In-Medium K^{+} Electromagnetic Form Factor with a Symmetric Vertex in a Light Front Approach Presented by George H. S. Yabusaki at LIGHT-CONE 2017 Conference in Mumbai, India.

In-Medium Electromagnetic Form Factor with a Symmetric Vertex in a Light Front Approach thanks: Presented by George H. S. Yabusaki at LIGHT-CONE 2017 Conference in Mumbai, India.

George H. S. Yabusaki Instituto Tecnológico de Aeronáutica - ITA Praça Marechal Eduardo Gomes, 50, Vila das Acácias, 12228-900, São José dos Campos, SP - Brazil
22email: yabusaki@gmail.comLaboratório de Física Teórica e Computacional - UCS Rua Galvão Bueno, 868, Bloco B - Sala 107, Liberdade, 01506-000, São Paulo, SP - Brazil
   J. P. B. C. de Melo Instituto Tecnológico de Aeronáutica - ITA Praça Marechal Eduardo Gomes, 50, Vila das Acácias, 12228-900, São José dos Campos, SP - Brazil
22email: yabusaki@gmail.comLaboratório de Física Teórica e Computacional - UCS Rua Galvão Bueno, 868, Bloco B - Sala 107, Liberdade, 01506-000, São Paulo, SP - Brazil
   Wayne de Paula Instituto Tecnológico de Aeronáutica - ITA Praça Marechal Eduardo Gomes, 50, Vila das Acácias, 12228-900, São José dos Campos, SP - Brazil
22email: yabusaki@gmail.comLaboratório de Física Teórica e Computacional - UCS Rua Galvão Bueno, 868, Bloco B - Sala 107, Liberdade, 01506-000, São Paulo, SP - Brazil
   K. Tsushima Instituto Tecnológico de Aeronáutica - ITA Praça Marechal Eduardo Gomes, 50, Vila das Acácias, 12228-900, São José dos Campos, SP - Brazil
22email: yabusaki@gmail.comLaboratório de Física Teórica e Computacional - UCS Rua Galvão Bueno, 868, Bloco B - Sala 107, Liberdade, 01506-000, São Paulo, SP - Brazil
   T. Frederico Instituto Tecnológico de Aeronáutica - ITA Praça Marechal Eduardo Gomes, 50, Vila das Acácias, 12228-900, São José dos Campos, SP - Brazil
22email: yabusaki@gmail.comLaboratório de Física Teórica e Computacional - UCS Rua Galvão Bueno, 868, Bloco B - Sala 107, Liberdade, 01506-000, São Paulo, SP - Brazil
Received: date / Accepted: date
Abstract

Using the light-front -meson wave function based on a Bethe-Salpeter amplitude model for the quark-antiquark bound state, we study the Electromagnetic Form Factor (EMFF) of the -meson in nuclear medium within the framework of light-front field theory. The -meson model we adopt is well constrained by previous and recent studies to explain its properties in vacuum. The in-medium -meson EMFF is evaluated for the plus-component of the electromagnetic current, , in the Breit frame. In order to consistently incorporate the constituent up and antistrange quarks of the -meson immersed in symmetric nuclear matter, we use the quark-meson coupling (QMC) model, which has been widely applied to various hadronic and nuclear phenomena in a nuclear medium with success. We predict the in-medium modification of the -meson EMFF in symmetric nuclear matter. It is found that, after a fine tuning of the regulator mass, i.e. GeV, the model is suitable to fit the available experimental data in vacuum within the theoretical uncertainties, and based on this we predict the in-medium modification of the -meson EMFF.

Keywords:
-meson Light Front Form Factor Nuclear Medium Meson Quark-Meson Coupling
journal: Few-Body Systems

1 Introduction

The main purpose of this work is to investigate the in-medium modification of the -meson EMFF in symmetric nuclear matter combined with the QMC model [1], where the -meson model [2] is adjusted so as to provide the best description of the -meson EMFF data in vacuum. The study of the lighter pseudoscalar mesons plays an important role to understand the low energy QCD. Their static and dynamical properties have also been investigated theoretically and experimentally [3; 4; 5; 6; 7; 8; 9; 10; 11; 12]. With respect to the description of bound states on the light cone, a detailed review of hadronic wave functions in QCD-based models can be found in Ref. [13]. Additional important knowledge about the meson’s internal structure can be inferred from their valence-quark distribution functions. The theoretical framework we adopt is the light-front field theory [13; 14], more specifically, we use a symmetric vertex model for -meson bound-state in the light-front approach for the Bethe-Salpeter amplitude. The light-front component of the electromagnetic current has been successfully used to calculate elastic form factor. For the symmetric vertex model [15], the components of the current are conveniently obtained in the Drell-Yan frame, where the light-front bound state wave functions are defined on the hypersurface and are covariant under kinematical boosts due to the stability of Fock-state decomposition [13; 16]. In this work, we consider the symmetric vertex function with the intention to optimize and unify the parameter set to simultaneously reproduce the electromagnetic form factor. Our numerical results are compared with experimental data in vacuum up to to explore the validity of the model, where , with being the four-momentum transfer.

