# Electroexcitation of the Roper resonance for GeV in

###### Abstract

The helicity amplitudes of the electroexcitation of the Roper resonance are extracted for GeV from recent high precision JLab-CLAS cross section and longitudinally polarized beam asymmetry data for electroproduction on protons at GeV. The analysis is made using two approaches, dispersion relations and a unitary isobar model, which give consistent results. It is found that the transverse helicity amplitude for the N(1440)P transition, which is large and negative at , becomes large and positive at GeV, and then drops slowly with . The longitudinal helicity amplitude , which was previously found from CLAS data to be large and positive at GeV, drops with . Available model predictions for N(1440)P allow us to conclude that these results provide strong evidence in favor of N(1440)P as a first radial excitation of the 3 ground state. The results of the present paper also confirm the conclusion of our previous analysis for GeV that the presentation of N(1440)P as a qG hybrid state is ruled out.

###### pacs:

PACS number(s): 11.55.Fv, 13.40.Gp, 13.60.Le, 14.20.Gk]Deceased ]Deceased

The CLAS Collaboration

The excitation of nucleon resonances in electromagnetic interactions has long been recognized as a sensitive source of information on the long- and short-range structure of the nucleon and its excited states in the domain of quark confinement. Constituent quark models (CQM) have been developed that relate electromagnetic resonance transition form factors to fundamental quantities, such as the quark confining potential. While this relationship is more direct for heavy quarks, even in the light quark sector such connections exist and may be probed by measuring transition form factors over a large range in photon virtuality , which defines the space-time resolution of the probe.

The so-called Roper resonance, or N(1440)P, is the lowest excited state of the nucleon. In the CQM, the simplest and most natural assumption is that this is the first radial excitation of the 3 ground state. However, calculations within the nonrelativistic CQM fail to reproduce even the sign of the transition photo-coupling amplitude Capstick1 (). Moreover, the mass of the state is more than 100 MeV lower than what is predicted in the CQM with gluon exchange interaction Capstick2 (); Richard (). More recent models that include also Goldstone boson exchange between quarks gave better agreement with the mass Glozman (). To deal with shortcomings of the quark model, alternative descriptions of N(1440)P were developed, where this resonance is treated respectively as: a hybrid qG state where the three quarks are bound together with a gluon Li1 (); Li2 (), a quark core dressed by a meson cloud Cano1 (); Cano2 (), and a dynamically generated resonance Krewald (); other models include 3 components, in particular a strong component (see Ref. Dillig () and references therein). Discrimination between these descriptions of the Roper resonance can provide deep insight into the underlying basic symmetries and the structure of quark confinement.

The dependence of the electromagnetic transition form factors is highly sensitive to different descriptions of the Roper state. However, until recently, the data base used to extract these form factors was almost exclusively based on production, and very limited in kinematical coverage. Also, the final state is dominated by the nearby isospin P resonance, whereas the isospin Roper state couples more strongly to the channel. The CLAS Collaboration has now published a large body of precise differential cross sections and polarized beam asymmetries for the process in the range of invariant hadronic mass GeV and photon virtuality GeV, with full azimuthal and polar angle coverage Park (). In this Letter we report the results on the electroexcitation of the Roper resonance extracted from this large data set.

The approaches we used to analyze the data are fixed- dispersion relations (DR) and a unitary isobar model (UIM). They were successfully employed in Refs. Azn0 (); Azn04 (); Azn065 () for analyses of pion-photoproduction and low--electroproduction data.

The imaginary parts of the amplitudes in the DR and UIM approaches are determined mainly by -channel resonance contributions that we parameterize in the usual Breit-Wigner form with energy-dependent widths. We also take into account inelastic channels in the form proposed in Ref. Drechsel (). An exception was made for the P resonance, which was treated differently. According to the phase-shift analyses of scattering, the amplitude corresponding to the resonance is elastic up to GeV (see, for example, the latest GWU analyses GWU1 (); GWU2 ()). In combination with DR and Watson’s theorem, this provides strict constraints on the multipole amplitudes , , that correspond to the P resonance. In particular, as was shown in Ref. Azn0 (), the -dependence of is close to that from the GWU analysis GWU3 () at if the same normalizations of the amplitudes at the resonance position are used. This constraint on the large amplitude plays an important role in the reliable extraction of the N(1440)P electroexcitation amplitudes, because the P and N(1440)P states are overlapping.

