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n-Particle irreducible effective action techniques for gauge theories
High Energy Physics - Phenomenology · Submitted 23 Jan 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We point out an equivalence hierarchy for nPI effective actions, which allows one to obtain a self-consistently complete result in practice.
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The abstract, sentence by sentence
A loop or coupling expansion of a so-called n-particle irreducible (nPI) generating functional provides a well-defined approximation scheme in terms of self-consistently dressed propagators and n-point vertices. A self-consistently complete description determines the functional for arbitrarily high n to a given order in the expansion. We point out an equivalence hierarchy for nPI effective actions, which allows one to obtain a self-consistently complete result in practice. The method is applied to a SU(N) gauge theory with fermions up to four-loop or O(g^6) corrections. For non-equilibrium we discuss the connection to kinetic theory. The leading-order on-shell results in g can be obtained from the three-loop effective action approximation, which already includes in particular all diagrams enhanced by the Landau Pomeranchuk Migdal effect. Furthermore, we compare the effective action approach with Schwinger-Dyson (SD) equations. By construction, SD equations are expressed in terms of loop diagrams including both classical and dressed vertices, which leads to ambiguities of whether classical or dressed ones should be employed at a given truncation order. We point out that these problems are absent using effective action techniques. We show that a wide class of truncations of SD equations cannot be obtained from the nPI effective action. In turn, our results can be used to resolve SD ambiguities of whether classical or dressed vertices should be employed at a given truncation order.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A loop or coupling expansion of a so-called n-particle irreducible (nPI) generating functional provides a well-defined approximation scheme in terms of self-consistently dressed propagators and n-point vertices. | background 0.95 | 0.14 | 0.11 | asserted 1.00 |
| s1 | A self-consistently complete description determines the functional for arbitrarily high n to a given order in the expansion. | background 0.61 | 0.28 | 0.13 | asserted 1.00 |
| s2 | We point out an equivalence hierarchy for nPI effective actions, which allows one to obtain a self-consistently complete result in practice. | contribution 0.94 | 0.88 | 0.37 | asserted 0.98 |
| s3 | The method is applied to a SU(N) gauge theory with fermions up to four-loop or O(g^6) corrections. | contribution 0.65 | 0.92 | 0.09 | asserted 1.00 |
| s4 | For non-equilibrium we discuss the connection to kinetic theory. | contribution 0.93 | 0.71 | 0.04 | asserted 0.67 |
| s5 | The leading-order on-shell results in g can be obtained from the three-loop effective action approximation, which already includes in particular all diagrams enhanced by the Landau Pomeranchuk Migdal effect. | result 0.98 | 0.80 | 0.14 | asserted 0.95 |
| s6 | Furthermore, we compare the effective action approach with Schwinger-Dyson (SD) equations. | contribution 0.87 | 0.82 | 0.06 | asserted 0.87 |
| s7 | By construction, SD equations are expressed in terms of loop diagrams including both classical and dressed vertices, which leads to ambiguities of whether classical or dressed ones should be employed at a given truncation order. | background 0.89 | 0.20 | 0.06 | asserted 1.00 |
| s8 | We point out that these problems are absent using effective action techniques. | result 0.77 | 0.82 | 0.17 | asserted 1.00 |
| s9 | We show that a wide class of truncations of SD equations cannot be obtained from the nPI effective action. | result 0.96 | 0.93 | 0.19 | asserted 1.00 |
| s10 | In turn, our results can be used to resolve SD ambiguities of whether classical or dressed vertices should be employed at a given truncation order. | interpretation 0.57 | 0.90 | 0.23 | asserted 0.96 |
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The paper
Original abstract
A loop or coupling expansion of a so-called n-particle irreducible (nPI) generating functional provides a well-defined approximation scheme in terms of self-consistently dressed propagators and n-point vertices. A self-consistently complete description determines the functional for arbitrarily high n to a given order in the expansion. We point out an equivalence hierarchy for nPI effective actions, which allows one to obtain a self-consistently complete result in practice. The method is applied to a SU(N) gauge theory with fermions up to four-loop or O(g^6) corrections. For non-equilibrium we discuss the connection to kinetic theory. The leading-order on-shell results in g can be obtained from the three-loop effective action approximation, which already includes in particular all diagrams enhanced by the Landau Pomeranchuk Migdal effect. Furthermore, we compare the effective action approach with Schwinger-Dyson (SD) equations. By construction, SD equations are expressed in terms of loop diagrams including both classical and dressed vertices, which leads to ambiguities of whether classical or dressed ones should be employed at a given truncation order. We point out that these problems are absent using effective action techniques. We show that a wide class of truncations of SD equations cannot be obtained from the nPI effective action. In turn, our results can be used to resolve SD ambiguities of whether classical or dressed vertices should be employed at a given truncation order.
