Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay

In view of the proliferation in the number of new charmonium states, it is really important to have an experimental way to prove that an observed bump is, indeed, a real resonance. To do that, in this paper we present an alternative method to demonstrate the resonant behavior of a state. With this m...

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Main Authors: Ignacio Bediaga, Jussara M. de Miranda, Fernando Rodrigues, Marina Nielsen
Format: Article
Language:English
Published: Elsevier 2015-09-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269315005109
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spelling doaj-f231713d47294cee958acb58cd9838272020-11-25T01:50:49ZengElsevierPhysics Letters B0370-26931873-24452015-09-01748C18719010.1016/j.physletb.2015.06.079Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decayIgnacio Bediaga0Jussara M. de Miranda1Fernando Rodrigues2Marina Nielsen3Centro Brasileiro de Pesquisas Físicas, Rua Xavier Sigaud 150, 22290-180 Rio de Janeiro, RJ, BrazilCentro Brasileiro de Pesquisas Físicas, Rua Xavier Sigaud 150, 22290-180 Rio de Janeiro, RJ, BrazilCentro Brasileiro de Pesquisas Físicas, Rua Xavier Sigaud 150, 22290-180 Rio de Janeiro, RJ, BrazilInstituto de Física, Universidade de São Paulo, C.P. 66318, 05314-970 São Paulo, SP, BrazilIn view of the proliferation in the number of new charmonium states, it is really important to have an experimental way to prove that an observed bump is, indeed, a real resonance. To do that, in this paper we present an alternative method to demonstrate the resonant behavior of a state. With this method, the phase variation of a generic complex amplitude can be directly revealed through interference in the Dalitz-plot region where it crosses a well established resonant state, used as a probe. We have tested the method for the Z−(4430) state by generating Monte Carlo samples for the B0→ψ(2S)π−K+ decay channel. We have shown that the proposed method gives a clear oscillation behavior, related to the phase variation associated with a real resonant state, in the case where the Z−(4430) is considered as a regular resonance with a strong phase variation.http://www.sciencedirect.com/science/article/pii/S0370269315005109
collection DOAJ
language English
format Article
sources DOAJ
author Ignacio Bediaga
Jussara M. de Miranda
Fernando Rodrigues
Marina Nielsen
spellingShingle Ignacio Bediaga
Jussara M. de Miranda
Fernando Rodrigues
Marina Nielsen
Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay
Physics Letters B
author_facet Ignacio Bediaga
Jussara M. de Miranda
Fernando Rodrigues
Marina Nielsen
author_sort Ignacio Bediaga
title Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay
title_short Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay
title_full Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay
title_fullStr Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay
title_full_unstemmed Phase motion in the Z−(4430) amplitude in B0→ψ′π−K+ decay
title_sort phase motion in the z−(4430) amplitude in b0→ψ′π−k+ decay
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2015-09-01
description In view of the proliferation in the number of new charmonium states, it is really important to have an experimental way to prove that an observed bump is, indeed, a real resonance. To do that, in this paper we present an alternative method to demonstrate the resonant behavior of a state. With this method, the phase variation of a generic complex amplitude can be directly revealed through interference in the Dalitz-plot region where it crosses a well established resonant state, used as a probe. We have tested the method for the Z−(4430) state by generating Monte Carlo samples for the B0→ψ(2S)π−K+ decay channel. We have shown that the proposed method gives a clear oscillation behavior, related to the phase variation associated with a real resonant state, in the case where the Z−(4430) is considered as a regular resonance with a strong phase variation.
url http://www.sciencedirect.com/science/article/pii/S0370269315005109
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