We present results for the production of a Z boson in association with single top at next-to-leading order (NLO), including the decay of the top quark and the Z boson. This electroweak process gives rise to the trilepton signature l+l-l′±+jets+missing energy. We present results for this signature and show that the rate is competitive with the contribution of the mixed strong and electroweak production process, tt̄Z. As such it should be observable in the full data sample from LHC running at √s=8 TeV. The single top+Z process is a hitherto unconsidered irreducible background in searches for flavor changing neutral current decays of the top quark in tt̄ production. For a selection of cuts used at the LHC involving a b-tag it is the dominant background. In the Appendices we also briefly discuss the impact of NLO corrections on the related tH process. © 2013 American Physical Society.

Single top production in association with a Z boson at the LHC / J. Campbell, R.K. Ellis, R. Röntsch. - In: PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY. - ISSN 1550-7998. - 87:11(2013 Jun 05), pp. 114006.114006-1-114006.114006-12. [10.1103/PhysRevD.87.114006]

Single top production in association with a Z boson at the LHC

R. Röntsch
Ultimo
2013

Abstract

We present results for the production of a Z boson in association with single top at next-to-leading order (NLO), including the decay of the top quark and the Z boson. This electroweak process gives rise to the trilepton signature l+l-l′±+jets+missing energy. We present results for this signature and show that the rate is competitive with the contribution of the mixed strong and electroweak production process, tt̄Z. As such it should be observable in the full data sample from LHC running at √s=8 TeV. The single top+Z process is a hitherto unconsidered irreducible background in searches for flavor changing neutral current decays of the top quark in tt̄ production. For a selection of cuts used at the LHC involving a b-tag it is the dominant background. In the Appendices we also briefly discuss the impact of NLO corrections on the related tH process. © 2013 American Physical Society.
Settore FIS/02 - Fisica Teorica, Modelli e Metodi Matematici
5-giu-2013
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2434/904367
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