We have taken into account all resonances from the first, second, and third resonance regions. These are 4- and 3-star resonances P, N(1440)P, N(1520)D, N(1535)S, P, S, N(1650)S, N(1675)D, N(1680)F, N(1700)D, D, N(1710)P, and N(1720)P. For the masses, widths, and branching ratios of these resonances, we used the mean values of the data presented in the Review of Particle Physics (RPP) PDG (). In particular for the Roper resonance, the values GeV, GeV, and were taken. Resonances of the fourth resonance region practically have no influence in the energy region under investigation and were not included.

For the values of under consideration, the available data are related mostly to the P resonance region Frolov (); Joo1 (); Ungaro (). The DESY data Haidan () at higher energies GeV (GeV) have very limited angular coverage. Our analysis showed that the combined Frolov (); Joo1 (); Ungaro (); Haidan () and Park () data give results that are very close to those obtained from the data Park () alone. For this reason, and also to avoid mixing data sets with different systematic uncertainties, in this letter we present the results for N(1440)P obtained from the analysis of the data Park () only.

At each available for Park (), GeV, we performed two kinds of fits in both approaches: (i) The magnitudes of the helicity amplitudes corresponding to all resonances listed above were fitted. (ii) The transverse amplitudes for the members of the multiplet : S, N(1650)S, N(1675)D, N(1700)D, and D, were fixed according to the single quark transition model SQTM (), which relates these amplitudes to those for N(1520)D and N(1535)S; the longitudinal amplitudes of these resonances and the amplitudes of the resonances P and N(1710)P, which have small photocouplings GWU3 (); PDG () and are not seen in low and 2 electroproduction Azn065 (), were assumed to be zero. The results obtained for P, N(1440)P, N(1520)D, and N(1535)S in the two fits were very close to each other. The amplitudes of the Roper resonance presented below are the average values of the results obtained in these fits. The uncertainties arising from the averaging procedure we will refer to as uncertainties (I). They were included in quadrature into the total systematic uncertainties.

The background of both approaches contains Born terms corresponding to the - and - channel nucleon exchanges and -channel pion contribution, and depends, therefore, on the proton, neutron, and pion form factors. The background of the UIM contains also the and -channel exchanges Drechsel () and, therefore, the contribution of the form factors . All of these form factors, except the neutron electric and ones, are known in the region of under investigation from existing experimental data. For the proton form factors we used the parameterizations found for the existing data in Ref. 21 (). The neutron magnetic form factor and the pion form factor were taken from Refs. 22 () and 23 (); 24 (); 25 (); 26 (), respectively. The neutron electric form factor, , is measured up to GeV 27 (), and Ref. 27 () presents a parameterization for all existing data on that we used for extrapolation of to GeV. In our final results we accounted for a systematic uncertainty assuming a deviation from this parameterization. There are no measurements of the form factors ; however, investigations made using both QCD sum rules 28 () and quark model 29 () predict a dependence of close to the dipole form factor . In our analysis we assumed that , and introduced in our final results a systematic uncertainty that can arise from a deviation from this assumption. All of these uncertainties, including those that arise from the measured proton, neutron, and pion form factors, were added in quadrature and will be referred to as systematic uncertainties (II) in our final results.

In Fig. 1, we present the comparison of our results with the experimental data for the lowest Legendre moments of the structure function at GeV Park (). The Legendre moment is the independent part of ; it does not contain interference of different multipole amplitudes and is related to the sum of squares of these amplitudes. The resonance behavior of the multipole amplitudes is revealed in in the form of enhancements. Resonance structures related to the resonances P, N(1520)D, and N(1535)S are clearly seen in . There is a shoulder between the and GeV peaks, which is related to the broad Roper resonance. To demonstrate this, we present in Fig. 1 the curves obtained by switching off the N(1440)P resonance in the final DR results. A fit to the data with the Roper amplitudes put to zero results in and gives the dip in of the same size as in Fig. 1. This clearly shows that the data can not be explained without the Roper resonance.

To stress the advantage of the investigation of the Roper resonance in the reaction , we note that for this reaction the relative contribution of N(1440)P in comparison with P in is four times larger than for , because isospin and resonances enter the amplitudes with the coefficients for in the final state and for .

The role of N(1440)P is also seen in other Legendre moments. In , the large effect caused by switching off this resonance is connected with the interference of corresponding to N(1440)P with the non-resonant and N(1535)S contributions to , which creates a linear dependence of in . Due to interference effects like those mentioned above and to the large width of this state, the N(1440)P plays a significant role in the entire range covered by the data.

