Fine structure of the diffraction cone: From the ISR to the LHC

Author:

Fagundes D. A.1,Jenkovszky L.2,Miranda E. Q.3,Pancheri G.4,Silva P. V. R. G.5

Affiliation:

1. Universidade Federal de Santa Catarina – Campus Blumenau, Rua Pomerode, 710 Salto do Norte, 89065-300 Blumenau, SC, Brazil

2. Bogolyubov Institute for Theoretical Physics, National Academy of Sciences of Ukraine, UA-03680 Kiev, Ukraine

3. InSTEC, Quinta de los Marinos, Ave. Salvador Allende y Lucas, La Habana 10400 Cuba

4. INFN Frascati National Laboratories, Via E. Fermi 40, 00444, Italy

5. Instituto de Física Gleb Wataghin, Universidade Estadual de Campinas, 13083-859, Campinas, SP, Brazil

Abstract

Following earlier findings, we argue that the low-[Formula: see text] structure in the elastic diffractive cone, recently reported by the TOTEM Collaboration at [Formula: see text] TeV, is a consequence of the threshold singularity required by [Formula: see text]channel unitarity, such as revealed earlier at the ISR. By using simple Regge-pole models, we analyze the available data on the [Formula: see text] elastic differential cross section in a wide range of c.m. energies, namely those from ISR to LHC8, obtaining good fits of all datasets. This study hints at the fact that the non-exponential behavior observed at LHC8 is a recurrence of the low-[Formula: see text] “break” phenomenon, observed in the seventies at ISR, being induced by the presence of a two-pion loop singularity in the Pomeron trajectory.

Publisher

World Scientific Pub Co Pte Lt

Subject

Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics

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