Are the reactions γγ→VV′ a challenge for the factorized Pomeron at high energies?

Physical Review D - Particles, Fields, Gravitation and Cosmology

Volumn 60, Issue 11, 1999, Pages 1-2

  Achasov, N N ^a   Shestakov, G N ^a  

^a SOBOLEV INSTITUTE OF MATHEMATICS   (Russian Federation)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 18044386841     PISSN: 05562821     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevD.60.117503     Document Type: Article

References (17)

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2. R. Engel and J. Ranft, Phys. Rev. D 54, 4244 (1996).
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5. S. Söldner-Rembold, presented at ICHEP'98, Vancouver, Canada, 1998; hep-ex/9810011, 1998.
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8. - Collisions from φ to J/ψ, Novosibirsk, Russia, 1999.
9. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
10. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
11. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
12. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
13. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
14. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
15. - production cross sections requires the presence of a flavor exotic isotensor tensor state near the nominal ρρ threshold [N. N. Achasov, S. A. Devyanin, and G. N. Shestakov, Phys. Lett. 108B, 134 (1982); Z. Phys. C 16, 55 (1982); 27, 99 (1985); N. N. Achasov and G. N. Shestakoy, Usp. Fiz. Nauk 161, 53 (1991) [Sov. Phys. Usp. 34, 471 (1991)]; H. Albrecht et al., Phys. Rep. 276, 223 (1996); Particle Data Group, R. M. Barnett et al., Phys. Rev. D 54, 1 (1996), pp. 46, 369, 558]. An analysis of this phenomena in connection with the L3 data will be presented elsewhere.
16. H. Albrecht et al., Z. Phys. G 50, 1 (1991).
17. H. Albrecht et al., Phys. Lett B 267, 535 (1991).