Relativistic effects in the two-nucleon system

Zuilhof, M.J.; Tjon, J.A.

doi:10.1103/physrevc.24.736

Cited by 78 publications

(31 citation statements)

References 17 publications

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“…Indeed, we see here that, as already found by Arnold et al [93] and Zuilhof and Tjon [94], that inclusion of relativistic effects actually worsens the agreement with the experimental data. The inclusion of these effects to all orders in a Q/M N expansion does not lead to a small correction which brings the theory into closer agreement with the experimental data.…”

Section: Equal Timesupporting

confidence: 77%

Measurement of the Electric and Magnetic Elastic Structure Functions of the Deuteron at Large Momentum Transfers

Suleiman

1999

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Section: Equal Timesupporting

confidence: 77%

Measurement of the Electric and Magnetic Elastic Structure Functions of the Deuteron at Large Momentum Transfers

Suleiman

1999

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“…It has however been solved for the two-nucleon system in Euclidean space [133] and applied to the calculation of electron-deuteron scattering [134,135].…”

Section: The Bethe-salpeter Equationmentioning

confidence: 99%

The Deuteron: Structure and Form Factors

Garçon

Orden

2001

Advances in the Physics of Particles and Nuclei

176

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“…Most relativistic calculations do not include contributions from MEC's such as the p r y process and are therefore referred to as relativistic impulse approximation (RIA). However the pair and retardation currents are included automatically in some models of RIA [64,65]. A fully relativistic analysis of the p r y and way currents, calculated consistently with the NN dynamics within a relativistic quasipotential one-boson-exchange model, has been done recently by Hummel and Tjon [66].…”

Section: Relativistic Impulse Approximationmentioning

confidence: 99%

Tensor polarization in elastic electron-deuteron scattering in the momentum transfer range 3.8≤Q≤4.6fm−1

et al. 1994

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The tensor polarization of the recoil deuteron in elastic electron-deuteron scattering has been measured at the Bates Linear Accelerator Center at three values of four-momentum transfer, Q = 3.78, 4.22, and 4.62 fm-', corresponding to incident electron energies of 653, 755, and 853 MeV. The scattered electrons and the recoil deuterons were detected in coincidence. The recoil deuterons were transported to a liquid hydrogen target to undergo a second scattering. The angular distribution of the d-p scattering was measured using a polarimeter. The polarimeter was calibrated in an auxiliary experiment using a polarized deuteron beam at the Laboratoire National Saturne. A Monte Carlo procedure was used to generate interpolated calibration data because the energy spread in the deuteron energies in the Bates experiment spanned the range of deuteron energies in the calibration experiment. The extracted values of tzo are compared to predictions of different theoretical models of the electromagnetic form factors of the deuteron: nonrelativistic and relativistic nucleon-meson dynamics, Skyrme model, quark models, and perturbative quantum chromodynamics. Along with the world data on the structure functions A ( Q ) and B(Q), they are used to separate the charge monopole and charge quadrupole form factors of the deuteron. A node in the charge monopole form factor is observed at Q = 4.39 i 0.16 fm-' .

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Relativistic effects in the two-nucleon system

Cited by 78 publications

References 17 publications

Measurement of the Electric and Magnetic Elastic Structure Functions of the Deuteron at Large Momentum Transfers

Measurement of the Electric and Magnetic Elastic Structure Functions of the Deuteron at Large Momentum Transfers

The Deuteron: Structure and Form Factors

Tensor polarization in elastic electron-deuteron scattering in the momentum transfer range 3.8≤Q≤4.6fm−1

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