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References
How later papers used it
51 later papers cite it
3 later papers by other authors are listed below: 2 used its method or tool and 1 compared its own results with it.
Uses its method or tool 2 of 15 papers with this label
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Derived its system of equations from the 3PI effective action truncated at three loops as in this paper.
Gluonic vertices and the gluon propagator in Landau gauge Yang-Mills theory (2019) · 0.92 · paraphrased: the licence does not allow quoting
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Followed this paper's method to derive the 4PI effective action for a scalar theory with cubic and quartic interactions and a non-vanishing field expectation value.
Next-to-Leading Order Transport Coefficients from the Four-Particle Irreducible Effective Action (2009) · 1.00 · paraphrased: the licence does not allow quoting
Compares with it 1 paper
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Said its truncation is similar to the one from a 3-loop expansion of a 3PI action analyzed in this paper, but differs in that the DSEs have one bare vertex in every graph.
Infrared singularities in Landau gauge Yang-Mills theory (2008) · 0.99 · paraphrased: the licence does not allow quoting
How the literature uses it
38 arXiv papers cite this in 80 sentences
Papers citing it · 58 sentences without a confident label
Uses its method or tool 10 papers
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We perform a semi-perturbative calculation of the quark-gluon vertex inspired from its equation of motion of the three-loop expanded 3PI effective action [ref] .
On the quark-gluon vertex at non-vanishing temperature · Setup · 0.93
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We use the Bethe-Salpeter equation (BSE) for a two-gluon bound state as derived from the 3PI effective action truncated to three loops [ref] as described in [ref] .
Quenched glueballs in the DSE/BSE framework · Methodology · 1.00
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We use the method of successive Legendre transformations [ref] and obtain the 4PI effective action to 4-loop order.
Next-to-Leading Order Transport Coefficients from the Four-Particle Irreducible Effective Action · the 4PI Effective Action · 0.99
Compares with it 1 paper
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The truncation we study here is also similar to the one obtained from a 3-loop expansion of a 3PI action analyzed in [ref] but with the difference that in the DSEs there is one bare vertex in every graph.
Infrared singularities in Landau gauge Yang-Mills theory · Inclusion of soft singularities and masses · 0.99
Cites it as background 9 papers
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These vacuum diagrams are part of a generating functional known as the 2PI effective action (cf. [ref]) [ref] .
Dark matter freeze-in from non-equilibrium QFT: towards a consistent treatment of thermal effects · Fundamentals of the CTP formalism · 0.91
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The $n$PI effective action formalism [ref] is another approach in which the action is expressed as a functional of non-perturbative vertex functions which are determined through a self-consistent stationary equation after the effective action is expanded to some order in the loop or $1/N$ expansion.
4-point vertices from the 2PI and 4PI Effective Actions · Introduction · 0.95
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For more details beyond the short overview presented here, see, e.g., [ref] .
Correlation functions of Landau gauge Yang-Mills theory · Equations of motion · 1.00
Discussion
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