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Main Authors: Ali, Sk M., Maher, C., Zegers, R. G. T., Scott, M., Bazin, D., Bowry, M., Brown, B. A., Campbell, C. M., Gade, A., Gales, S., Garg, U., Harakeh, M. N., Kwan, E., Langer, C., Loelius, C., Morse, C., Noji, S., Redpath, T., Sakai, H., Sasano, M., Sullivan, C., Weisshaar, D.
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2505.06772
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author Ali, Sk M.
Maher, C.
Zegers, R. G. T.
Scott, M.
Bazin, D.
Bowry, M.
Brown, B. A.
Campbell, C. M.
Gade, A.
Gales, S.
Garg, U.
Harakeh, M. N.
Kwan, E.
Langer, C.
Loelius, C.
Morse, C.
Noji, S.
Redpath, T.
Sakai, H.
Sasano, M.
Sullivan, C.
Weisshaar, D.
author_facet Ali, Sk M.
Maher, C.
Zegers, R. G. T.
Scott, M.
Bazin, D.
Bowry, M.
Brown, B. A.
Campbell, C. M.
Gade, A.
Gales, S.
Garg, U.
Harakeh, M. N.
Kwan, E.
Langer, C.
Loelius, C.
Morse, C.
Noji, S.
Redpath, T.
Sakai, H.
Sasano, M.
Sullivan, C.
Weisshaar, D.
contents The isovector response in $^{12}$B was investigated via the $^{12}$C($^{10}\mathrm{Be}$,$^{10}\mathrm{B}$+$γ$)$^{12}$B$^\ast$ reaction at $100 A \, \mathrm{MeV}$. By utilizing the $γ$-decay properties of the 1.74 MeV $0^{+}$ and 0.718 MeV $1^{+}$ states in $^{10}\mathrm{B}$, the separate extraction of the non-spin-transfer ($ΔS=0$) and spin-transfer ($ΔS=1$) isovector responses up to an excitation energy of 50 MeV in $^{12}$B in a single measurement is demonstrated. The experimental setup employed the S800 spectrometer to detect and analyze the $^{10}\mathrm{B}$ ejectiles and the Gamma-Ray Energy Tracking In-beam Nuclear Array (GRETINA) for obtaining the Doppler-reconstructed spectrum for $γ$-rays emitted in-flight by $^{10}\mathrm{B}$. A $^{12}$C foil was placed at the pivot point of the spectrograph. The $^{12}$B reaction product was not detected. Contributions from transitions associated with the transfer of different units of angular momentum in the non-spin- and spin-transfer responses were analyzed using a multipole decomposition analysis. The extracted non-spin-dipole ($ΔS=0$, $ΔL=1$) and spin-dipole ($ΔS=1$, $ΔL=1$) responses were found to be consistent with available data from other charge-exchange probes, validating the non-spin- and spin-transfer filters used. While statistical uncertainties and experimental resolutions were relatively large due to the modest intensity of the $^{10}\mathrm{Be}$ secondary beam, the results show that, with the much higher intensities that will be available at new rare-isotope beam facilities, the ($^{10}\mathrm{Be}$,$^{10}\mathrm{B}$+$γ$) reaction and its $ΔT_{z}=-1$ partner, the ($^{10}$C,$^{10}\mathrm{B}$+$γ$) reaction, are powerful tools for elucidating the isovector non-spin- and spin-transfer responses in nuclei.
format Preprint
id arxiv_https___arxiv_org_abs_2505_06772
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Extraction of the non-spin- and spin-transfer isovector responses via the $^{12}\mathrm{C}(^{10}\mathrm{Be},{}^{10}\mathrm{B}+γ)^{12}\mathrm{B}$ reaction
Ali, Sk M.
Maher, C.
Zegers, R. G. T.
Scott, M.
Bazin, D.
Bowry, M.
Brown, B. A.
Campbell, C. M.
Gade, A.
Gales, S.
Garg, U.
Harakeh, M. N.
Kwan, E.
Langer, C.
Loelius, C.
Morse, C.
Noji, S.
Redpath, T.
Sakai, H.
Sasano, M.
Sullivan, C.
Weisshaar, D.
Nuclear Experiment
The isovector response in $^{12}$B was investigated via the $^{12}$C($^{10}\mathrm{Be}$,$^{10}\mathrm{B}$+$γ$)$^{12}$B$^\ast$ reaction at $100 A \, \mathrm{MeV}$. By utilizing the $γ$-decay properties of the 1.74 MeV $0^{+}$ and 0.718 MeV $1^{+}$ states in $^{10}\mathrm{B}$, the separate extraction of the non-spin-transfer ($ΔS=0$) and spin-transfer ($ΔS=1$) isovector responses up to an excitation energy of 50 MeV in $^{12}$B in a single measurement is demonstrated. The experimental setup employed the S800 spectrometer to detect and analyze the $^{10}\mathrm{B}$ ejectiles and the Gamma-Ray Energy Tracking In-beam Nuclear Array (GRETINA) for obtaining the Doppler-reconstructed spectrum for $γ$-rays emitted in-flight by $^{10}\mathrm{B}$. A $^{12}$C foil was placed at the pivot point of the spectrograph. The $^{12}$B reaction product was not detected. Contributions from transitions associated with the transfer of different units of angular momentum in the non-spin- and spin-transfer responses were analyzed using a multipole decomposition analysis. The extracted non-spin-dipole ($ΔS=0$, $ΔL=1$) and spin-dipole ($ΔS=1$, $ΔL=1$) responses were found to be consistent with available data from other charge-exchange probes, validating the non-spin- and spin-transfer filters used. While statistical uncertainties and experimental resolutions were relatively large due to the modest intensity of the $^{10}\mathrm{Be}$ secondary beam, the results show that, with the much higher intensities that will be available at new rare-isotope beam facilities, the ($^{10}\mathrm{Be}$,$^{10}\mathrm{B}$+$γ$) reaction and its $ΔT_{z}=-1$ partner, the ($^{10}$C,$^{10}\mathrm{B}$+$γ$) reaction, are powerful tools for elucidating the isovector non-spin- and spin-transfer responses in nuclei.
title Extraction of the non-spin- and spin-transfer isovector responses via the $^{12}\mathrm{C}(^{10}\mathrm{Be},{}^{10}\mathrm{B}+γ)^{12}\mathrm{B}$ reaction
topic Nuclear Experiment
url https://arxiv.org/abs/2505.06772