2 The Model

The electromagnetic current for a two-fermion bound state system with spin zero and intrinsic negative parity, , a -meson ( bound state), is calculated in one-loop approximation (triangle diagram shown in Fig. 1), modelling the Bethe-Salpeter amplitude through a symmetric vertex function in momentum space with a pseudoscalar coupling between -meson and quarks. This coupling is given by the effective Lagrangian [2; 15; 17]:

(1)

here, and , is given by the with , the symmetric vertex function in nuclear medium and the -meson decay constant. In this study we approximate to use value in vacuum. In the Hartree mean field approximation the modifications enter as the shift of the light-quark momentum via due to the vector potential, and in the Lorentz-scalar part through the Lorentz-scalar potential as [1; 18] and based on the QMC model [1]. The QMC model has been applied to many nuclear and hadronic phenomena in a nuclear medium with success, and the inputs in vacuum as well as quantities calculated in-medium shown in Table 1 were adopted in the model to describe the effects of nuclear medium. The electromagnetic current for -meson with the plus-component, is obtained from the covariant expression Eq. (2) corresponding to the triangle diagram in Fig. 1

Figure 1: Diagrams for -meson photon interaction.
(2)

where , and are the symmetric vertex function in nuclear medium, where the vertex function is given by [15]

(3)

with being the number of colors in QCD, and

(4)

are corresponding to the up and antistrange quark propagators, respectively, in symmetric nuclear matter. In addiction we use , the vacuum value.

We summarize here the light-front model in vacuum for the symmetric vertex function ( and ) for the pseudoscalar bound states. Also, we work in the Breit frame and using light-front variables, , and , and one has

(5)

where the Drell-Yan condition is recovered with [6; 15; 19]. As is well known the -meson form factor can be extracted from the covariant expression below:

(6)

If covariance and current conservation are fulfilled, one can obviously use any frame and any nonvanishing component of the current to calculate the electromagnetic form factor. In the light-front approach, however, besides the valence component of the electromagnetic current, we can have the nonvalence contribuition or zero modes; thus in the light-front, this two contributions enter in the full electromagnetic form factor:

(7)

where , has the loop integration on constrained by (see the light-front time-ordered diagram in Fig. 2 (a)) the valence , and has the loop integration on in the interval (see Fig. 2 (b)) the nonvalence , pair production contributions with , we use only the valence component, since the non-valence component goes to zero in the adopted framework (further see Ref. [2] for more details).

Figure 2: Light-Front diagrams: (a) valence contribution and (b) non-valence contributions.

Now we considerer in symmetric nuclear matter. After the integration for current Eq. (2) using the Cauchy’s Theorem, a light-front wave function emerges for a symmetric vertex function with the change of variable in medium where . The -meson light-front wave function in symmetric nuclear matter is defined as:

(8)

where is the normalization factor, is a mass operator and is a regulator mass function given by

(9)

and (recall that ).

Using only the valence component, the electromagnetic form factor evaluated in the Breit-frame reads [2; 6; 15; 17; 18]

(10)

the trace in light-front coordinates is

(11)

3 Numerical Results

We have three model parameters: the regulator mass, , the quark masses, and to compute EMFF. Our main aim of this work is to jointly analyze the -meson’s elastic form factors to determine more accurately the model’s quark masses in view of future applications and to test whether a single mass scale, , can satisfactorily describe experimental data for -meson [10; 11], as well as to study the in-medium EMFF. We use the quantities described in Tab. 1 for vacuum, and in-medium inputs computed by the QMC model [1; 18]. Our main results of this study are shown in Fig. 3. As the nuclear matter density increases EMFF decreases faster than that in vacuum, and thus this implies charge radius increases in-medium.

