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A study of the vector meson ψ(4040)

M. Piotrowska1,a and F. Giacosa1,2

1Institute of Physics, Jan Kochanowski University, ul. Swietokrzyska 15, 25-406, Kielce, Poland.

2Institute for Theoretical Physics, J. W. Goethe University, Max-von-Laue-Str. 1, 60438 Frankfurt, Germany.

Abstract. We investigate the well-knownc¯cvector stateψ(4040)in the frame- work of a quantum eld theoretical model. In particular, we study its spectral function and search for the pole(s) in the complex plane. Quite interestingly, the spectral function has a non-standard shape and two poles are present. The role of the meson-meson quantum loops (in particularDDones) is crucial and could also explain the not yet conrmed stateY(4008).

1 Introduction

In the past 15 years many new mesonic states have been observed in the charmonium sector.

However, not all of them can be accommodated in the picture of the standard quark model, where mesons are conventional quark-antiquark (qq¯) objects. Some of the newly discovered states, called X, Y and Z, are good candidates for non-conventional mesons such as hybrids, multiquarks, molecules or glueballs, see Refs. [1, 2] and refs. therein.

In these proceedings, based on the forthcoming paper [3], we explore the energy regime close to4GeV, and we concentrate on the vector state ψ(4040)[4]. This resonance is a con- ventionalc¯cstate characterised by the quantum numbersn2S+1LJ= 3 3S1, wheren, S, L, J are the principal number, the spin, the angular momentum and the total spin, respectively.

Moreover, in the charmonium spectrum, at about 4 GeV (very close to ψ(4040)) a puzzling broad enhancement, called Y(4008), was noticed by the Belle Collaboration when studying the cross-section of e+e J/Ψπ+π [5, 6]. However, this state was not conrmed by other groups measuring the same process. Although not yet conrmed, there have been var- ious theoretical speculations (mostly within non-conventional scenarios) trying to explain its nature [2]. In our approach, we checked if it is possible to describe bothψ(4040)andY(4008) simultaneously within a model in which only a single ordinaryc¯cseed state corresponding to ψ(4040)is taken into account. A similar method was used to study the scalar kaon K0(1430), where an additional companion pole describing the lightκemerges [7].

ae-mail: milena.soltysiak@op.pl , 0 (201

EPJ Web of Conferences 199 9) https://doi.org/10.1051/epjconf /201919904013 MESON 2018

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© The Authors, published by EDP Sciences. This is an open access article distributed under the terms of the Creative Commons Attribution License 4.0 (http://creativecommons.org/licenses/by/4.0/).

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2 Theoretical model and results

First, we introduce the following relativistic interaction Lagrangian:

L=igψDDψμ

μD+D

+igψDDψ˜μν

μD∗+νD

+igψDDψμν

D∗+μD∗−ν

+h.c. . (1) Each term describes dierent decays of the state ψ(4040): DD (and also DsDs) in the rst term, DD (and DsDs) in the second term, and DD in the last one. In our model we have ve free parameters: the bare mass Mψ of the state ψ, the three coupling constants gψDD, gψDD and gψDD in Eq. (1) (determined by using some results listed in the PDG [4]), and nally, the cuto Λ. The latter is part of the cuto function (or form factor) FΛ, which assures that our model is nite. We test two types of the form factor, the Gaussian and the dipolar one, see Table 1. Here, for illustration we use Λ = 0.42GeV, for which the pole width is exactly 80 MeV in the Gaussian case. The numerical values of the parameters are presented in the second column of Table 1.

Next, we evaluate the spectral function (alias the mass distribution) of the resonance ψ(4040). In Fig. 1.a we show the results for both types of the cuto function. It is visible that, besides the expected peak close to4.04GeV, an additional enhancement appears close to3.9GeV. In both cases, the shape of the spectral function has not a standard Breit-Wigner form, mainly due to the presence of a deformation left from the peak generated by mesonic quantum loops (most notablyDDones).

a) b)

Figure 1. Panel (a) shows the form of the spectral function of the stateψ(4040) for a Gaussian form factor (blue solid line) and for dipolar one (red dashed line). Panel (b) shows the position of the poles in the complex plane. Blue dots corresponds to the Gaussian form factor, while the red marks to a dipolar one.

Moreover, even if a single seed state is present, we nd that two poles appear in the complex plane, one related to the state ψ(4040) and the second to the enhancement. The results for these poles are shown in Fig. 1.b and in the last two columns of Table 1.

Naively, one is tempted to identify this enhancement and the corresponding pole with the puzzling state Y(4008)and interprete it as a dynamically generated companion pole of ψ(4040). However, a deeper analysis of the reaction e+e ψ(4040)→DD →π+π can explain the formation of the stateY(4008)as aDDloop eect [3], even without invoking the presence of a pole.

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Form factor Parameters Pole forψ(4040) Second pole FΛ=e−2k22 gψDD = 39.6±5.0 (4.053±0.004) (3.934±0.006)

(Gaussian) gψDD= 3.43±0.80GeV−1 −i(0.040±0.010) −i(0.030±0.001) gψDD = 1.90±0.95

Mψ= 4.01GeV

FΛ= (1 +Λk44)−2 gψDD = 21.6±4.4 (4.063±0.023) (3.942±0.004) (Dipolar) gψDD= 3.05±0.49GeV−1 −i(0.057±0.010) −i(0.052±0.010)

gψDD = 2.00±0.91 Mψ= 4.03GeV

Table 1. The numerical values of the parameters of the model and the coordinates of the poles in the complex plane for two types of cuto function andΛ = 0.42GeV.

3 Conclusions

We explored the well-established charm-anticharm vector resonanceψ(4040)by usinga quan- tum eld approach. In particular, we studied its spectral function, which turns out to be not compatible with a standard Breit-Wigner shape due to a signicant deformation in the energy region close to 3.9 GeV. Moreover, two poles emerge in the complex plane: an expected one for the resonance ψ(4040) and a second one related to the left enhancement generated by DD loops. Although a direct assignment of this additional pole to Y(4008)is not possible, the study of the reactione+e→ψ(4040)→DD→π+π shows thatY(4008)does not necessarly describe a genuine resonance, but is an eect ofDD quantum uctuations.

Acknowledgements

The authors thank P. Kovacs for cooperation and S. Coito for useful discussions and acknowledge nancial support from the Polish National Science Centre (NCN) through the OPUS project no.

2015/17/B/ST2/01625.

References

[1] N. Brambilla et al., Eur. Phys. J. C 71, 1534 (2011)

[2] H. X. Chen, W. Chen, X. Liu and S. L. Zhu, Phys. Rept. 639, 1 (2016) [3] M. Piotrowska, F. Giacosa and P. Kovacs, in preparation

[4] M. Tanabashi et al. (Particle Data Group), Phys. Rev. D 98, 030001 (2018) [5] C. Z. Yuan et al. [Belle Collaboration], Phys. Rev. Lett. 99, 182004 (2007) [6] Z. Q. Liu et al. [Belle Collaboration], Phys. Rev. Lett. 110, 252002 (2013) [7] T. Wolkanowski, M. Soªtysiak and F. Giacosa, Nucl. Phys. B 909, 418 (2016)

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