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d(e,e'p) Studies of Exclusive Deuteron Electro-Disintegration

Fuente: arXiv

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Detalles Bibliográficos
Autores principales:	Boeglin, W. U., Ambrozewicz, P., Aniol, K., Arrington, J., Batigne, G., Bosted, P., Camsonne, A., Coman, L., Chang, G., Chen, J. P., Choi, S., Deur, A., Epstein, M., Finn, J. M., Frullani, S., Furget, C., Garibaldi, F., Gayou, O., Gilman, R., Hansen, O., Hayes, D., Higinbotham, D. W., Hinton, W., Hyde, C. E., Ibrahim, H., de Jager, C. W., Jiang, X., Jones, M. K., Kaufman, L. J., Khanal, H., Klein, A., Kox, S., Kramer, L., Kumbartzki, G., Laget, J. M., LeRose, J., Lindgren, R., Margaziotis, D. J., Markowitz, P., McCormick, K., Meziani, Z., Michaels, R., Milbrath, B., Mitchell, J., Monaghan, P., Moteabbed, M., Moussiegt, P., Nasseripour, R., Paschke, K., Perdrisat, C., Piasetzky, E., Punjabi, V., Qattan, I. A., Quéméner, G., Ransome, R. D., Raue, B., Réal, J. S., Reinhold, J., Reitz, B., Roché, R., Roedelbronn, M., Saha, A., Slifer, K., Solvignon, P., Sulkosky, V., Ulmer, P. E., Voutier, E., Weinstein, L. B., Wojtsekhowski, B., Zeier, M.
Formato:	Preprint
Publicado:	2026
Materias:	Nuclear Experiment
Acceso en línea:	Acceder al recurso
Etiquetas:	Agregar Etiqueta Sin Etiquetas, Sea el primero en etiquetar este registro!

