dorsal/arxiv
View SchemaRelativistic Charge Form Factor of the Deuteron
| Authors | Andrei V. Afanasev, V. D. Afanasev, S. V. Trubnikov |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9712082 |
| URL | https://arxiv.org/abs/nucl-th/9712082 |
Abstract
Relativistic integral representation in terms of experimental neutron-proton scattering phase shifts alone is used to compute the charge form factor of the deuteron $G_{Cd}(Q^2)$. The results of numerical calculations of $|G_{Cd}(Q^2)|$ are presented in the interval of the four-momentum transfers squared $0 \leq Q^2 \leq 35 fm^{-2}$. Zero and the prominent secondary maximum in $ |G_{Cd}(Q^2)|$ are the direct consequences of the change of sign in the experimental $^3S_1$- phase shifts. Till the point $Q^2 \simeq 20 fm^{-2}$ the total relativistic correction to $|G_{Cd}(Q^2)|$ is positive and reaches the maximal value of 25% at $Q^2 \simeq 14 fm^{-2}$.
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"date_created": "2026-03-02T18:00:22.451000Z",
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"abstract": "Relativistic integral representation in terms of experimental neutron-proton\nscattering phase shifts alone is used to compute the charge form factor of the\ndeuteron $G_{Cd}(Q^2)$. The results of numerical calculations of\n$|G_{Cd}(Q^2)|$ are presented in the interval of the four-momentum transfers\nsquared $0 \\leq Q^2 \\leq 35 fm^{-2}$. Zero and the prominent secondary maximum\nin $ |G_{Cd}(Q^2)|$ are the direct consequences of the change of sign in the\nexperimental $^3S_1$- phase shifts. Till the point $Q^2 \\simeq 20 fm^{-2}$ the\ntotal relativistic correction to $|G_{Cd}(Q^2)|$ is positive and reaches the\nmaximal value of 25% at $Q^2 \\simeq 14 fm^{-2}$.",
"arxiv_id": "nucl-th/9712082",
"authors": [
"Andrei V. Afanasev",
"V. D. Afanasev",
"S. V. Trubnikov"
],
"categories": [
"nucl-th",
"hep-ph"
],
"title": "Relativistic Charge Form Factor of the Deuteron",
"url": "https://arxiv.org/abs/nucl-th/9712082"
},
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"source": {
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"variant": "snapshot-2026-03-01",
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