(GeV) | GeV | ||

DR | |||

1.72 | 5101 | 3.1 | |

2.05 | 5844 | 2.4 | |

2.44 | 6177 | 2.1 | |

2.91 | 6251 | 2.0 | |

3.48 | 6105 | 1.5 | |

4.16 | 5778 | 1.1 | |

UIM | |||

1.72 | 5101 | 3.5 | |

2.05 | 5844 | 2.3 | |

2.44 | 6177 | 2.1 | |

2.91 | 6251 | 2.2 | |

3.48 | 6105 | 1.6 | |

4.16 | 5778 | 1.1 |

We now discuss the results for the N(1440)P helicity amplitudes presented in Table 1 and Fig. 2. The results obtained using DR and UIM are given in Table 1 separately; it can be seen that they are close to each other. As the non-resonant background of these approaches is built in conceptually different ways, we conclude that the model uncertainties of the obtained results are relatively small. In Fig. 2 we present average values of the results obtained within the DR and UIM approaches. The uncertainties that originate from this averaging procedure are referred to as systematic uncertainties (III) in our final results.

Combined with the information obtained from the previous CLAS data at GeV Azn04 (); Azn065 (); Joo1 (); Joo2 (); Joo3 (); Egiyan (), and that at PDG (), our results show the following behavior of the transverse helicity amplitude : being large and negative at , it crosses zero between and GeV and becomes large and positive at GeV. With increasing , this amplitude drops smoothly in magnitude. The longitudinal helicity amplitude , which is large and positive at small , drops smoothly with increasing .

In Fig. 2, we compare our results with model predictions. These are (i) quark model predictions Capstick1 (); Weber (); Simula (); Riska (); Quark () where the N(1440)P is described as the first radial excitation of the 3 ground state; (ii) those assuming the N(1440)P is a hybrid state Li2 (); and (iii) the results for the Roper resonance treated as a quark core (which is a radial excitation of the 3 ground state) dressed by a meson cloud Cano1 (); Cano2 ().

It is known that with increasing , when the momentum transfer becomes larger than the masses of the constituent quarks, a relativistic treatment of the electroexcitation of the nucleon resonances, which is important already at , becomes crucial. A consistent way to perform the relativistic treatment of the transitions is to consider them in light-front (LF) dynamics. In Fig. 2 we present the results obtained in the LF quark models Capstick1 (); Weber (); Simula (); Riska (); Quark (). All LF approaches Capstick1 (); Weber (); Simula (); Riska (); Quark () give a good description of nucleon form factors, however, the predictions for the N(1440)P helicity amplitudes differ significantly. This is caused by the large sensitivity of these amplitudes to the N and N(1440)P wave functions Quark (). The approaches Capstick1 (); Weber (); Simula (); Riska (); Quark () fail to describe the value of the transverse amplitude at . This can be an indication of a large meson cloud contribution to N(1440)P, which is expected to be significant at small . As a confirmation of this assumption, one can consider the results of Refs. Cano1 (); Cano2 () where this contribution is taken into account, and a good description of the helicity amplitudes is obtained at small .

In spite of the differences, all LF predictions for the N(1440)P helicity amplitudes have common features that agree with the results extracted from the experimental data: (i) the sign of the transverse amplitude at is negative, (ii) the sign of the longitudinal amplitude is positive, (iii) all LF approaches predict the sign change of the transverse amplitude at small . We take this qualitative agreement as evidence in favor of the N(1440)P resonance as a radial excitation of the 3 ground state. Final confirmation of this conclusion requires a complete simultaneous description of the nucleon form factors and the N(1440)P amplitudes. This will allow us to find the magnitude of the meson cloud contribution, and to better specify the and N(1440)P wave functions. To achieve a satisfactory description at large , it may be necessary to take into account quark form factors, as well as other effects, such as the quark mass dependence on the momentum transfer.

The results of Refs. Li1 (); Li2 (), where N(1440)P is treated as a hybrid state, are obtained via non-relativistic calculations. Nevertheless the suppression of the longitudinal amplitude has its physical origin in the fact that the longitudinal transition operator for the vertex requires both a spin and angular momentum flip by one unit, while the angular momenta of quarks in the N and N(1440)PqG are equal to 0. This makes this result practically independent of relativistic effects. The predicted suppression of the longitudinal amplitude strongly disagrees with the experimental results.

In summary, for the first time the transverse and longitudinal helicity amplitudes of the N(1440)P transition are extracted from experimental data at high . The results are obtained from differential cross sections and longitudinally polarized beam asymmetries for electroproduction on protons at GeV Park (). The data were analyzed using two conceptually different approaches, DR and UIM, which give close results.

Comparison with quark model predictions provides strong evidence in favor of N(1440)P as a first radial excitation of the 3 ground state.

The results for the longitudinal helicity amplitude confirm our conclusion made from the previous analysis of CLAS data for GeV Azn04 () that the presentation of the Roper resonance as a qG hybrid state is ruled out.

