the symmetries and the conservation laws. Although we initially follow the standard treatise of the material, with emphasis on the role of gauging either as part of the dynamics or as an auxiliary handle, we point out how a common confusion over Noether’s energy-momentum tensor stems from an ill-conceived implementation of translations. When properly equipped with the Lie derivative, we show how the Noether procedure always reproduces the symmetric energy-momentum tensor from the metric variation and obviates the "improvement" terms.
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