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Chiral Loops and Ghost States in the Quenched Scalar Propagator
High Energy Physics - Lattice · Submitted 13 Jun 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that this is a quenched chiral loop effect associated with the anomalous structure of the $\eta '$ propagator in quenched QCD.
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The abstract, sentence by sentence
The scalar, isovector meson propagator is analyzed in quenched QCD, using the MQA pole-shifting ansatz to study the chiral limit. In addition to the expected short-range exponential falloff characteristic of a heavy scalar meson, the propagator also exhibits a longer-range, negative metric contribution which becomes pronounced for smaller quark masses. We show that this is a quenched chiral loop effect associated with the anomalous structure of the $\eta '$ propagator in quenched QCD. Both the time dependence and the quark mass dependence of this effect are well-described by a chiral loop diagram corresponding to an $\eta '- \pi$ intermediate state, which is light and effectively of negative norm in the quenched approximation. The relevant parameters of the effective Lagrangian describing the scalar sector of the quenched theory are determined.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The scalar, isovector meson propagator is analyzed in quenched QCD, using the MQA pole-shifting ansatz to study the chiral limit. | contribution 0.74 | 0.85 | 0.05 | asserted 0.95 |
| s1 | In addition to the expected short-range exponential falloff characteristic of a heavy scalar meson, the propagator also exhibits a longer-range, negative metric contribution which becomes pronounced for smaller quark masses. | result 1.00 | 0.81 | 0.31 | asserted 1.00 |
| s2 | We show that this is a quenched chiral loop effect associated with the anomalous structure of the $\eta '$ propagator in quenched QCD. | interpretation 0.97 | 0.84 | 0.62 | asserted 1.00 |
| s3 | Both the time dependence and the quark mass dependence of this effect are well-described by a chiral loop diagram corresponding to an $\eta '- \pi$ intermediate state, which is light and effectively of negative norm in the quenched approximation. | result 0.60 | 0.84 | 0.39 | asserted 0.99 |
| s4 | The relevant parameters of the effective Lagrangian describing the scalar sector of the quenched theory are determined. | contribution 0.51 | 0.88 | 0.05 | asserted 0.96 |
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The paper
Original abstract
The scalar, isovector meson propagator is analyzed in quenched QCD, using the MQA pole-shifting ansatz to study the chiral limit. In addition to the expected short-range exponential falloff characteristic of a heavy scalar meson, the propagator also exhibits a longer-range, negative metric contribution which becomes pronounced for smaller quark masses. We show that this is a quenched chiral loop effect associated with the anomalous structure of the $\eta '$ propagator in quenched QCD. Both the time dependence and the quark mass dependence of this effect are well-described by a chiral loop diagram corresponding to an $\eta '- \pi$ intermediate state, which is light and effectively of negative norm in the quenched approximation. The relevant parameters of the effective Lagrangian describing the scalar sector of the quenched theory are determined.
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References
How the literature uses it
6 arXiv papers cite this in 9 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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For the lightest quark masses used, this propagator is dominated by a quenched chiral loop effect associated with the $\eta'$-$\pi$ two-meson intermediate state.
Chiral Loop Effects in the Quenched Scalar Isovector Propagator · 0.90
Papers citing it · 8 sentences without a confident label
Cites it as background 1 paper
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This is best known in the situation of scalar mesons, where there is a long history of observations going back to the quenched studies of Ref. [ref] .
Diquark effects in light baryon correlators from lattice QCD · Lattice action and simulation details · 0.89
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