0.440
0.600
Table 1: Parameters used to compute the electromagnetic form factor for -meson in medium, which are calculated by the from QMC model, (for details see Ref. [1; 18]).
Figure 3: Results for -meson form factor squared calculated for different nuclear matter densities using the parameters from Tab. 1. Experimental data form vacuum given by references [10; 11].

Acknowledgements: This work was partially supported by the Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP), Brazil, No. 2015/16295-5 (JPBCM), and No. 2015/17234-0 (KT),  and Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq), Brazil, No. 401322/2014-9 (JPBCM), No. 400826/2014-3 (KT), No. 308025/2015-6 (JPBCM), and No. 308088/2015-8 (KT). This work was part of the projects, Instituto Nacional de Ciência e Tecnologia - Nuclear Physics and Applications (INCT-FNA), Brazil, No. 464898/2014-5, and FAPESP Temático, No. 2017/05660-0.

References

  • [1] K. Saito, K. Tsushima and A. W. Thomas, “Nucleon and hadron structure changes in the nuclear medium and impact on observables,” Prog. Part. Nucl. Phys. 58, 1 (2007)
  • [2] G. H. S. Yabusaki, I. Ahmed, M. A. Paracha, J. P. B. C. de Melo and B. El-Bennich, “Pseudoscalar mesons with symmetric bound state vertex functions on the light front,” Phys. Rev. D 92, no. 3, 034017 (2015)
  • [3] T. Frederico and G. A. Miller, “Null plane phenomenology for the pion decay constant and radius,” Phys. Rev. D 45, 4207 (1992)
  • [4] P. Maris and C. D. Roberts, “Pi- and K meson Bethe-Salpeter amplitudes,” Phys. Rev. C 56, 3369 (1997)
  • [5] H. M. Choi and C. R. Ji, “Nonvanishing zero modes in the light front current,” Phys. Rev. D 58, 071901 (1998)
  • [6] J. P. C. B. de Melo, H. W. L. Naus and T. Frederico, “Pion electromagnetic current in the light cone formalism,” Phys. Rev. C 59, 2278 (1999)
  • [7] H. M. Choi and C. R. Ji, “-meson electroweak form-factors in the light front quark model,” Phys. Rev. D 59, 034001 (1999)
  • [8]  F. Gao, L. Chang, Y. X. Liu, C. D. Roberts and P. C. Tandy, “Exposing strangeness: projections for -meson electromagnetic form factors,” Phys. Rev. D 96, no. 3, 034024 (2017)
  • [9] A. F. Krutov, S. V. Troitsky and V. E. Troitsky, “The -meson form factor and charge radius: linking low-energy data to future Jefferson Laboratory measurements,” Eur. Phys. J. C 77, no. 7, 464 (2017)
  • [10] E. B. Dally et al., “Direct Measurement Of The Negative -meson Form-factor,” Phys. Rev. Lett. 45, 232 (1980)
  • [11] S. R. Amendolia et al., “A Measurement of the -meson Charge Radius,” Phys. Lett. B 178, 435 (1986)
  • [12] K. A. Olive et al. [Particle Data Group], “Review of Particle Physics,” Chin. Phys. C 38, 090001 (2014)
  • [13] S. J. Brodsky, H. C. Pauli and S. S. Pinsky, “Quantum chromodynamics and other field theories on the light cone,” Phys. Rept. 301, 299 (1998)
  • [14] P. A. M. Dirac, “Forms of Relativistic Dynamics,” Rev. Mod. Phys. 21, 392 (1949)
  • [15] J. P. B. C. de Melo, T. Frederico, E. Pace and G. Salme, “Pair term in the electromagnetic current within the front form dynamics: Spin-0 case,” Nucl. Phys. A 707, 399 (2002)
  • [16] R. J. Perry, A. Harindranath and K. G. Wilson, “Light front Tamm-Dancoff field theory,” Phys. Rev. Lett. 65, 2959 (1990)
  • [17] E. O. da Silva, J. P. B. C. de Melo, B. El-Bennich and V. S. Filho, “Pion and -meson elastic form factors in a refined light-front model,” Phys. Rev. C 86, 038202 (2012)
  • [18] J. P. B. C. de Melo, K. Tsushima, B. El-Bennich, E. Rojas and T. Frederico, “Pion structure in the nuclear medium,” Phys. Rev. C 90, no. 3, 035201 (2014)
  • [19] B. L. G. Bakker, H. M. Choi and C. R. Ji, “Regularizing the fermion loop divergencies in the light front meson currents,” Phys. Rev. D 63, 074014 (2001)
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