On the low energy behavior of Regge poles

2010 ◽  
Vol 51 (10) ◽  
pp. 102104 ◽  
Author(s):  
A. Hiscox ◽  
B. M. Brown ◽  
M. Marletta
Keyword(s):  
Low Energy ◽  
Energy Behavior ◽  
Regge Poles

scholarly journals Low-energy behavior of spin-liquid electron spectral functions

2013 ◽  
Vol 87 (4) ◽  
Author(s):  
Evelyn Tang ◽  
Matthew P. A. Fisher ◽  
Patrick A. Lee
Keyword(s):  
Low Energy ◽  
Spin Liquid ◽  
Spectral Functions ◽  
Energy Behavior

Low-Energy Theorems and High-Energy Behavior

1972 ◽  
Vol 6 (9) ◽  
pp. 2483-2487
Author(s):  
Michael Creutz
Keyword(s):  
High Energy ◽  
Low Energy ◽  
High Energy Behavior ◽  
Energy Behavior

BATSE Observations of Gamma‐Ray Burst Spectra. III. Low‐Energy Behavior of Time‐averaged Spectra

1996 ◽  
Vol 473 (1) ◽  
pp. 310-321 ◽  
Author(s):  
R. D. Preece ◽  
M. S. Briggs ◽  
G. N. Pendleton ◽  
W. S. Paciesas ◽  
J. L. Matteson ◽  
...  
Keyword(s):  
Gamma Ray ◽  
Low Energy ◽  
Gamma Ray Burst ◽  
Energy Behavior

scholarly journals What is duality?

1970 ◽  
Vol 318 (1534) ◽  
pp. 257-278 ◽  
Keyword(s):  
Sum Rules ◽  
Scattering Amplitude ◽  
Finite Energy ◽  
High Energy ◽  
Low Energy ◽  
Strong Interactions ◽  
High Energies ◽  
Resonance Formation ◽  
Interference Models ◽  
Regge Poles

Duality gives a satisfying connexion between two different areas of strong interaction physics, Regge poles at high energy and resonances at low energy. This interlocking gives powerful bootstrap conditions, and together with the assumption that certain channels do not contain resonances it gives strong restrictions on the hadron spectrum. Since there is some confusion about the term duality, we shall explain what is meant by the various forms of duality (f. e. s. r. (finite energy sum rules) duality, local duality), and what is meant by ‘building up’, and we shall show in what way antidual models (such as the generalized interference model) come into conflict with basic empirical facts. Duality expresses the relation between two descriptions of the hadronic scattering amplitude. At low energy (l. e.) the description by direct-channel resonances is simple and useful (see figure 1). At low energy the data show prominent peaks as a function of energy, and one may try the approximation of resonance saturation, i. e. of neglecting the non-resonating background. The second description is the exchange of Regge poles, and it is useful at high energies (h.e.), where typical features are forward peaks, energy dependence s α , and structure at fixed t (see figure 2). The two descriptions are very different; resonance formation corresponds to poles in the s channel, Regge exchange to poles in the t channel. Duality says that there are direct relations between these two descriptions, that they are equivalent in a certain sense. In complete contrast, the interference models postulate that one must add the two descriptions. (If lowest order perturbation theory was relevant to strong interactions, one would be led to adding the diagrams.)

scholarly journals Gauge theory of nonrelativistic fermions and its low-energy behavior

1995 ◽  
Vol 441 (3) ◽  
pp. 483-514 ◽  
Author(s):  
Ikuo Ichinose ◽  
Tetsuo Matsui
Keyword(s):  
Gauge Theory ◽  
Low Energy ◽  
Energy Behavior

Exchange Degeneracy and Duality in a Generalized Interference Model

1972 ◽  
Vol 50 (17) ◽  
pp. 2033-2036
Author(s):  
R. K. Logan
Keyword(s):  
Scattering Amplitude ◽  
Low Energy ◽  
The Other ◽  
Interference Model ◽  
Exchange Degeneracy ◽  
Exotic Mesons ◽  
Energy Scattering ◽  
Strong Exchange ◽  
Regge Poles

We consider a generalized interference model in which the Pomeron and the other Regge poles are built in the sense of a FESR bootstrap from both the resonance and background part of the low energy scattering amplitude. We develop a test of strong exchange degeneracy on the background part of the low energy scattering amplitude through the use of FESR. We show that the restrictions through FESR imposed by exchange degeneracy are weaker than those of duality. Finally, we are able to relate the amount of duality breaking in [Formula: see text] in the absence of exotic mesons to the ratio of NN or πN, P′, and ρ Regge residues.

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