2004
DOI: 10.1103/physrevd.70.094037
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Spectral density in the resonance region and analytic confinement

Abstract: We study the role of finite widths of resonances in a nonlocal version of the Wick-Cutkosky model. The spectrum of bound states is known analytically in this model and forms linear Regge tragectories. We compute the widths of resonances, calculate the spectral density in an extension of the Breit-Wigner ansatz and discuss a mechanism for the damping of unphysical exponential growth of observables at high energy due to finite widths of resonances.

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Cited by 8 publications
(11 citation statements)
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“…Note also that such a mean width is essentially different from both the linear mass dependence of string models [36] and from an exponential form of the nonlocal field theoretical models [37]. Nevertheless, as we demonstrate …”
Section: Analysis Of the Fwm Spectrummentioning
confidence: 74%
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“…Note also that such a mean width is essentially different from both the linear mass dependence of string models [36] and from an exponential form of the nonlocal field theoretical models [37]. Nevertheless, as we demonstrate …”
Section: Analysis Of the Fwm Spectrummentioning
confidence: 74%
“…IV one can find the mean mass (37) for T ≥ c ± T H (or for m ≥ 0 ) to be equal to the most probable mass of bag from which one determines the resonance width:…”
Section: Asymptotic Behavior Of the Regge Trajectoriesmentioning
confidence: 99%
“…Calculated in terms of the same underlying quantum field theory, these also exhibit exponential growth in energy. This guar- antees that the spectral density is well-behaved over the region for which the Breit-Wigner ansatz is valid, as discussed in [5].…”
Section: Dynamical Confinement and Spectral Densitymentioning
confidence: 81%
“…This was calculated in [5] using several variations of the Breit-Wigner ansatz. The most obvious choice is where the decay-widths implicit in the ansatz are for on-shell bound states.…”
Section: Dynamical Confinement and Spectral Densitymentioning
confidence: 99%
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