The first three pomerons

V. A. Petrov; A. V. Prokudin

doi:10.1007/s100520100838

The first three pomerons

V. A. Petrov, A. V. Prokudin

Division of Science (Berks)

Research output: Contribution to journal › Article › peer-review

48 Scopus citations

Abstract

A model of a three pomeron contribution to high energy elastic pp and p̄p scattering is proposed. The data are well described for all momenta (0.01 ≤ |t| ≤ 14. GeV²) and energies (8. ≤ s^1/2 ≤ 1800. GeV) (Χ²/d.o.f. = 2.60). The model predicts the appearance of two dips in the differential cross-section which will be measured at LHC. The parameters of the pomeron trajectories are α(0)_P1 = 1.058, α′(0)_P1 = 0.560 GeV^-2; α(0) _P2 = 1.167, α′(0)_P2 = 0.273 GeV^-2; α(0)_P3 = 1.203, α′(0)_P3 = 0.094 GeV ^-2.

Original language	English (US)
Pages (from-to)	135-143
Number of pages	9
Journal	European Physical Journal C
Volume	23
Issue number	1
DOIs	https://doi.org/10.1007/s100520100838
State	Published - Mar 2002

All Science Journal Classification (ASJC) codes

Engineering (miscellaneous)
Physics and Astronomy (miscellaneous)

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title = "The first three pomerons",

abstract = "A model of a three pomeron contribution to high energy elastic pp and {\=p}p scattering is proposed. The data are well described for all momenta (0.01 ≤ |t| ≤ 14. GeV2) and energies (8. ≤ s1/2 ≤ 1800. GeV) (Χ2/d.o.f. = 2.60). The model predicts the appearance of two dips in the differential cross-section which will be measured at LHC. The parameters of the pomeron trajectories are α(0)P1 = 1.058, α′(0)P1 = 0.560 GeV-2; α(0) P2 = 1.167, α′(0)P2 = 0.273 GeV-2; α(0)P3 = 1.203, α′(0)P3 = 0.094 GeV -2.",

author = "Petrov, {V. A.} and Prokudin, {A. V.}",

year = "2002",

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doi = "10.1007/s100520100838",

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pages = "135--143",

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T1 - The first three pomerons

AU - Petrov, V. A.

AU - Prokudin, A. V.

PY - 2002/3

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N2 - A model of a three pomeron contribution to high energy elastic pp and p̄p scattering is proposed. The data are well described for all momenta (0.01 ≤ |t| ≤ 14. GeV2) and energies (8. ≤ s1/2 ≤ 1800. GeV) (Χ2/d.o.f. = 2.60). The model predicts the appearance of two dips in the differential cross-section which will be measured at LHC. The parameters of the pomeron trajectories are α(0)P1 = 1.058, α′(0)P1 = 0.560 GeV-2; α(0) P2 = 1.167, α′(0)P2 = 0.273 GeV-2; α(0)P3 = 1.203, α′(0)P3 = 0.094 GeV -2.

AB - A model of a three pomeron contribution to high energy elastic pp and p̄p scattering is proposed. The data are well described for all momenta (0.01 ≤ |t| ≤ 14. GeV2) and energies (8. ≤ s1/2 ≤ 1800. GeV) (Χ2/d.o.f. = 2.60). The model predicts the appearance of two dips in the differential cross-section which will be measured at LHC. The parameters of the pomeron trajectories are α(0)P1 = 1.058, α′(0)P1 = 0.560 GeV-2; α(0) P2 = 1.167, α′(0)P2 = 0.273 GeV-2; α(0)P3 = 1.203, α′(0)P3 = 0.094 GeV -2.

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The first three pomerons

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