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Volumn 55, Issue 1, 1997, Pages 161-166

Neutral current interference in the TeV region: The experimental sensitivity at the CERN LHC

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0006157515     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.55.161     Document Type: Article
Times cited : (66)

References (25)
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    • Discussions and further references on the use of forward-backward fermion asymmetries in high energy (Formula presented) collisions can be found in G. Barbiellini et al., in Physics at LEP, LEP Jamboree, Geneva, Switzerland, 1985, edited by J. Ellis and R. Peccei (CERN Report No. 86-02, Geneva, 1986), Vol. II, pp. 46–54; A. Blondel et al., in Proceedings of the ECFA Workshop on LEP 200, Aachen, West Germany, 1986, edited by A. Bohm and W. Hoogland (CERN Report No. 87-08, and ECFA 87/108 Geneva, Switzerland, 1987), Vol. II, pp. 414-452; and V. Angelopoulos et al., in Proceedings of the Workshop on Physics at Future Accelerators, La Thuile, Italy, 1987, edited by J. H. Mulvey (CERN Report No. 87-07, Geneva, Switzerland, 1987), Vol. I, pp. 80–122
    • Discussions and further references on the use of forward-backward fermion asymmetries in high energy (Formula presented) collisions can be found in G. Barbiellini et al., in Physics at LEP, LEP Jamboree, Geneva, Switzerland, 1985, edited by J. Ellis and R. Peccei (CERN Report No. 86-02, Geneva, 1986), Vol. II, pp. 46–54; A. Blondel et al., in Proceedings of the ECFA Workshop on LEP 200, Aachen, West Germany, 1986, edited by A. Bohm and W. Hoogland (CERN Report No. 87-08, and ECFA 87/108 Geneva, Switzerland, 1987), Vol. II, pp. 414-452; and V. Angelopoulos et al., in Proceedings of the Workshop on Physics at Future Accelerators, La Thuile, Italy, 1987, edited by J. H. Mulvey (CERN Report No. 87-07, Geneva, Switzerland, 1987), Vol. I, pp. 80–122.
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    • The PYTHIA subprocesses 1 and 165 are used to simulate dilepton events according to the formalism given in 11
    • The PYTHIA subprocesses 1 and 165 are used to simulate dilepton events according to the formalism given in 11.
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    • The PYTHIA subprocesses 141 is used to simulate (Formula presented) production according to the formalism given in
    • The PYTHIA subprocesses 141 is used to simulate (Formula presented) production according to the formalism given in;
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    • The CTEQ2 and the Eichten-Hinchliffe-Lane-Quigg (EHLQ) structure functions (mainly CTEQ2L, the PYTHIA 5.7 default) have been used for the simulation
    • The CTEQ2 and the Eichten-Hinchliffe-Lane-Quigg (EHLQ) structure functions (mainly CTEQ2L, the PYTHIA 5.7 default) have been used for the simulation.
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    • For a recent review of asymmetries and (Formula presented) Models see, for example, 12
    • For a recent review of asymmetries and (Formula presented) Models see, for example, 12 and further references therein.


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