nLab worldline formalism

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Contents

Idea

In contrast, in what is called the worldline formalism of perturbative quantum field theory this assignment is obtained instead more conceptually as the correlators/n-point functions of a 1-dimensional QFT that lives on the Feynman graphs, namely the worldline theory (usually a sigma-model into the given target spacetime), which may be thought of as being the (relativistic) quantum mechanics of the particles that are the quanta of the fields in the field theory.

One may think of this as realizing the intuition that the edges in a Feynman diagram correspond to worldlines of virtual particles.

Mathematically, the key step here is a Mellin transform – introducing a “Schwinger parameter” – which realizes the Feynman propagator $\Delta_F(x,y)$ as a path integral for a relativistic particle travelling from $y$ to $x$ .

This worldline formalism is equivalent to the traditional formulation. It has the conceptual advantage that it expresses the Feynman perturbation series of perturbative quantum field theory manifestly as a second quantization of its particle content given explicitly as the superposition of all 1-particle processes, and the calculational advantage of automatically summing over subsets of Feynman diagrams related by exchange of external legs, thus maintaining permutation symmetry and explicit gauge invariance of on-shell scattering amplitudes.

The worldline formulation of QFT has an evident generalization to higher dimensional worldvolumes: in direct analogy one can consider summing the correlators/n-point functions over worldvolume theories of “higher dimensional particles” (“branes”) over all possible worldvolume geometries. Indeed, for 2-dimensional branes this is precisely the way in which perturbative string theory is defined: the string scattering amplitudes are given by the analogous “worldsheet formalism” known as the string perturbation series as the sum over all surfaces of the correlators/n-point functions of of a 2d SCFT of central charge 15.

worldvolume field theory	of fundamental branes	and their second quantization	which in perturbation theory is given by
worldline formalism	particle	quantum field theory	scattering amplitudes
2d CFT correlators	string	string field theory	string scattering amplitudes

Indeed, after decades of Feynman rules, the worldline formalism for QFT was found only via string theory in (Bern-Kosower 91), by looking at the point particle limit of string scattering amplitudes.

graphics grabbed from Jurke 10

graphics grabbed from Schubert 96

Then (Strassler 92, Strassler 93) observed that generally the worldline formalism is obtained from the correlators of the 1d QFT of relativistic particles on their worldline.

graphics grabbed from (Schmidt-Schubert 94)

The first calculation along these lines was actually done earlier in (Metsaev-Tseytlin 88) where the 1-loop beta function for pure Yang-Mills theory was obtained as the point-particle limit of the partition function of a bosonic open string in a Yang-Mills background field. This provided a theoretical explanation for the observation, made earlier in (Nepomechie 83) that when computed via dimensional regularization then this beta function coefficient of Yang-Mills theory vanishes in spacetime dimension 26. This of course is the critical dimension of the bosonic string.

Precursor observations include

Richard Feynman, Appendix of Mathematical formulation of the quantum theory of electromagnetic interaction, Physics Review Volume 80 (1950) 440.
R.I. Nepomechie, Remarks on quantized Yang-Mills theory in 26 dimensions, Physics Letters B Volume 128, Issues 3–4, 25 August 1983, Pages 177-178 Phys. Lett. B128 (1983) 177 (doi:10.1016/0370-2693(83)90385-4)
Ruslan Metsaev, Arkady Tseytlin, On loop corrections to string theory effective actions, Nuclear Physics B Volume 298, Issue 1, 29 February 1988, Pages 109-132 (doi:10.1016/0550-3213(88)90306-9)

The worldline formalism as such was first derived from the point-particle limit of string scattering amplitudes in

Zvi Bern, D. Kosower, Efficient calculation of one-loop QCD amplitudes Phys. Rev. D 66 (1991),(journal)
Zvi Bern, D. Kosower, The computation of loop amplitudes in gauge theories, Nucl. Phys. B379 (1992) (journal)

Then it was related to actual worldline quantum field theory in

Matthew Strassler, Field Theory Without Feynman Diagrams: One-Loop Effective Actions, Nucl. Phys. B385:145-184,1992 (arXiv:hep-ph/9205205)
Matthew Strassler, The Bern-Kosower Rules and Their Relation to Quantum Field Theory, PhD thesis, Stanford 1993 (spires)

Review:

M. G. Schmidt, Christian Schubert, The Worldline Path Integral Approach to Feynman Graphs (arXiv:hep-ph/9412358)
Christian Schubert, An Introduction to the Worldline Technique for Quantum Field Theory Calculations, Acta Phys. Polon.B27:3965-4001, 1996 (arXiv:hep-th/9610108)
Christian Schubert, Perturbative Quantum Field Theory in the String-Inspired Formalism, Phys.Rept. 355 (2001) 73-234 (arXiv:hep-th/0101036)
Olindo Corradini, Christian Schubert, James P. Edwards, Naser Ahmadiniaz, Spinning Particles in Quantum Mechanics and Quantum Field Theory (arXiv:1512.08694)

(with emphasis on spinning particles)
James P. Edwards, C. Moctezuma Mata, U. Müller, Christian Schubert, New techniques for worldline integration, SIGMA 17 (2021), 065, 19 pages (arXiv:2106.12071)
James P. Edwards, Christian Schubert, Quantum mechanical path integrals in the first quantised approach to quantum field theory, (arXiv:1912.10004)

Exposition with an eye towards quantum gravity:

Edward Witten, from 30:40 on in Quantum Gravity, Solomon Lefschetz Memorial Lecture Series, November 2011 (video)
Edward Witten, What every physicist should know about string theory, talk at Strings2015 (pdf, pdf, video recording)