This work was supported in part by the U.S. Department of Energy and the National Science Foundation, the Korea Research Foundation, the French Commissariat a l’Energie Atomique, and the Italian Instituto Nazionale di Fisica Nucleare. Jefferson Science Associates, LLC, operates Jefferson Lab under U.S. DOE contract DE-AC05-060R23177.

## References

- (1) S. Capstick and B. D. Keister, Phys. Rev. D , 3598 (1995).
- (2) S. Capstick and N. Isgur, Phys. Rev. D , 2809 (1986).
- (3) J.-M. Richard, Phys. Rep. , 1 (1992).
- (4) L. Ya. Glozman and D. O. Riska, Phys. Rep. , 263 (1996).
- (5) Z. P. Li, Phys. Rev. D , 2841 (1991).
- (6) Z. P. Li, V. Burkert, and Zh. Li, Phys. Rev. D , 70 (1992).
- (7) F. Cano, P. González, S. Noguera, and B. Desplanques, Nucl. Phys. A , 257 (1996).
- (8) F. Cano and P. González, Phys. Lett. B , 270 (1998).
- (9) O. Kreil, C. Hanhart, S. Krewald, and J. Speth, Phys. Rev. C , 025207 (2000).
- (10) M. Dillig and J. Schott, Phys. Rev. C , 067001 (2007).
- (11) K. Park et al., CLAS Collaboration, Phys. Rev. C , 015208 (2008).
- (12) I. G. Aznauryan, Phys. Rev. C , 015209 (2003).
- (13) I. G. Aznauryan, V. D. Burkert, H. Egiyan, et al., Phys. Rev. C , 015201 (2005).
- (14) I. G. Aznauryan, V. D. Burkert, et al., Phys. Rev. C , 045201 (2005).
- (15) D. Drechsel, O. Hanstein, S. Kamalov, and L. Tiator, Nucl. Phys. A , 145 (1999).
- (16) R. A. Arndt, W. J. Briscoe, I. I. Strakovsky, and R. L. Workman, Phys. Rev. C , 035213 (2004).
- (17) R. A. Arndt, W. J. Briscoe, I. I. Strakovsky, and R. L. Workman, Phys. Rev. C , 045205 (2006).
- (18) R. A. Arndt, W. J. Briscoe, I. I. Strakovsky, and R. L. Workman, Phys. Rev. C , 055213 (2002).
- (19) W.-M. Yao et al. [Particle Data Group], Journal of Physics G , 1 (2006).
- (20) V. V. Frolov et al., Phys. Rev. Lett. , 45 (1999).
- (21) K. Joo et al., CLAS Collaboration, Phys. Rev. Lett. , 122001 (2002).
- (22) M. Ungaro et al., CLAS Collaboration, Phys. Rev. Lett. , 112003 (2006).
- (23) R. Haidan, PhD thesis, University of Hamburg, Hamburg, 1979.
- (24) V. D. Burkert et al., Phys. Rev. C , 035204 (2003).
- (25) J. Arrington, W. Melnitchouk, and J. A. Tjon, Phys. Rev. C , 035205 (2007).
- (26) W. K. Brooks et al., Nucl. Phys. A , 261 (2005).
- (27) C. J. Bebek et al., Phys. Rev. D , 25 (1976).
- (28) C. J. Bebek et al., Phys. Rev. D , 1693 (1978).
- (29) T. Horn et al., Phys. Rev. Lett. , 192001 (2006).
- (30) V. Tadevosyan et al., Phys. Rev. C , 055205 (2007).
- (31) R. Madey et al., Phys. Rev. Lett. , 122002 (2003).
- (32) V. Eletski and Ya. Kogan, Yad. Fiz. , 138 (1984).
- (33) I. Aznauryan and K. Oganessyan, Phys. Lett. B , 309 (1990).
- (34) K. Joo et al., CLAS Collaboration, Phys. Rev. C , 032201 (2003).
- (35) K. Joo et al., CLAS Collaboration, Phys. Rev. C , 042201 (2004).
- (36) H. Egiyan et al., CLAS Collaboration, Phys. Rev. C , 025204 (2006).
- (37) H. J. Weber, Phys. Rev. C , 2783 (1990).
- (38) F. Cardarelli, E. Pace, G. Salme, and S. Simula, Phys. Lett. B , 13 (1997).
- (39) B. Juliá-Díaz, D. O. Riska, and F. Coester, Phys. Rev. C , 035212 (2004).
- (40) I. G. Aznauryan, Phys. Rev. C , 025212 (2007).