_version_	1866914536088403968
author	Boeglin, W. U. Ambrozewicz, P. Aniol, K. Arrington, J. Batigne, G. Bosted, P. Camsonne, A. Coman, L. Chang, G. Chen, J. P. Choi, S. Deur, A. Epstein, M. Finn, J. M. Frullani, S. Furget, C. Garibaldi, F. Gayou, O. Gilman, R. Hansen, O. Hayes, D. Higinbotham, D. W. Hinton, W. Hyde, C. E. Ibrahim, H. de Jager, C. W. Jiang, X. Jones, M. K. Kaufman, L. J. Khanal, H. Klein, A. Kox, S. Kramer, L. Kumbartzki, G. Laget, J. M. LeRose, J. Lindgren, R. Margaziotis, D. J. Markowitz, P. McCormick, K. Meziani, Z. Michaels, R. Milbrath, B. Mitchell, J. Monaghan, P. Moteabbed, M. Moussiegt, P. Nasseripour, R. Paschke, K. Perdrisat, C. Piasetzky, E. Punjabi, V. Qattan, I. A. Quéméner, G. Ransome, R. D. Raue, B. Réal, J. S. Reinhold, J. Reitz, B. Roché, R. Roedelbronn, M. Saha, A. Slifer, K. Solvignon, P. Sulkosky, V. Ulmer, P. E. Voutier, E. Weinstein, L. B. Wojtsekhowski, B. Zeier, M.
author_facet	Boeglin, W. U. Ambrozewicz, P. Aniol, K. Arrington, J. Batigne, G. Bosted, P. Camsonne, A. Coman, L. Chang, G. Chen, J. P. Choi, S. Deur, A. Epstein, M. Finn, J. M. Frullani, S. Furget, C. Garibaldi, F. Gayou, O. Gilman, R. Hansen, O. Hayes, D. Higinbotham, D. W. Hinton, W. Hyde, C. E. Ibrahim, H. de Jager, C. W. Jiang, X. Jones, M. K. Kaufman, L. J. Khanal, H. Klein, A. Kox, S. Kramer, L. Kumbartzki, G. Laget, J. M. LeRose, J. Lindgren, R. Margaziotis, D. J. Markowitz, P. McCormick, K. Meziani, Z. Michaels, R. Milbrath, B. Mitchell, J. Monaghan, P. Moteabbed, M. Moussiegt, P. Nasseripour, R. Paschke, K. Perdrisat, C. Piasetzky, E. Punjabi, V. Qattan, I. A. Quéméner, G. Ransome, R. D. Raue, B. Réal, J. S. Reinhold, J. Reitz, B. Roché, R. Roedelbronn, M. Saha, A. Slifer, K. Solvignon, P. Sulkosky, V. Ulmer, P. E. Voutier, E. Weinstein, L. B. Wojtsekhowski, B. Zeier, M.
contents	The d(e,e'p) cross section was measured at momentum transfers $Q^2 = $ 0.8, 2.1 and 3.5 $(GeV/c)^2$ covering a wide range of proton kinematics at each $Q^2$ setting that made it possible to study this reaction as a function of missing momentum as well as a function of the neutron laboratory recoil angle $θ_{nq}$. Missing momentum distributions were determined for fixed values of $θ_{nq}$ up to missing momenta of 0.65 $GeV/c$. For the two larger momentum transfer settings, the characteristics of the experimental momentum distributions confirm the theoretical prediction that final state interactions (FSI) contribute maximally around a $θ_{nq} \sim 70^\circ$, while for $θ_{nq} < 45^\circ$ FSI are significantly reduced. The data at reduced FSI settings were best reproduced by calculations using the CD-Bonn potential wave functions.
format	Preprint
id	arxiv_https___arxiv_org_abs_2603_17081
institution	arXiv
publishDate	2026
record_format	arxiv
spellingShingle	d(e,e'p) Studies of Exclusive Deuteron Electro-Disintegration Boeglin, W. U. Ambrozewicz, P. Aniol, K. Arrington, J. Batigne, G. Bosted, P. Camsonne, A. Coman, L. Chang, G. Chen, J. P. Choi, S. Deur, A. Epstein, M. Finn, J. M. Frullani, S. Furget, C. Garibaldi, F. Gayou, O. Gilman, R. Hansen, O. Hayes, D. Higinbotham, D. W. Hinton, W. Hyde, C. E. Ibrahim, H. de Jager, C. W. Jiang, X. Jones, M. K. Kaufman, L. J. Khanal, H. Klein, A. Kox, S. Kramer, L. Kumbartzki, G. Laget, J. M. LeRose, J. Lindgren, R. Margaziotis, D. J. Markowitz, P. McCormick, K. Meziani, Z. Michaels, R. Milbrath, B. Mitchell, J. Monaghan, P. Moteabbed, M. Moussiegt, P. Nasseripour, R. Paschke, K. Perdrisat, C. Piasetzky, E. Punjabi, V. Qattan, I. A. Quéméner, G. Ransome, R. D. Raue, B. Réal, J. S. Reinhold, J. Reitz, B. Roché, R. Roedelbronn, M. Saha, A. Slifer, K. Solvignon, P. Sulkosky, V. Ulmer, P. E. Voutier, E. Weinstein, L. B. Wojtsekhowski, B. Zeier, M. Nuclear Experiment The d(e,e'p) cross section was measured at momentum transfers $Q^2 = $ 0.8, 2.1 and 3.5 $(GeV/c)^2$ covering a wide range of proton kinematics at each $Q^2$ setting that made it possible to study this reaction as a function of missing momentum as well as a function of the neutron laboratory recoil angle $θ_{nq}$. Missing momentum distributions were determined for fixed values of $θ_{nq}$ up to missing momenta of 0.65 $GeV/c$. For the two larger momentum transfer settings, the characteristics of the experimental momentum distributions confirm the theoretical prediction that final state interactions (FSI) contribute maximally around a $θ_{nq} \sim 70^\circ$, while for $θ_{nq} < 45^\circ$ FSI are significantly reduced. The data at reduced FSI settings were best reproduced by calculations using the CD-Bonn potential wave functions.
title	d(e,e'p) Studies of Exclusive Deuteron Electro-Disintegration
topic	Nuclear Experiment
url	https://arxiv.org/abs/2603.17081